Co-reporter:Xiang-Mei Shi, Jian-Chen Li, Xing-You Lang, and Qing Jiang
The Journal of Physical Chemistry C March 23, 2017 Volume 121(Issue 11) pp:5974-5974
Publication Date(Web):March 6, 2017
DOI:10.1021/acs.jpcc.7b00481
Although α-V2O5 as an attractive electrode material for electrochemical energy storage devices exhibits a high theoretical capacity, its atomic structure with the confined size of channels for Na-ion transport and low electronic conductivity lead to the poor rate performance. Here we demonstrate that hydrogen incorporation in α-V2O5 is an effective way to improve the kinetics of ionic and electronic transports by using the density functional theory. Among various structures of hydrogen-incorporated α-V2O5, H2V2O5 presents enlarged diffusion channels along the [010] and [001] directions where the diffusion energy barriers decrease to 0.844 eV (−34.93%) and 1.737 eV (−41.81%), respectively. Improved electronic conductivity is also achieved for H2V2O5 due to the insulator–metal transition attributed by the high concentration of hydrogen atoms. As H2V2O5 has smaller volume expansion occurring during the Na-intercalation process, H2V2O5 at the comparable specific capacity exhibits higher rate capability and cyclability than α-V2O5.
Co-reporter:L. F. Duan;Y. Q. Wang;L. J. Zhao;Q. Jiang
The Journal of Physical Chemistry C June 24, 2010 Volume 114(Issue 24) pp:10691-10696
Publication Date(Web):Publication Date (Web): June 1, 2010
DOI:10.1021/jp9112377
Marked morphological changes in Co microcrystals are achieved by varying the reaction conditions, such as dosages of precursors (D), reaction temperatures (T), and types of alkali during the solvothermal treatment. Discussion is focused on the fundamental understanding and experimental designs in the control of shape of cobalt particles in solvothermal systems. UV−vis spectra show that the adsorption peak for the Co microcrystals ranges from 216 to 222 nm, which corresponds to the morphologies of disk, truncated prism, chain, hierarchical structure, and sphere, respectively. The final morphologies are complex results of the time-dependent oriented attachment and growth processes. By combining experimental results gained from XRD and SEM characterization, the formation mechanisms of Co microcrystals in solvothermal systems are conjectured.
Co-reporter:Z. W. Chen;Q. Jiang;Z. Wen
The Journal of Physical Chemistry C February 16, 2017 Volume 121(Issue 6) pp:3463-3468
Publication Date(Web):January 26, 2017
DOI:10.1021/acs.jpcc.6b12434
Clusters with precise numbers of atoms can exhibit unique and unexpected properties due to their size-dependent active sites. Besides, to obtain the superior stability and catalytic activity, an appropriate substrate can prevent the metal clusters aggregating as well as change the geometric and electronic structures of metal clusters. In this study, the catalytic oxidation of CO on the Ag38 cluster supported by graphdiyne (Ag38–GDY) is investigated by density functional theory (DFT) and molecular dynamics (MD) simulations, which provide an intensive understanding of its catalytic properties. Moreover, the process of CO oxidation on the Ag38–GDY system has a high activity with low energy barrier (0.26 eV), which originates from the intrinsic activity of Ag38 cluster and the vital role of GDY.
Co-reporter:Gao-Feng Han;Lin Gu;Xing-You Lang;Bei-Bei Xiao;Zhen-Zhong Yang;Zi Wen
ACS Applied Materials & Interfaces December 7, 2016 Volume 8(Issue 48) pp:32910-32917
Publication Date(Web):November 11, 2016
DOI:10.1021/acsami.6b12553
Author: Bimetallic platinum–nickel (Pt–Ni) alloys as oxygen reduction reaction (ORR) electrocatalysts show genuine potential to boost widespread use of low-temperature fuel cells in vehicles by virtue of their high catalytic activity. However, their practical implementation encounters primary challenges in structural and catalytic durability caused by the low formation heat of Pt–Ni alloys. Here, we report nanoporous (NP) (Pt1–xNix)3Al intermetallic nanoparticles as oxygen electroreduction catalyst NP (Pt1–xNix)3Al, which circumvents this problem by making use of the extraordinarily negative formation heats of Pt–Al and Ni–Al bonds. The NP (Pt1–xNix)3Al nanocatalyst, which is mass-produced by alloying/dealloying and mechanical crushing technologies, exhibits specific activity of 3.6 mA cm–2Pt and mass activity of 2.4 A mg–1Pt at 0.90 V as a result of both ligand and compressive strain effects, while strong Ni–Al and Pt–Al bonds ensure their exceptional durability by alleviating evolution of Pt, Ni, and Al components and dissolutions of Ni and Al atoms.Keywords: dealloying; electrocatalysis; fuel cells; intermetallic compounds; nanoporous metals; oxygen reduction reaction; platinum alloys;
Co-reporter:Ying-Qi Li;Jian-Chen Li;Xing-You Lang;Zi Wen;Wei-Tao Zheng
Advanced Functional Materials 2017 Volume 27(Issue 29) pp:
Publication Date(Web):2017/08/01
DOI:10.1002/adfm.201700447
Transition-metal oxides show genuine potential in replacing state-of-the-art carbonaceous anode materials in lithium- or sodium-ion batteries because of their much higher theoretical capacity. However, they usually undergo massive volume change, which leads to numerous problems in both material and electrode levels, such as material pulverization, instable solid-electrolyte interphase, and electrode failure. Here, it is demonstrated that lithium-ion breathable hybrid electrodes with 3D architecture tackle all these problems, using a typical conversion-type transition-metal oxide, Fe3O4, of which nanoparticles are anchored onto 3D current collectors of Ni nanotube arrays (NTAs) and encapsulated by δ-MnO2 layers (Ni/Fe3O4@MnO2). The δ-MnO2 layers reversibly switch lithium insertion/extraction of internal Fe3O4 nanoparticles and protect them against pulverizing and detaching from NTA current collectors, securing exceptional integrity retention and efficient ion/electron transport. The Ni/Fe3O4@MnO2 electrodes exhibit superior cyclability and high-capacity lithium storage (retaining ≈1450 mAh g−1, ≈96% of initial value at 1 C rate after 1000 cycles).
Co-reporter:N. Gao;G. Y. Lu;Z. Wen;Q. Jiang
Journal of Materials Chemistry C 2017 vol. 5(Issue 3) pp:627-633
Publication Date(Web):2017/01/19
DOI:10.1039/C6TC04943E
The potential of silicene-based integrated electronics originates from its extremely high carrier mobility, whereas the lack of a band gap impedes its application. Thus, opening a sizeable band gap without degrading its carrier mobility is a significant challenge for application in logic circuits. In this study, a sizable band gap is created in silicene by the dual effect of organic molecule adsorption and a substrate. As an electron donor molecule, tetrathiafulvalene (TTF) is found to non-covalently functionalize the silicene sheet. As a result, silicene with adsorbed TTF exhibits an open band gap. When silicane (hydrogenated silicene) substrate is applied, the band gap further widens. Moreover, the high carrier mobility is largely retained. These results provide effective and reversible routes for engineering the band gap of silicene.
Co-reporter:B. B. Xiao;H. Y. Liu;X. B. Jiang;Z. D. Yu;Q. Jiang
RSC Advances (2011-Present) 2017 vol. 7(Issue 86) pp:54332-54340
Publication Date(Web):2017/11/27
DOI:10.1039/C7RA09974F
To achieve renewable energy technologies, low-cost electrocatalysts for the oxygen reduction reaction (ORR) and the oxygen evolution reaction (OER) are required to replace Pt and IrO2/RuO2 catalysts. Based on density functional theory, the catalytic activity of TM3(HHTP)2 (2,3,6,7,10,11-hexahydroxytriphenylene) monolayer and its variations (TMX4, where TM = Fe, Co, Ni, X = O, S, Se) for bifunctional ORR/OER have been investigated. The adsorption ability is dominated by the metal center, in the order of Fe > Co > Ni while the ligand shows the minor contribution. Due to the presence of linear relations between the intermediates, the activity of TMX4 for the ORR/OER follows a dual volcano curve as a function of the OH adsorption strength. Considering the overpotential, CoO4 and CoS4 possess superior bifunctional activity, implying their promise as candidates for the oxygen electrode reaction. This systematical work may open new avenues for the development of high-performance non-PGM catalysts for practical applications of ORR and OER.
Co-reporter:Yong-Fu Zhu;Ning Zhao;Bo Jin;Ming Zhao
Physical Chemistry Chemical Physics 2017 vol. 19(Issue 13) pp:9253-9260
Publication Date(Web):2017/03/29
DOI:10.1039/C6CP08061H
Nanoscale core/shell structures are of interest in catalysis due to their superior catalytic properties. Here we investigated the thermal stability of the coherent core–shell structures in a thermodynamic way by considering the impact from the core with the bulk melting point Tm(∞) lower or higher than the shell. When a low-Tm(∞) core is adopted, core–shell melting induced by the melting depression of the core does not occur upon heating because of the superheating, although the melting depression of the core can be triggered ultimately by the preferential melting of the high-Tm(∞) shell for small cores. The superheating of the core is contributed by the negative solid–solid interface energy, while the depression is originated from the positive solid–liquid interface energy. Owing to the presence of the negative interface energy, moreover, the low-Tm(∞)-core structure possesses a low difference in thermal expansion between the core and the shell, high activation energy of outward atomic diffusion from the core to shell, and low heat capacity. This result is beneficial for the core–shell structure design for its application in catalysis.
Co-reporter:Cang Lang Yao;Jian Chen Li;Wang Gao
Physical Chemistry Chemical Physics 2017 vol. 19(Issue 23) pp:15067-15072
Publication Date(Web):2017/06/14
DOI:10.1039/C7CP01881A
The urgent need for artificially fixing CO2 calls for catalysts of high efficiency. The transition metal functionalized porphyrin (TMP) is one of the most important types of organic catalysts for CO2 reduction. However, the catalytic mechanisms of TMP in CO2 reduction still remain controversial. Starting from the previously neglected catalyst self-protonation model, we uncover a new CO2 reduction mechanism on cobalt-porphine, which involves an indirect proton transfer step occurring at the beginning of the reduction cycle. Based on this protonation mechanism, we demonstrate the different correlations between producing rate and pH for the formation of CO and methane, in good agreement with available experimental observations. Our results reveal how pH and potential affect the CO2 reduction process, providing important clues and insights for further optimization of TMP catalysts.
Co-reporter:N. Gao;Y. F. Zhu;Q. Jiang
Journal of Materials Chemistry C 2017 vol. 5(Issue 29) pp:7283-7290
Publication Date(Web):2017/07/27
DOI:10.1039/C7TC01972F
Arsenene-based device applications such as transistors and photodetectors benefit from precise control over the carrier type and concentration as well as a combination of both high-quality p-doped and n-doped components to form p–n junctions. Here, it is demonstrated using first-principles calculations that selective organic molecular adsorption allows us to effectively control the carrier type in arsenene. Moreover, upon applying an in-plane tensile strain, the carrier concentration effectively increases. Furthermore, the BN substrate can increase the structural stability without any impact on the doping character of the arsenene sheet. This opens the possibility of creating arsenene p–n junctions.
Co-reporter:Chun Cheng Yang;Chang Chun Wang;Miao Miao Li
Journal of Materials Chemistry A 2017 vol. 5(Issue 3) pp:1145-1152
Publication Date(Web):2017/01/17
DOI:10.1039/C6TA09736G
Nickel metal hydride (Ni-MH) batteries have demonstrated key technology advantages for applications in new-energy vehicles, while the main challenge derives from the insufficient cycle lives (about 500 cycles) of their negative electrode materials—hydrogen storage alloys. As a result, progress in their development has been very limited over the past decades. Here we propose a theoretical framework to design a series of long-life and low-cost hydrogen storage alloys, by considering the electronegativities of the elements to enhance the alloys' corrosion resistance. Two novel candidate alloys, La0.6Ce0.3Y0.1Ni3.7Co0.75Mn0.3Al0.35 and La0.55Ce0.3Y0.15Ni3.7Co0.75Mn0.3Al0.35, show ultra-long cycle lives of 1325 and 1407 cycles, respectively, which are almost triple that of the commercial alloy (MmNi3.55Co0.75Mn0.4Al0.3) that is used in Ni-MH batteries. The usage costs of Ni-MH batteries based on these two alloys are only 1/4 of that of the lithium-ion battery, showing better market prospects for large-scale applications.
Co-reporter:Y.F. Zhu, Q. Jiang
Coordination Chemistry Reviews 2016 Volume 326() pp:1-33
Publication Date(Web):1 November 2016
DOI:10.1016/j.ccr.2016.06.012
•The edge or interface effect on the bandgap openings is reviewed.•The openings can be induced by change in the atomic cohesive energy.•The openings in graphene nanostructures are influenced by a series of parameters.As a two-dimensional (2D) material with hexagonal structure, graphene shows high electron mobility, high thermal conductivity, and compatibility to industry-standard lithographic processing for nano and microelectronics applications. Different ways have been adopted to theoretically explore the mechanism of bandgap openings (BOs) in graphene nanostructures with regard to the edge or interface effect, involving the quantum confinement model, the bond-order-length-strength model, the lattice model, and the bandgap thermodynamic approach. By eliminating limitations in other theories, the bandgap thermodynamic approach, free of adjustable parameters, can be applied to systematically elucidate the BO mechanisms in graphene nanostructures. Supported by the energy band theory, this approach correlates the BOs to changes in the atomic cohesive energy of C atoms in graphene nanostructures at the edge or interface, which is associated with coordination imperfections or distinct chemical bonding. Hence, the openings can be modulated by a series of parameters, such as size, dimension, edge geometry, edge saturation, interfacial interaction, and electronic configuration of C atoms. Using the bandgap thermodynamic approach, strikingly, new routes are suggested to engineer and control the bandgaps of graphene and graphene-based nanostructures, helping the design of graphene-based devices for its application in electronics.
Co-reporter:Ying-Qi Li;Xiang-Mei Shi;Xing-You Lang;Zi Wen;Jian-Chen Li
Advanced Functional Materials 2016 Volume 26( Issue 11) pp:1830-1839
Publication Date(Web):
DOI:10.1002/adfm.201504886
Transition-metal oxides as faradaic charge-storage intermediates sandwiched between conductor and electrolyte are key components to store/deliver high-density energy in microsupercapacitors for many applications in miniaturized portable electronics and microelectromechanical systems. While the conductor facilitating their electron transports, they generally suffer from a switch of rate-determining step to their sluggish redox reactions in pseudocapacitive energy storage, during which poor cation accessibility and diffusion leads to high internal resistances and lowers volumetric capacitance and rate performance. Here it is shown that the faradaic processes in a model system of MnO2 can be radically boosted by tuning crystallographic structures from cryptomelane (α-MnO2) to birnessite (δ-MnO2). As a result of greatly enhanced Na+ accessibility and diffusion, 3D layered crystalline δ-MnO2 microelectrodes exhibit volumetric capacitance as high as ≈922 F cm−3 (≈1.5-fold higher than α-MnO2, ≈617 F cm−3) and excellent rate performance. This enlists δ-MnO2 microsupercapacitor to deliver ultrahigh stack electrical powers (up to ≈295 W cm−3) while maintaining volumetric energy density much higher than that of thin-film lithium battery.
Co-reporter:Xing-You Lang;Bo-Tian Liu;Xiang-Mei Shi;Ying-Qi Li;Zi Wen
Advanced Science 2016 Volume 3( Issue 5) pp:
Publication Date(Web):
DOI:10.1002/advs.201500319
Nanostructured transition-metal oxides can store high-density energy in fast surface redox reactions, but their poor conductivity causes remarkable reductions in the energy storage of most pseudocapacitors at high power delivery (fast charge/discharge rates). Here it is shown that electron-correlated oxide hybrid electrodes made of nanocrystalline vanadium sesquioxide and manganese dioxide with 3D and bicontinuous nanoporous architecture (NP V2O3/MnO2) have enhanced conductivity because of metallization of electron-correlated V2O3 skeleton via insulator-to-metal transition. The conductive V2O3 skeleton at ambient temperature enables fast electron and ion transports in the entire electrode and facilitates charge transfer at abundant V2O3/MnO2 interface. These merits significantly improve the pseudocapacitive behavior and rate capability of the constituent MnO2. Symmetric pseudocapacitors assembled with binder-free NP V2O3/MnO2 electrodes deliver ultrahigh electrical powers (up to ≈422 W cm23) while maintaining the high volumetric energy of thin-film lithium battery with excellent stability.
Co-reporter:B. B. Xiao, X. B. Jiang and Q. Jiang
Physical Chemistry Chemical Physics 2016 vol. 18(Issue 21) pp:14234-14243
Publication Date(Web):20 Apr 2016
DOI:10.1039/C6CP01066K
Developing efficient catalysts for the oxygen reduction reaction (ORR) to reduce cathode Pt loading without sacrificing the performance has been under intensive research. Herein, by using density functional theory calculations, the activity and stability of a Pt monolayer supported on Pd3Al(111) as the ORR catalyst have been systematically studied. The simulations demonstrate that due to alloying, the ORR intermediates bind weakly on Pt/Pd3Al(111) with optimal adsorption energy of O and OH. By considering the elemental ORR steps, the ORR mechanism is predicted to be an OOH dissociation mechanism. The rate determining step is OOH dissociation with a reaction barrier of 0.37 eV, lower than the corresponding value on Pt/Pt3Al(111) and Pt(111), indicating the superior activity of Pt/Pd3Al(111). Even considering the unfeasible H adsorption under high potential, the ORR mechanism on Pt/Pd3Al(111) would proceed via O2 hydration, OOH hydration, H2O formation, and H2O desorption, indicating a good ORR electrocatalyst. Furthermore, stability was evaluated by calculating the alloy formation energy and the electrochemical potential shift of surface Pt dissolution. The exceptionally negative alloy formation energy of Pd3Al and the positive dissolution potential shift of the surface Pt atoms show the enhanced durability of Pt/Pd3Al(111). The improved activity, in combination with its enhanced stability, makes the novel ternary alloy electrocatalyst very promising for development of new cathode catalysts for fuel cells.
Co-reporter:Jun-Min Yan;Zhi-Li Wang;Lin Gu;Si-Jia Li;Hong-Li Wang;Wei-Tao Zheng
Advanced Energy Materials 2015 Volume 5( Issue 10) pp:
Publication Date(Web):
DOI:10.1002/aenm.201500107
The safe and efficient storage and release of hydrogen are widely recognized as the main challenges for the establishment of a fuel-cell-based hydrogen economy. Formic acid (FA) has great potential as a safe and convenient source of hydrogen for fuel cells. Despite tremendous efforts, the development of heterogeneous catalysts with high activity and relatively low cost remains a major challenge. The synthesis of AuPd–MnOx nanocomposite immobilized on ZIF-8–reduced-graphene-oxide (ZIF-8–rGO) bi-support by a wet-chemical method is reported here. Interestingly, the resultant AuPd–MnOx/ZIF-8–rGO shows excellent catalytic activity for the generation of hydrogen from FA, and the initial turnover frequency (TOF) reaches a highest value of 382.1 mol H2 mol catalyst−1 h−1 without any additive at 298 K. This good performance of AuPd–MnOx/ZIF-8–rGO results from the modified electronic structure of Pd in the AuPd–MnOx/ZIF-8–rGO composite, the small size and high dispersion of the AuPd–MnOx nanocomposite, and also the strong metal-support interaction between the AuPd–MnOx and ZIF-8–rGO bi-support.
Co-reporter:Xing-You Lang;Gao-Feng Han;Bei-Bei Xiao;Lin Gu;Zhen-Zhong Yang;Zi Wen;Yong-Fu Zhu;Ming Zhao;Jian-Chen Li
Advanced Functional Materials 2015 Volume 25( Issue 2) pp:230-237
Publication Date(Web):
DOI:10.1002/adfm.201401868
Alloying techniques show genuine potential to develop more effective catalysts than Pt for oxygen reduction reaction (ORR), which is the key challenge in many important electrochemical energy conversion and storage devices, such as fuel cells and metal-air batteries. Tremendous efforts have been made to improve ORR activity by designing bimetallic nanocatalysts, which have been limited to only alloys of platinum and transition metals (TMs). The Pt-TM alloys suffer from critical durability in acid-media fuel cells. Here a new class of mesostructured Pt–Al catalysts is reported, consisting of atomic-layer-thick Pt skin and Pt3Al or Pt5Al intermetallic compound skeletons for the enhanced ORR performance. As a result of strong Pt–Al bonds that inhibit the evolution of Pt skin and produce ligand and compressive strain effects, the Pt3Al and Pt5Al mesoporous catalysts are exceptionally durable and ≈6.3- and ≈5.0-fold more active than the state-of-the-art Pt/C catalyst at 0.90 V, respectively. The high performance makes them promising candidates as cathode nanocatalysts in next-generation fuel cells.
Co-reporter:Chao Hou, Xing-You Lang, Zi Wen, Yong-Fu Zhu, Ming Zhao, Jian-Chen Li, Wei-Tao Zheng, Jian-She Lian and Qing Jiang
Journal of Materials Chemistry A 2015 vol. 3(Issue 46) pp:23412-23419
Publication Date(Web):14 Oct 2015
DOI:10.1039/C5TA05335H
Transition-metal hydroxides (TMHOs) or oxides (TMOs) with layered crystalline structures are attractive electrode materials for high-density charge storage in electrochemical supercapacitors. However, their randomly stacked nanostructures on conductive reinforcements, typically carbon materials, exhibit only modest enhancement of rate capability because of poor electron and ion transports that are limited by highly anisotropic conductivity, excessive grain boundaries and weak TMHO or TMO/C interfaces. Here we report a hybrid electrode design to tackle all three of these problems in layered Ni(OH)2 for high-performance asymmetric supercapacitors, wherein the single-crystalline Ni(OH)2 nanosheets are vertically aligned on a three-dimensional bicontinuous nanoporous gold skeleton with epitaxial Au/Ni(OH)2 interfaces (NP Au/VA Ni(OH)2). As a result of the unique nanoarchitecture, the pseudocapacitive behavior of Ni(OH)2 is dramatically enhanced for ensuring a volumetric capacitance as high as ∼2911 F cm−3 (∼2416 F g−1 for the constituent Ni(OH)2) in the NP Au/VA Ni(OH)2 electrode with excellent rate capability. Asymmetric supercapacitors assembled with this NP Au/VA Ni(OH)2 electrode and activated carbon have a high gravimetric energy of 31.4 W h kg−1 delivered at an exceptionally high power density of 100 kW kg−1 with excellent cycling stability.
Co-reporter:D. Liu, Y. F. Zhu and Q. Jiang
RSC Advances 2015 vol. 5(Issue 2) pp:1587-1597
Publication Date(Web):19 Nov 2014
DOI:10.1039/C4RA10881G
Although Au–Cu alloy nanoparticles on inert substrates show high activity for catalyzing CO oxidation, the corresponding catalytic mechanism is not clear. To clarify the mechanism of this alloy catalysis method, CO oxidation reactions on Au–Cu alloy surfaces with different surface oxidation states are studied via density functional theory simulations. The simulation results indicate that on AuCu(111) and Cu2O/Au3Cu(111), CO and O2 cannot move together for reactions since they are adsorbed on separate Cu sites. On Cu2O–Au/Au3Cu(111), O2 prefers to be located at the Cu hollow sites near Cu2O–Au interfaces. When CO diffuses to its neighboring Au sites, they can easily combine to generate CO2, for which the reaction barriers are no more than 0.42 eV. The Au and Cu synergetic effect for catalyzing CO oxidation can be realized on Cu2O–Au interfaces at Au–Cu nanoparticle surfaces.
Co-reporter:Hongmin Su, Hongming He, Yuyang Tian, Nian Zhao, Fuxing Sun, Xiaoming Zhang, Qing Jiang, Guangshan Zhu
Inorganic Chemistry Communications 2015 Volume 55() pp:92-95
Publication Date(Web):May 2015
DOI:10.1016/j.inoche.2015.03.027
•Two pharmaceutical cocrystals have been prepared.•JUC-C14 displays a 1D chain.•The di-keto structure of curcumin in JUC-C15 is rarely reported.Two pharmaceutical cocrystals, named Jilin University China–Cocrystal-14 (JUC-C14) and Jilin University China–Cocrystal-15 (JUC-C15), which were composed of curcumin and 4, 4′-bipyridine-N, N′-dioxide, were successfully prepared by crystal engineering strategy. The crystal structures of the two cocrystals were solved and refined by single crystal X-ray diffraction. It is indicated that the crystal structures are assembled via intermolecular interactions including hydrogen bonds and π⋯π stacking. Additionally, in the structure of JUC-C15 curcumin existed in a di-keto form which is rare in other reported curcumin polymorphs. Power X-ray diffraction, Fourier-transform infrared spectra, thermogravimetric analyses and differential scanning calorimetry were executed as well to confirm the formation of the cocrystals.Two pharmaceutical cocrystals, JUC-C14 and JUC-C15, which were composed of curcumin and 4, 4′-bipyridine-N, N′-dioxide, were successfully prepared under the similarly synthetic conditions. It is indicated that JUC-C14 exhibits 1D chain structure, while JUC-C15 is a 2D net structure linked via hydrogen bonds and π⋯π packing interactions. Additionally, in the structure of JUC-C15 curcumin existed in a di-keto form which is rare in other reported curcumin polymorphs.
Co-reporter:Hong-Ying Fu, Xing-You Lang, Chao Hou, Zi Wen, Yong-Fu Zhu, Ming Zhao, Jian-Chen Li, Wei-Tao Zheng, Yong-Bing Liu and Qing Jiang
Journal of Materials Chemistry A 2014 vol. 2(Issue 35) pp:7216-7222
Publication Date(Web):08 Jul 2014
DOI:10.1039/C4TC00603H
There is a strong interest in plasmonic nanostructures that uniformly enhance Raman signals of chemical and biological molecules using surface-enhanced Raman spectroscopy (SERS) for trace detection. Although the resonant excitation of localized surface plasmons of single or assembled metallic nanoparticles can generate large electromagnetic fields, their SERS effects suffer from poor reproducibility and uniformity, limiting their highly reliable and stable applications. Here, we report self-supported large-scale nanoporous hybrid films with high density and uniform hot spots, produced by the implantation of SnO nanoparticles into nanoporous Au/Ag bimetallic films (NP Au/SnO/Ag) for the trace detections of both resonant and non-resonant molecules. The NP Au/SnO/Ag films exhibit extraordinary SERS enhancements, which increase with the increasing density of Au/SnO/Ag sandwich protrusions, as a result of the formation of abundant and uniform hot spots. The nanogaps in their wrinkled films further improve the capability to detect molecules at single molecular levels, making the hybrid films promising SERS-active substrates with superior reproducibility and reliability for applications in life science and environment protection.
Co-reporter:Chao Hou, Xiang-Mei Shi, Chen-Xu Zhao, Xing-You Lang, Lin-Lin Zhao, Zi Wen, Yong-Fu Zhu, Ming Zhao, Jian-Chen Li and Qing Jiang
Journal of Materials Chemistry A 2014 vol. 2(Issue 37) pp:15519-15526
Publication Date(Web):25 Jul 2014
DOI:10.1039/C4TA02604G
Nanostructured SnO2 is an attractive anode material for high-energy-density lithium-ion batteries because of the fourfold higher theoretical charge capacity than commercially used graphite. However, the poor capacity retention at high rates and long-term cycling have intrinsically limited applications of nanostructured SnO2 anodes due to large polarization and ∼300% volume change upon lithium insertion/extraction. Here we report the design of a SnO2-based anode, which is constructed by embedding SnO2 nanoparticles into a seamlessly integrated 3D nanoporous/solid copper current collector (S/NP Cu/SnO2), with an aim at tackling both problems for the high-performance reversible lithium storage. As a result of the unique hybrid architecture that enhances electron transfer and rapid access of the lithium ion into the particle bulk, the S/NP Cu/SnO2 anode can store charge with a capacity density as high as ∼3695 mA h cm−3 and an exceptional rate capability. Even when the discharge rate is increased by a factor of 160 (12 A g−1), it still retains ∼1178 mA h cm−3, one order of magnitude higher than that of a traditional SnO2-based electrode (∼111.6 mA h cm−3), which is assembled by mixing SnO2 nanoparticles with conductive carbon black and a polymeric binder and coating on flat Cu foil. In addition, not only do the rigid Cu skeleton and the stable Cu/SnO2 interface improve the microstructural stability, but also the pore channels accommodate the large SnO2 volume changes, enlisting the S/NP Cu/SnO2 anode to exhibit high specific capacity over 1000 cycles at a high rate.
Co-reporter:Gao-Feng Han, Bei-Bei Xiao, Xing-You Lang, Zi Wen, Yong-Fu Zhu, Ming Zhao, Jian-Chen Li, and Qing Jiang
ACS Applied Materials & Interfaces 2014 Volume 6(Issue 19) pp:16966
Publication Date(Web):September 12, 2014
DOI:10.1021/am504541a
Au nanostructures as catalysts toward electrooxidation of small molecules generally suffer from ultralow surface adsorption capability and stability. Here, we report Ni(OH)2 layer decorated nanoporous (NP) AuNi alloys with a three-dimensional and bimodal porous architecture, which are facilely fabricated by a combination of chemical dealloying and in situ surface segregation, for the enhanced electrocatalytic performance in biosensors. As a result of the self-grown Ni(OH)2 on the AuNi alloys with a coherent interface, which not only enhances adsorption energy of Au and electron transfer of AuNi/Ni(OH)2 but also prohibits the surface diffusion of Au atoms, the NP composites are enlisted to exhibit significant enhancement in both electrocatalytic activity and stability toward glucose electrooxidation. The highly reliable glucose biosensing with exceptional reproducibility and selectivity as well as quick response makes it a promising candidate as electrode materials for the application in nonenzymatic glucose biosensors.Keywords: biosensor; electrooxidation; nanoporous gold; nickel hydrate
Co-reporter:T.H. Wang, Y.F. Zhu, Q. Jiang
Carbon 2014 Volume 77() pp:431-441
Publication Date(Web):October 2014
DOI:10.1016/j.carbon.2014.05.048
In this work, based on experimental possibilities, our first-principles calculations predict a sizeable bandgap opening in bilayer graphene (BLG) by n-doping from decamethylcobaltocene (DMC) and p-doping from functionalized amorphous SiO2 (a-SiO2) gate dielectric. With DMC monolayer on BLG and the maximum O2− on the surface of a-SiO2 gate dielectric, the dual-doped BLG presents a bandgap of 390–394 meV and a Dirac level shift of −59 to −52 meV. The former is very close to the technical requirement of 400 meV, while the latter properly lies in the accessible range of the gate voltage of 300 meV. The high carrier mobility largely remains with the on/off current ratio satisfying the technical requirement of 104−107. The external electric field is not needed in this technique, which avoids a complex fabrication step for preparing a dual-gate structure and a substantial reduction in carrier mobility and on/off current ratio induced by adding an extra gate.
Co-reporter:Q. Q. Dai, Y. F. Zhu and Q. Jiang
Physical Chemistry Chemical Physics 2014 vol. 16(Issue 22) pp:10607-10613
Publication Date(Web):31 Mar 2014
DOI:10.1039/C4CP00868E
Grain boundaries (GBs) that inevitably appear in CVD-grown graphene affect the electronic properties of graphene-based nanomaterials. In this paper, we introduce 558 GB (composed of a pair of pentagons and one octagon alternately) into armchair graphene nanoribbons (AGNRs) and divide them into three groups in light of the end configurations of 558 GB at the ribbon edges. By using first-principles calculations, the variations of electronic and magnetic properties with two adjustable parameters W (ribbon widths) and NZ (the distances between 558 GBs) are systematically investigated for each group. The results show that different electronic and magnetic behaviors versus W and NZ are presented for varying end configurations of 558 GB, including nonmagnetic metals, ferromagnetic metals and nonmagnetic semiconductors. By introducing 558 GB into AGNRs, the impurity states that are completely contributed by 558 GB appear around the Fermi level. Furthermore, a ferromagnetic ordering on the two zigzag chains of 558 GB occurs for the ferromagnetic metals due to the spin splitting energy bands near the Fermi level. These unique electronic and magnetic properties of AGNRs with 558 GB would find their potential applications in electronic and spintronic devices.
Co-reporter:N. Gao, J. C. Li and Q. Jiang
Physical Chemistry Chemical Physics 2014 vol. 16(Issue 23) pp:11673-11678
Publication Date(Web):24 Mar 2014
DOI:10.1039/C4CP00089G
The geometric and electronic properties of silicene paired with a MoS2 substrate are studied systematically by using density functional theory with van der Waals corrections. It is found that the nearly linear band dispersions can be preserved in the heterobilayers due to the weak interface interactions. Meanwhile, the band gap is opened because of the sublattice symmetry broken by the intrinsic interface dipole. Moreover, the band gap values could be effectively modulated under an external electric field. Therefore, a way is paved for silicene–MoS2 heterobilayers to be candidate materials for logic circuits and photonic devices.
Co-reporter:Y. F. Zhu, Q. Q. Dai, W. T. Zheng and Q. Jiang
Physical Chemistry Chemical Physics 2014 vol. 16(Issue 12) pp:5600-5604
Publication Date(Web):2014/02/11
DOI:10.1039/C3CP55222E
Based on the size-dependent cohesive energy formula for two-dimensional materials, we investigate the gap openings in graphene layers regarding distinct interfacial interaction from substrates. Depending on the interfacial physicochemical nature, the gap is opened weakly induced by the van der Waals interaction but readily by the chemical bonding. Relative to the former, in essence, the distinct opening behavior for the latter comes from the substantial change in atomic cohesive energy of graphene associated with the coordination imperfection. Our predictions agree with the available experimental or computer simulation results for graphene layers on layered BN or bulk truncated SiC. The present work is of benefit for the application of graphene in electronics.
Co-reporter:B. B. Xiao, X. Y. Lang and Q. Jiang
RSC Advances 2014 vol. 4(Issue 54) pp:28400-28408
Publication Date(Web):16 Jun 2014
DOI:10.1039/C4RA03387F
Among the issues inherent to fuel cells, the high cost of the Pt electrocatalyst restricts its widespread application. Controlling nano- or subnano-material structures could improve the utilization of Pt. Here, the catalytic activity of the oxygen reduction reaction (ORR) on Pt monatomic wire that is supported on the zigzag edges of graphene nanoribbon (Pt–GNR) is studied using density functional theory. It is found that Pt–GNR is inert for ORR, due to the strong binding of OH and H2O. However, when Pt–GNR is covered by the chain of OH and H2O (cPt–GNR), it becomes catalytically active for ORR. Through the free energy diagrams on cPt–GNR, we demonstrate that the highest potential U for ORR as an exothermic process is 0.82 eV. When U is larger than 0.82 V, the rate-determined step (RDS) of ORR is located at the reduction of O2* to OOH* (* denotes adsorbed species) where the energy barrier ΔG is less than 0.41 eV. These results support cPt–GNR as a candidate for ORR.
Co-reporter:L. L. Wang, M. Zhao and Q. Jiang
RSC Advances 2014 vol. 4(Issue 80) pp:42585-42590
Publication Date(Web):04 Sep 2014
DOI:10.1039/C4RA04653F
Using density-functional theory, we show that the NiAs-type is a more favorable structure for the (W0.5Al0.5)C phase than the experimentally proposed WC-type structure when we compare the thermodynamic, dynamic and elastic properties of the two types. Furthermore, it is found that this NiAs-type (W0.5Al0.5)C phase could be synthesized under pressures of 12 GPa or higher, while the advanced mechanical properties of the (W0.5Al0.5)C phase, including the bulk modulus of B = 268 GPa, the shear modulus of G = 206 GPa, and the hardness of HV = 30 GPa, could be reproduced by the NiAs-type structure. The fantastic mechanical properties of the phase are attributed to the synergistic effect of stronger C–Al bonding and weaker C–W bonding of the NiAs-type structure.
Co-reporter:Xian Fei Chen, Yong Fu Zhu and Qing Jiang
RSC Advances 2014 vol. 4(Issue 8) pp:4146-4154
Publication Date(Web):29 Oct 2013
DOI:10.1039/C3RA44550J
Graphene-based device applications such as ultrafast transistors and photodetectors benefit from precise control over its carrier type and concentration as well as a combination of both high-quality p- and n-doped components with spatial control and seamless connection (p–n junctions/superlattices). However, this remains experimentally a challenge for an atom-scale control over the doping in graphene and the attendant formation of p–n junctions/superlattices. Here, we demonstrate that sandwiching a janus material (a functionalized graphene layer with one side by H atoms and another side by F atoms, defined as H–G–F) between MoSe2 (BN) substrate and graphene allows us to effectively control the carrier type in graphene, where the janus material acts as an electron pump, facilitating the electron tunneling between MoSe2 (BN) and graphene. Appropriate functionalization of the janus material would open the possibility of creating well ordered and atomically sharp graphene p–n junctions/superlattices in a single layer of graphene. Furthermore, upon applying an external electric field, the charge concentration in both n-type and p-type regions can be continuously tuned except for a platform area. A comprehensive and detailed picture built by density functional theory calculations sheds light on the physical mechanism of the observed doping course as well as its response to an external field. Our results not only introduce single-layer H–G–F as a new 2D Janus material with the ability of electron extraction, but also open up a new direction for local control over the properties of graphene without destroying its intrinsic structure.
Co-reporter:N. Gao, J.C. Li, Q. Jiang
Chemical Physics Letters 2014 Volume 592() pp:222-226
Publication Date(Web):30 January 2014
DOI:10.1016/j.cplett.2013.12.036
Highlights
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Several possible semiconducting substrates for silicene are investigated.
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The factor that controls the size of band gap in silicene/substrates is analyzed.
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The structures with SiH/π interaction have potential in field effect transistors.
Co-reporter:X. F. Chen, J. M. Yan, and Q. Jiang
The Journal of Physical Chemistry C 2014 Volume 118(Issue 4) pp:2122-2128
Publication Date(Web):January 10, 2014
DOI:10.1021/jp411183h
Single atom catalysts (SAC) are highly desirable to maximize atom efficiency, while fabricating them is largely dependent on choosing a suitable substrate to effectually fasten them. Here, in terms of strong metal–metal interaction, first-principle calculations have been performed to study the possibility of monolayer polymeric transition metal–phthalocyanines (TM–Pcs, M from Sc to Zn) as the substrate in an effect to obtain evenly distributed single Pt atom catalyst. We found that Ti–Pc is the most appropriate compound by virtue of high binding strength of Pt/Ti–Pc system and high diffusion energy barrier of Pt catalyst atom, which jointly prevent the formation of Pt clusters. CO oxidation on Pt/Ti–Pc presents some unexpected behaviors, where a presorbed CO (pCO) molecule could activate the catalyst and reduce the reaction barrier. Examining the electronic structure evolution in the reaction process demonstrates that the presence of a pCO promotes O2 adsorption and activation. Our results demonstrate that two-dimensional (2D) TM–Pcs provide a unique platform to fabricate regularly and separately distributed SAC with high activity.
Co-reporter:Yongfu Zhu, Ning Zhao, Jianshe Lian, and Qing Jiang
The Journal of Physical Chemistry C 2014 Volume 118(Issue 5) pp:2385-2390
Publication Date(Web):January 27, 2014
DOI:10.1021/jp412257g
Graphene quantum dots (GQDs) are promising photonic materials for light harvesting. However, only low photoelectron conversion efficiency can be generated in single-junction graphene-based solar cells when isolated GQDs with the edge bonding defects are used as semiconductors. To address this issue, a four-junction GQD-based tandem solar cell with high theoretical conversion efficiency was proposed in this paper. Instead of isolated GQDs, nanoarray GQDs embedded in hexagonal host materials, such as graphane or boron nitride, was adopted as the photoactive layer. Utilizing our universal thermodynamic approach to the gap openings in low-dimensional graphene, nanoarray armchair-interfaced GQDs embedded in graphane to achieve the maximal diameter of confined GQDs are found preferential for fabricating tandem solar cell devices. Besides these, the separation between GQDs and the thickness of GQD-based sheets were determined. This contribution is of benefit to the application of graphene for solar cell devices.
Co-reporter:Ming Wu;Dr. Jun-Min Yan;Xian-nian Tang;Dr. Ming Zhao ;Dr. Qing Jiang
ChemSusChem 2014 Volume 7( Issue 9) pp:2654-2658
Publication Date(Web):
DOI:10.1002/cssc.201402180
Abstract
Potassium-modified graphitic carbon nitride (K-g-C3N4) nanosheets are synthesized by a facile KCl-template method that holds the advantage of easy removal of residual template. A combination of XRD, X-ray photoelectron spectroscopy, and inductively coupled plasma analyses are utilized to characterize the obtained resultant K-g-C3N4 architectures, which are composed of nanosheets of variable thickness (<10 nm). Photocatalytic hydrogen evolution experiments under visible light irradiation showed that K-g-C3N4 nanosheets have high photocatalytic activities (up to about thirteen times higher than that of pure g-C3N4) as well as good stability (no reduction in activity within 16 h); both features emanate from their unique structural characteristics. These results illustrate the viability of this methodology for the facile synthesis of efficient heterogeneous photocatalysts for potential commercial applications.
Co-reporter: Yongfu Zhu; Jianshe Lian ; Qing Jiang
ChemPhysChem 2014 Volume 15( Issue 5) pp:958-965
Publication Date(Web):
DOI:10.1002/cphc.201301127
Abstract
By using a size-dependent cohesive energy formula for two-dimensional coordination materials, the bandgap openings of ideal graphene quantum dots (GQDs) and nanoribbons (GNRs) have been investigated systematically regarding dimension, edge geometry, and magnetic interaction. Results demonstrate that the bandgap openings in GQDs can be dominated by the change of atomic cohesive energy. Relative to zigzag GQDs, the openings in the armchair ones are more substantial, attributed to its edge instability. The change of cohesive energy can also lead to bandgap openings in zigzag and armchair GNRs. The contribution from the interedge magnetic interaction in zigzag GNRs is negligible, while the cohesive-energy induced openings in armchair GNRs can oscillate according to the so-called full-wavelength effect, depending on the width. The model prediction provides physicochemical insight into the bandgap openings in graphene.
Co-reporter:Zhi-Li Wang, Jun-Min Yan, Hong-Li Wang, Qing Jiang
Journal of Power Sources 2013 Volume 243() pp:431-435
Publication Date(Web):1 December 2013
DOI:10.1016/j.jpowsour.2013.05.193
•We have explored a facile but very efficient method to realize the long-time recycle application of Co nanocatalyst.•Oxidizes Co0 completely into Co2+ for the long-time and oxygen-fearless storage in air.•Reduces Co2+ back to fresh and highly active Co0 for the recycle application in air.•There is no obvious decrease in activity after 20th recycle application (73 days) for hydrogen generation in air.Cobalt nanoparticles have attracted much attention in nanocatalysis due to their low cost and high activities. However, the easy-oxidative deactivation of cobalt nanocatalysts in air seriously limits their practical applications, especially in a long-time recycle application. Herein, by intentionally taking advantage of the readily oxidizable character of metallic cobalt, we describe a simple but efficient method to overcome the above obstacle through a free and reverse metal-ion conversion of cobalt in air at room temperature. With this novel method, the cobalt nanocatalyst demonstrates the superior activity even after the long-time (73 days) recycle application for hydrogen generation from ammonia borane.
Co-reporter:Q. G. Jiang, Z. M. Ao, W. T. Zheng, S. Li and Q. Jiang
Physical Chemistry Chemical Physics 2013 vol. 15(Issue 48) pp:21016-21022
Publication Date(Web):07 Oct 2013
DOI:10.1039/C3CP52976B
To facilitate the dissociative adsorption of H2 molecules on pristine graphene, the addition of a mono-atom-vacancy to graphene is proposed. This leads to reduction of the dissociative energy barrier for a H2 molecule on graphene from 3.097 to 0.805 eV for the first H2 and 0.869 eV for the second, according to first principles calculations. As a result, two H2 molecules can be easily dissociatively adsorbed on this defected graphene at room temperature. The electronic structure and conductivity of the graphene change significantly after H2 adsorption. In addition, the related dissociative adsorption phase diagrams under different temperatures and partial pressures show that this dissociative adsorption at room temperature is very sensitive (10−35 mol L−1). Therefore, this defected graphene is promising for ultra-sensitive room temperature hydrogen sensing.
Co-reporter:Q. G. Jiang, Z. M. Ao and Q. Jiang
Physical Chemistry Chemical Physics 2013 vol. 15(Issue 26) pp:10859-10865
Publication Date(Web):23 Apr 2013
DOI:10.1039/C3CP00128H
The effect of the Al dopant on the dissociative adsorption of a H2O molecule on graphene is investigated using first principles calculations. It is found that doping Al into graphene can facilitate the dissociative adsorption of H2O molecules. The dissociative energy barrier is reduced from 3.609 eV on pristine graphene to 0.456 eV on Al-doped graphene and the reaction releases an energy of 0.413 eV, which indicates a smooth dissociative adsorption on Al-doped graphene at room temperature. In addition, the dissociative adsorption of H2O molecules can convert the Al-doped graphene from hydrophobic to hydrophilic while obtaining conductive graphene with doping concentration higher than 5.56%. This hydrophilic and conductive graphene has potential applications in supercapacitors and biomaterial supports.
Co-reporter:T. H. Wang, Y. F. Zhu, and Q. Jiang
The Journal of Physical Chemistry C 2013 Volume 117(Issue 24) pp:12873-12881
Publication Date(Web):May 15, 2013
DOI:10.1021/jp402583j
The lack of a bandgap limits the application of pristine graphene in logic circuits and photonic devices. Breaking the inversion symmetry in bilayer graphene (BG) by charge transfer doping is a promising way to open a bandgap. In this work, a sizable bandgap is created in BG by the opposite doping from organic molecule and substrate. Our first-principles calculations have quantitatively identified that BG is n-doped in the N,N-dimethyl-p-phenylenediamine/BG (DMPD/BG) system while it is p-doped in the tetracyanoethylene/BG (TCNE/BG) system. The opposite p-doping from amorphous SiO2 substrate with O2– on its surface (a-SiO2-p) increases the bandgap of DMPD/BG from 106 to 253 meV. Similarly, the bandgap of TCNE/BG is enhanced from 98 to 211 meV by the opposite n-doping from Si-terminated 4H-SiC(0001) with a C buffer layer (C-SiC-n). Moreover, the molecular level of DMPD and a-SiO2-p related states locate below the opened bandgap, while the molecular levels of TCNE and C-SiC-n induced states lie above the bandgap. The increased bandgap without the intergap states should really improve the on/off current ratio of BG-based electronic devices. Meanwhile, the high carrier mobility is largely maintained due to the weak interaction at the interface. Thus, this work provides the scientific basis for further development in BG-based electronic devices.
Co-reporter:Q. Q. Dai, Y. F. Zhu, and Q. Jiang
The Journal of Physical Chemistry C 2013 Volume 117(Issue 9) pp:4791-4799
Publication Date(Web):February 15, 2013
DOI:10.1021/jp3068987
Using first-principles calculations, we perform a comprehensive study of the locations of a topological line defect (a line defect consisting of alternating pairs of pentagons and octagons or 585 LD) on the electronic and magnetic properties of zigzag graphene nanoribbon, with 12 zigzag chains (12-ZGNR) with or without tensile strain (ε). When ε = 0, it is found that 585 LD preferably forms near the edge. As 585 LD shifts from the center to the edge, the systems experience transitions from antiferromagnetic (AFM) semiconductors to an AFM half-metal and then to a ferromagnetic (FM) metal. As ε increases, the band gaps of the AFM semiconductors decrease and then the AFM semiconductors change into AFM half-metals. Finally, all the AFM systems turn into FM metals. The critical ε values of these transitions decrease as 585 LD moves to the edge. A similar behavior can also be found in 8- and 16-ZGNRs. However, the AFM half-metal region disappears in 8- and 16-ZGNRs due to different variation tendencies of the critical ε values for the electronic and magnetic phase transitions with the width of ZGNRs. These intriguing electronic and magnetic modulation behaviors make such defective ZGNRs very useful in nanoelectronic and spintronic devices.
Co-reporter:Zhi-Li Wang; Jun-Min Yan;Yun Ping;Hong-Li Wang; Wei-Tao Zheng ; Qing Jiang
Angewandte Chemie International Edition 2013 Volume 52( Issue 16) pp:4406-4409
Publication Date(Web):
DOI:10.1002/anie.201301009
Co-reporter:Tonghui Wang, Yongfu Zhu and Qing Jiang
Chemical Science 2012 vol. 3(Issue 2) pp:528-536
Publication Date(Web):13 Oct 2011
DOI:10.1039/C1SC00681A
The device performance of organic field-effect transistors depends strongly on the morphology and molecular orientation of the first few molecular layers near gate dielectrics, which are in turn governed by the initial growth stage. In this work, we establish a unified thermodynamic model to characterize the initial growth stage of disk-like and rod-like organic molecules during an organic vapor deposition process. Under a high substrate temperature and low deposition rate, the initially grown parallel cluster can transfer to the normal one at a critical molecular number Nc, which is determined by the competition between the surface energy of the molecule γf (surface energy of the molecular surface normal to the π–π interaction direction for a disk-like molecule or parallel to the molecular axis for a rod-like molecule) and that of the substrate γsub. By thermodynamic analyses and molecular dynamics simulations, we further confirm this transformation from disk-like phthalocyanine. When N < Nc, a parallel cluster is grown by self-assembly of individual lying down molecules driven by γf. At N ≥ Nc, together with γf > (5/7)γsub, the grown parallel cluster tilts down to form a normal one where Nc ≈ γfW/γlH (γl is the surface energy of the molecular surface parallel to the π–π interaction direction. W and H denote the molecular width and the intermolecular distance in the π–π interaction direction).
Co-reporter:Jun-Min Yan, Zhi-Li Wang, Hong-Li Wang and Qing Jiang
Journal of Materials Chemistry A 2012 vol. 22(Issue 22) pp:10990-10993
Publication Date(Web):29 Mar 2012
DOI:10.1039/C2JM31042B
A general and energy-efficient strategy has been successfully applied for synthesis of a graphene–CuCo nanohybrid, which leads to the highest catalytic activity of Cu-based catalysts up to now toward the dehydrogenation of ammonia borane, and also the excellent activity for electrochemical hydrogen evolution reaction. Moreover, this general method can be easily extended to facile preparation of other graphene–metal systems.
Co-reporter:P. Zhang, J. S. Lian and Q. Jiang
Physical Chemistry Chemical Physics 2012 vol. 14(Issue 33) pp:11715-11723
Publication Date(Web):09 Jul 2012
DOI:10.1039/C2CP40087A
Nitrogen-doped carbon nanotubes (NCNTs) are attractive for electrocatalytic applications in fuel cells due to their low cost and high electrocatalytic activity. By using density functional theory calculations, the electrocatalytic mechanisms of the oxygen reduction reaction (ORR) under electrochemical conditions are studied at graphite-like N groups (NG) and pyridine-like N groups (NP) of NCNTs, in which the effect of electrode potentials on the activation energy (Ea) and reaction energy (Er) is taken into account. The ORR occurs at both NG and NP defect sites via two different four-electron OOH and two-electron H2O2 mechanisms. At the lower potential region, both mechanisms are simultaneously responsible for the reaction at NG and NP defect sites; while at higher potentials, the four-electron mechanism becomes dominant and the ORR at NP defect sites is more energetically favorable than that at NG defect sites.
Co-reporter:Q. Q. Dai, Y. F. Zhu and Q. Jiang
Physical Chemistry Chemical Physics 2012 vol. 14(Issue 3) pp:1253-1261
Publication Date(Web):01 Dec 2011
DOI:10.1039/C1CP22866H
Stability, electronic and magnetic properties of triangular graphene nanoflakes embedded in graphane (graphane-embedded TGNFs) are investigated by density functional theory. It is found that the interface between the embedded TGNF and graphane is stable since the diffusion of H atoms from the graphane region to the embedded TGNF is energetically unfavorable with high energy barriers. The electronic and magnetic properties of the system completely depend on the embedded TGNF. The band gaps of graphane-embedded ATGNFs (armchair-edged TGNFs) arise due to the quantum confinement, while the special characteristics of nonbonding states of graphane-embedded ZTGNFs (zigzag-edged TGNFs) play an important role in their electronic properties. As the edge sizes increase, the differences of band gaps between graphane-embedded TGNFs and the isolated ones decrease. Furthermore, owing to the partially paired pz orbitals of edge C atoms, graphane-embedded ZTGNFs exhibit a ferrimagnetic ground state with size-dependant total spin being consistent with Lieb's theorem. Our work provides a possible way to obtain TGNFs without physical cutting.
Co-reporter:Nan Gao, Wei Tao Zheng and Qing Jiang
Physical Chemistry Chemical Physics 2012 vol. 14(Issue 1) pp:257-261
Publication Date(Web):14 Nov 2011
DOI:10.1039/C1CP22719J
The electronic structures and band gaps of silicene (the Si analogue of graphene) adsorbed with halogen elements are studied using the density functional theory based screened exchange local density approximation method. It is found that the band gaps of silicene adsorbed with F, Cl, Br and I have a nonmonotonic change as the periodic number of the halogen elements increases. This is attributed to the transfer of contributions to band gaps from Si–Si bonding to Si–halogen bonding.
Co-reporter:Hong-Li Wang, Jun-Min Yan, Zhi-Li Wang, Qing Jiang
International Journal of Hydrogen Energy 2012 Volume 37(Issue 13) pp:10229-10235
Publication Date(Web):July 2012
DOI:10.1016/j.ijhydene.2012.04.007
This paper investigates a facile and one-step synthesis of trimetallic magnetic Cu@FeNi core–shell nanoparticles, which are composed of crystalline Cu cores and amorphous FeNi shells, at room temperature under ambient atmosphere within 2 min. It is found that among the Cu@FeNi system, Cu0.4@Fe0.1Ni0.5 shows the best synergistic performance for catalyzing the hydrolytic dehydrogenation of ammonia borane with the activation energy of 32.9 kJ/mol, being lower than most of the reported data, and the catalytic activity of Cu0.4@Fe0.1Ni0.5 is much better than its monometallic, bimetallic and trimetallic counterparts whether in states of pure metals, alloys or physical mixtures. Further, the present catalyst has a good recycle stability with an easy magnetic separation method.Highlights► Cu0.4@Fe0.1Ni0.5 core–shell nanoparticles have been synthesized within 2 min. ► Cu0.4@Fe0.1Ni0.5 has good catalytic activity/stability to hydrogen generation. ► This work has innovation for catalyst synthesis and its application on energy.
Co-reporter:Zhi-Wei Zhang, Wei-Tao Zheng, Qing Jiang
International Journal of Hydrogen Energy 2012 Volume 37(Issue 6) pp:5090-5099
Publication Date(Web):March 2012
DOI:10.1016/j.ijhydene.2011.12.036
The adsorption of H2 on Ce-doped boron nitride nanotubes (BNNT) is investigated by using density functional theory. For the Ce/BNNT system, it is found that Ce preferentially occupies the hollow site over the BN hexagon. The results indicate that seven H2 per Ce can be adsorbed and 5.68 wt% H2 can be stored in Ce3/BNNT system. Among nanotubes doped with metals, Ce exhibits the most favorable hydrogen adsorption characteristics in terms of the adsorption energy and the uptake capacity. Both hybridization of the Ce-5d orbital with the H-1s orbital and the polarization of the H2 molecules contribute to the hydrogen adsorption. Ce clustering can be suppressed by preferential binding of Ce atoms on BNNT, which denotes that BNNT as a hydrogen storage substrate is better than CNT due to its heteropolar binding nature.Ce/BNNT system is a good candidate for hydrogen storage where seven H2 per Ce can be adsorbed.Highlights► Ce/BNNT system as a good candidate for hydrogen storage can adsorb seven H2 per Ce. ► BNNT as a hydrogen storage substrate is better than CNT. ► Metal clustering can be suppressed by preferential binding of metal atoms on BNNT. ► H2 adsorption is due to the electronic hybridization and electrostatic interactions.
Co-reporter:Q.G. Jiang, Z. Wen, Q. Jiang
Solid State Communications 2012 Volume 152(Issue 23) pp:2120-2122
Publication Date(Web):December 2012
DOI:10.1016/j.ssc.2012.09.010
We investigated the electronic properties of Zn-doped InAs/InP core-shell nanowires by using first principles calculations. It is found that efficient p-type doping of InAs nanowires can be achieved by remotely doping the InP shell. The activation energy of Zn dopant is zero since the valence band offset and one-dimensional hole gas is created in the InAs core without thermal activation. Moreover, the separation between the free carrier and ionized dopant may result in higher carrier mobility due to the reduced scattering. Our results provide insights for the efficient p-type doping of nanodevices based on III−V nanowires.Highlights► The VBM state is mainly confined in the core of the InAs/InP core-shell nanowires. ► Hole gas is created in the core without thermal activation by doping the shell. ► The separation between hole and dopant may result in higher carrier mobility. ► Remote doping provides insights for the efficient p-type doping of nanodevices.
Co-reporter:Mei Xia Xiao, Yong Fu Zhu, Qing Jiang
Solid State Communications 2012 Volume 152(Issue 3) pp:210-214
Publication Date(Web):February 2012
DOI:10.1016/j.ssc.2011.11.006
The atomic structures of α-Al2O3-coated Cu films doped with different concentrations of Al under external electric field FF are investigated using density-functional theory. As FF reaches 0.040 au (1 au=51.4 V/Å), large deformation is observed for pure Cu films, indicating the occurrence of electromigration (EM) in the Cu slabs. Under the same or even larger FF, in contrast, almost no deformation occurs for the α-Al2O3-coated Cu(Al) films, except that a slight change is found at the Cu(Al)/α-Al2O3 interfaces. The main reason for this stability should be attributed to the existence of Cu–O covalent–ionic and Al–O ionic bonds at the interface, suggesting that the EM reliability of Cu atoms can be effectively improved by the strong bonding strength.Highlights► We investigate the changes of four atomic structures under external electric fields. ► The Cu films undergo large deformation, indicating that electromigration occurs, as FF reaches 0.040 au (1 au = 51.4 V/Å). ► The Cu(Al) films at Cu(Al)/-Al2O3 interfaces change slightly under the same and larger FF. ► Cu–O covalent–ionic and Al–O ionic bonds exist at the Cu(Al)/-Al2O3 interfaces. ► The stronger bonding strength effectively improves the EM reliability of Cu atoms.
Co-reporter:Q. G. Jiang, Z. M. Ao, D. W. Chu, and Q. Jiang
The Journal of Physical Chemistry C 2012 Volume 116(Issue 36) pp:19321-19326
Publication Date(Web):August 22, 2012
DOI:10.1021/jp3050466
The catalytic effect of a perpendicular electric field on the reversible transition of graphene with water from hydrophobic to hydrophilic has been investigated by using first principles calculations. It is found that a negative electric field F can reduce the energy barrier for H2O dissociative adsorption on graphene, while a positive electric field has an opposite effect. Under F = −0.39 V/Å, the energy barrier becomes negative and the dissociative adsorption occurs smoothly without any potential barrier, which results in hydrophilic graphene. For the desorption of H and OH from graphene after the dissociative adsorption of the H2O molecule, the positive electric field of F = 0.36 V/Å leads to a negative desorption energy barrier and the desorption progress is present automatically, making the graphene hydrophobic again. Therefore, the electric field can act as a switch to reversibly change the graphene from hydrophobic to hydrophilic in the presence of water vapor.
Co-reporter:E. H. Song, J. M. Yan, J. S. Lian, and Q. Jiang
The Journal of Physical Chemistry C 2012 Volume 116(Issue 38) pp:20342-20348
Publication Date(Web):September 5, 2012
DOI:10.1021/jp304757f
Adsorption ability and reaction rate are two essential parameters that define the efficiency of a catalyst. Herein, we study the effects of the external electric field F on the catalytic decomposition of N2O on a Mn-embedded graphene system (Mn/graphene) based on density functional theory calculations. Our study demonstrates that Mn/graphene has a better adsorption ability than the corresponding typical catalysts, such as platinum group metals, while the appropriate positive F can make the N2O decomposition spontaneously occur via a two-step mechanism of N2O → N2 + O and N2O + O → N2 + O2. In addition, F simultaneously facilitates O2 desorption and regeneration of the Mn/graphene system, completing the whole catalytic cycle. The high synergetic catalytic effect may be attributed to that F induces an enhancement of the charge transfer between N2O and Mn/graphene. Thus, the Mn/graphene system together with the synergy of F is a good candidate for N2O adsorptive decomposition.
Co-reporter:P. Zhang ; X. F. Chen ; J. S. Lian ;Q. Jiang
The Journal of Physical Chemistry C 2012 Volume 116(Issue 33) pp:17572-17579
Publication Date(Web):August 2, 2012
DOI:10.1021/jp304097m
Fe/N/C electrocatalysts are attractive for electrocatalytical applications in fuel cells due to their low cost and high electrocatalytic activity. Because of its complex nature, the mechanism of CO oxidation on Fe/N/C electrocatalysts remains largely unknown. Aiming to provide insight into the mechanism of CO oxidation, we have performed extensive density functional theory calculations for the elementary steps in CO oxidation on Fe/N/C active sites, including Fe-N4 and Fe-N3 porphyrin-like carbon nanotube (T-FeN4 and T-FeN3), Fe-N4 porphyrin-like graphene (G-FeN4), and Fe-N2 nanoribbon (R-FeN2). It is found that CO adsorption and oxidation are very sensitive to the active site structures. CO adsorption is energetically more favorable than O2, and CO oxidation to CO2 hardly occurs on T-FeN4 and G-FeN4. In comparison, O2 prefers to adsorb and CO can easily be oxidized on T-FeN3 and R-FeN2, suggesting the CO tolerant property of T-FeN3 and R-FeN2.
Co-reporter:Ming Wu;Dr. Jun-Min Yan;Dr. Ming Zhao ;Dr. Qing Jiang
ChemPlusChem 2012 Volume 77( Issue 10) pp:931-935
Publication Date(Web):
DOI:10.1002/cplu.201200159
Abstract
An Ag2O–ZnO nanohybrid is synthesized for the first time through a facile, basic coprecipitation-assisted hydrothermal strategy. This novel method endows the Ag2O–ZnO nanohybrid (Ag2O/ZnO=0.3:0.7) with small particle size and strong electronic synergistic effects owing to the uniform distribution of the constituents. The as-synthesized nanohybrid shows excellent photocatalytic properties for degradation of rhodamine B, even under visible light irradiation. This effect is much better than pure or physical mixtures of Ag2O and ZnO, as well as the traditional homogenous Fenton catalyst (Fe3+/H2O2).
Co-reporter:Y. F. Zhu, W. T. Zheng and Q. Jiang
Physical Chemistry Chemical Physics 2011 vol. 13(Issue 48) pp:21328-21332
Publication Date(Web):31 Oct 2011
DOI:10.1039/C1CP22748C
Young's modulus (Y) of nanostructured materials (NSs) free of porosity is modeled with regard to the coordination number imperfection at grain boundaries. In light of it, Y of NSs is suppressed substantially in the whole solid temperature range, differing from the case of nanocrystals (NCs) where Y is enhanced at lower temperature (T) but weakened at higher T. It is found that, similar to NCs, the thermally-driven decline associated with the melting point depression plays an increasing role in suppressing Y of NSs on raising T. On the other hand, the lattice expansion and the bond weakening lead to a further suppression in Y of NSs independent of T, while the lattice contraction and the reinforced bonding strength result in an enhancement in Y of NCs, which should be responsible for the distinction in Y between NSs and NCs. The established functions were supported by available experimental and computer simulation results.
Co-reporter:Z. W. Zhang, W. T. Zheng and Q. Jiang
Physical Chemistry Chemical Physics 2011 vol. 13(Issue 20) pp:9483-9489
Publication Date(Web):12 Apr 2011
DOI:10.1039/C0CP02917C
The adsorption of H2 on Ce doped single-walled carbon nanotubes (SWCNT) and graphene are investigated by using density functional theory. For both systems, it is found that Ce preferentially occupies the hollow site on the outside. The results indicate that Ce/SWCNT system is a good candidate for hydrogen storage where six H2 per Ce can be adsorbed and 5.14 wt% H2 can be stored in the Ce3/SWCNT system. Among metal-doped SWCNTs, Ce exhibits the most favorable hydrogen adsorption characteristics in terms of the adsorption energy and the uptake capacity. The hybridization of the Ce-4f and Ce-5d orbitals with the H orbital contributes to the H2 binding where Ce-4f electrons participate in the hybridization due to the instability of the 4f state. The interaction between H2 and Ce/SWCNT is balanced by the electronic hybridization and electrostatic interactions. Curvature of SWCNT changes the size of the binding energy of Ce and C and the adsorption energy of H2 on Ce.
Co-reporter:M.X. Xiao, M. Zhao, Q. Jiang
Chemical Physics Letters 2011 Volume 512(4–6) pp:251-254
Publication Date(Web):25 August 2011
DOI:10.1016/j.cplett.2011.07.049
Abstract
Using density-functional theory, we investigate the effects of surface modifications on electronic properties of GaN/InN core/shell nanowires (CSNWs) with different core radii and shell thicknesses in triangular and hexagonal shapes. Our calculations demonstrate that surface modifications with H and F substantially modulate the band gaps and induce the separation of electrons and holes. The results elucidate that surface modifications change electronic structures of CSNWs with a transition from type-I band alignment to quasi-type-II, which could open a new way in the field of renewable energy applications.
Co-reporter:Ren Qin Zhang;Chao Hou;Nan Gao; Zi Wen; Qing Jiang
ChemPhysChem 2011 Volume 12( Issue 7) pp:1302-1309
Publication Date(Web):
DOI:10.1002/cphc.201100030
Abstract
The quantum confinement and electronic properties of silicon nanowires (SiNWs) under an external strain field ε and an electric field E—as well as both (ε plus E)—are systematically investigated using density functional theory. These two fields exist in working environments of integrated circuits. It is found that both ε and E lead to a drop of the band gap Eg(ε,E) of the SiNWs. If both fields coexist, the interaction between ε and E causes that Eg(ε,E) becomes orientation-dependent, which results from variations of both the conduction-band minimum and the valence-band maximum. The interaction is further illustrated by the density of states near the Fermi level and the eigenvalue of the highest occupied molecular orbital.
Co-reporter:R.Q. Zhang ; X.M. Liu ; Z. Wen ;Q Jiang.
The Journal of Physical Chemistry C 2011 Volume 115(Issue 8) pp:3425-3428
Publication Date(Web):February 3, 2011
DOI:10.1021/jp111182c
Hydrogen as an efficient energy carrier is an environmentally benign fuel of the future. Solar-powered water splitting, using semiconductor photocatalysts, is an efficient generation method of hydrogen where excellent photocatalysts are key factors. In this work, we investigate silicon nanowires (SiNWs) as photocatalysts for the water splitting. By utilizing density functional theory calculations, we demonstrated that SiNWs terminated with suitable H and Cl surface coverage should be a promising photocatalyst for this purpose. The interaction between Cl-3p and surface Si-3p states of SiNWs leads to suitable reducing and oxidizing powers simultaneously while the separation of HOMO and LUMO of SiNWs prevents the electron−hole recombination.
Co-reporter:E. H. Song ; Z. Wen ;Q. Jiang
The Journal of Physical Chemistry C 2011 Volume 115(Issue 9) pp:3678-3683
Publication Date(Web):February 11, 2011
DOI:10.1021/jp108978c
The catalytic oxidation of CO on Cu-embedded graphene is investigated by DFT. The reaction proceeds via a two-step mechanism of CO + O2 → OOCO → CO2 + O and CO + O → CO2. The energy barriers of the former are 0.25 and 0.54 eV, respectively, while the latter is a process with energetic drop. The high activity of Cu-embedded graphene may be attributed to the electronic resonance among electronic states of CO, O2, and the Cu atom, particularly among Cu-3d, CO-2π*, and O2-2π* orbitals. This good catalytic activity opens a new avenue to fabricate carbon-based catalysts for CO oxidation with lower cost and higher activity.
Co-reporter:Grégory Guisbiers, Di Liu, Qing Jiang and Lionel Buchaillot
Physical Chemistry Chemical Physics 2010 vol. 12(Issue 26) pp:7203-7210
Publication Date(Web):19 May 2010
DOI:10.1039/C002496A
In this paper, top-down and bottom-up approaches are used to predict material properties of group III-nitride nanostructures. The first approach calculates the melting temperature, melting enthalpy, Debye temperature and energy bandgap of InN, GaN and AlN through classical thermodynamics. The second approach calculates the surface energies in the liquid and solid states of the considered nitrides materials through molecular dynamics. Moreover, the liquid and solid surface energies of the zinc-blende and wurtzite III–V materials are compared. Finally, the phase diagram of a ternary III-nitride nanomaterial, AlGaN, is presented and the variation of its energy bandgap with composition is predicted.
Co-reporter:L.J. Zhao, Q. Jiang
Materials Letters 2010 Volume 64(Issue 6) pp:677-679
Publication Date(Web):31 March 2010
DOI:10.1016/j.matlet.2009.12.036
A facile solvothermal route is used for the synthesis of Co/CoFe2O4 nanobelts by rationally manipulating the dosages of a surfactant Poly(vinylpyrrolidone) (PVP, MW 40000). PVP plays a pivotal role in preparing the Co/CoFe2O4 nanobelts. The optimal dosage for the synthesis of the Co/CoFe2O4 nanobelts is 0.5 g. Lower than this value, octahedral particles and nanobelts were coexistent; higher than this value, octahedral particles were obtained. Furthermore, the possible formation mechanism of Co/CoFe2O4 nanobelts was proposed. A small quantity of Co2+ ions are reduced by glycerol, which is the reason for the presence of metallic Co in the CoFe2O4 ferrite. The Co/CoFe2O4 nanobelts may be very attractive for potential applications because of their outstanding magnetic properties (Ms = 110 emu/g, Hc = 387 Oe).
Co-reporter:C. Li, J.C. Li, Q. Jiang
Solid State Communications 2010 Volume 150(37–38) pp:1818-1821
Publication Date(Web):October 2010
DOI:10.1016/j.ssc.2010.07.005
The Phillips ionicity is modified, simulated and calculated for conductors. The results show that the percentage of metallic bonding in multiplex chemical bonds of transition metal (TM) carbides and nitrides is large; this affects the Phillips ionicity. The redefinition of Phillips ionicity has been applied to estimate the hardness of TM carbides and nitrides; the values obtained are in agreement with experimental and theoretical evidence. In addition, materials with the zinc blende structure are harder than those with rock salt structure.
Co-reporter:Z.M. Ao, S. Li, Q. Jiang
Solid State Communications 2010 Volume 150(13–14) pp:680-683
Publication Date(Web):April 2010
DOI:10.1016/j.ssc.2009.12.016
Recently, Al-doped graphene was proposed as a highly sensitive CO gas sensor material. In this work, the correlation of the applied electric field FF and the adsorption/desorption behavior of a CO molecule on Al-doped graphene was studied by density functional theory calculations. The results indicate that a negative FF strengthens the adsorption of the CO on the Al-doped graphene, while the adsorption is reduced when a positive FF is present. Furthermore, desorption of the CO molecule from the graphene layer commences when F≥0.03a.u. is applied, which can be used to reactivate the sensor material for repetitious application.
Co-reporter:Z. W. Zhang, J. C. Li and Q. Jiang
The Journal of Physical Chemistry C 2010 Volume 114(Issue 17) pp:7733-7737
Publication Date(Web):April 6, 2010
DOI:10.1021/jp100017y
Within the first-principles density functional theory, we investigate the interaction between H2 and Eu-doped single-walled carbon nanotubes (SWCNT). For the Eu/SWCNT system, the hollow site on the outer wall of SWCNT is the most favorable for the adsorption. The charge analysis results show that two 6s electrons in Eu transfer to SWCNT while 4f electrons remain in Eu, and the Eu atom is thus divalent. The results indicate that five H2 per Eu atom can be adsorbed in the Eu/SWCNT system while 4.44 wt % H2 can be stored in the Eu3/SWCNT system. The interaction between H2 and Eu/SWCNT is balanced by the electronic hybridization and electrostatic interactions.
Co-reporter:W. Gao, X. F. Chen, J. C. Li and Q. Jiang
The Journal of Physical Chemistry C 2010 Volume 114(Issue 2) pp:1148-1153
Publication Date(Web):November 24, 2009
DOI:10.1021/jp909345j
The styrene epoxidation on Au38 and Au55 clusters, which could be a benchmark to probe high catalytic activity of gold clusters, has been studied by using density functional theory. Results suggest that epoxidation proceeds via a surface oxametallacycle intermediate (OME structure). Two parallel reaction pathways coexist on the Au38 cluster: O2 dissociates before epoxidation and O2 directly reacts with styrene, whereas only the latter pathway is found on the Au55 cluster, which is induced by different geometries of the Au38 and Au55 clusters. The mechanism of O2 directly reacting is essentially determined by the electronic resonance between electronic states of adsorbed intermediates and Au atoms at reaction sites. Moreover, Au atoms correlated with the reaction on the Au38 cluster are more electropositive than those on the Au55 cluster, which leads to a higher catalytic activity of the former. Thus, the Au38 cluster should be the size threshold for epoxidation catalysis, being consistent with the obtained barrier values.
Co-reporter:P. Zhang ; W. T. Zheng ;Q. Jiang
The Journal of Physical Chemistry C 2010 Volume 114(Issue 45) pp:19331-19337
Publication Date(Web):October 28, 2010
DOI:10.1021/jp105180d
Ab initio density functional theory has been used to investigate the effects of surface charge on adsorption and dissociation of H2O on the Cu(111) surface. The adsorption energies at all high symmetry adsorption sites are similar on the negatively charged surface, indicating that there is no preferable adsorption site. While on the positively charged surface, H2O molecule on the atop site has the strongest adsorption among all adsorption sites. We also show that changes in the surface charge can significantly alter the activation energy of dissociation as well as the mechanism selectivity.
Co-reporter:W. Liu ; Y. F. Zhu ;Q. Jiang
The Journal of Physical Chemistry C 2010 Volume 114(Issue 49) pp:21094-21099
Publication Date(Web):November 15, 2010
DOI:10.1021/jp107251a
First-principles calculations are performed to study the adsorption and oxidation of CO on three decahedral Au clusters with the stability sequence of Au146 > Au75 > Au101. Our calculations suggest that a cluster with a moderate stability should be an ideal catalyst when structural differences are excluded. As exemplified in our case, Au75 is the best catalyst since O2 adsorption on Au146 is endothermic (adsorption energy Ead = −0.13 eV), whereas CO oxidation on Au101 has the highest activation energy (Ea = 0.75 eV). Reactions are found to be particularly sensitive to the direction and intensity of an electric field, where the magnitude of Ea is considerably lowered from 0.55 to 0.32 eV after superimposing a −0.005 au field into the Au75 cluster. The promoted reactivity in the oxidation stage is ascribed to the lowered Fermi level and enhanced charge transfer between the adsorbates and the catalyst. Our calculations demonstrate that moderate field intensity is a better option for CO oxidation reaction since a strong electric field dramatically weakens the adsorption of the reactants.
Co-reporter:Y. F. Zhu, X. Y. Lang, W. T. Zheng and Q. Jiang
ACS Nano 2010 Volume 4(Issue 7) pp:3781
Publication Date(Web):June 17, 2010
DOI:10.1021/nn101014k
For electrical conductance in polycrystalline metallic films and wires, the reflection coefficient of electrons at grain boundaries is explored and found to be proportional to the square root of the melting points of metals. As validated by available experimental results, this exploration enables classical models to take an essential role in theoretically predicting the electrical conductance of low-dimensional metals. One thus sees that the mechanism dominating the suppression of electrical conductance is transformed from the surface scattering into the grain boundary scattering as the ratio of film thickness (or wire diameter) to grain size rises. Furthermore, the impact of grain boundary scattering becomes less important for metals with lower melting points.Keywords: electrical conductance; films; grain boundary scattering; polycrystalline; surface scattering; wires
Co-reporter:W. Liu, Y.H. Zhao, J. Nguyen, Y. Li, Q. Jiang, E.J. Lavernia
Carbon 2009 Volume 47(Issue 15) pp:3452-3460
Publication Date(Web):December 2009
DOI:10.1016/j.carbon.2009.08.012
In an ideal hydrogen storage system, binding strength should increase during adsorption whereas the opposite should be the case during desorption. These two seemingly contradictory requirements limit the types of systems that can be utilized. Density-functional theory (DFT) calculations are carried out to investigate hydrogen physisorption on Li-doped single-layer and bilayer graphenes. We propose that the superimposition of an electric field can be used to effectively control hydrogen adsorption. More specifically, we report that hydrogen binding can be enhanced under a positive electric field, whereas it can be weakened under a negative electric field. Our results show that the binding strength increases by 88% when a field with a magnitude of +0.020 au is imposed. Hirshfeld charge analysis results suggest that an increase in the binding strength will occur as long as the Li (or C) carries more positive (or negative) charges. Our calculations demonstrate that, in the case of Li-doped graphene, the application of a positive electric field yields an increase in binding strength during adsorption while a negative field decreases the binding strength during desorption.
Co-reporter:W. Liu, Y. H. Zhao, Y. Li, E. J. Lavernia and Q. Jiang
Physical Chemistry Chemical Physics 2009 vol. 11(Issue 40) pp:9233-9240
Publication Date(Web):17 Aug 2009
DOI:10.1039/B907591G
Implementation of hydrogen storage systems requires moderate bonding strength. However, this goal has remained a challenge, either due to the weak physisorption or extremely strong chemisorption. Here, we report on a new phenomenon, namely that H2 binding can be externally enhanced (or weakened) via superimposition of a positive (or negative) electric field. We demonstrate this concept using an 8-Li-doped carbon nanotube. The calculated adsorption energy Ead = −0.58 eV/H2 under F = +0.010 au is 93.33% lower than that under 0.000 au (F indicates the field intensity). This is because the positive field produces an extra dipole moment. In contrast, Ead increases from −0.30 to −0.20 eV/H2 when F = −0.010 au. In view of the fact that storage systems are insensitive to small unexpected field fluctuations, the application of the electric field as a reversible switch makes practical sense.
Co-reporter:Z. M. Ao, S. Li and Q. Jiang
Physical Chemistry Chemical Physics 2009 vol. 11(Issue 11) pp:1683-1687
Publication Date(Web):29 Jan 2009
DOI:10.1039/B812188E
The thermal stability of interaction between CO molecules and Al doped graphene is studied using ab initio molecular dynamics calculations to reveal the adsorption/desorption behavior of the system. With these results, an adsorption–desorption phase diagram was established with atomic thermodynamics. The temperature (T) dependent desorption time τ(T) was determined with a thermal desorption method. The results show that the optimal desorption temperature is 400 K. The effect of T on atomic structure parameters and electrical properties were analyzed. It shows that the maximum variation of electrical conductivity induced by the adsorption occurs at 400 K, indicating that the best sensing performance of the devices should be at this particular temperature.
Co-reporter:Z.M. Ao, T.T. Tan, S. Li, Q. Jiang
Solid State Communications 2009 Volume 149(33–34) pp:1363-1367
Publication Date(Web):September 2009
DOI:10.1016/j.ssc.2009.05.022
Molecular hydrogen storage at room temperature in Al-doped bulk graphite with wider layer distances was studied using density functional theory calculation. Hydrogen storage capacity of 3.48 wt% or volume density of 51 kg/m3 was predicted at T=300 K and P=0.1 GPa with adsorption energy Eb=−0.264 eV/H2. This is close to the target of volume density 62 kg/m3 and satisfies the requirement of immobilization hydrogen with binding strength of 0.2–0.7 eV/H2 at ambient temperature and modest pressure for commercial applications specified by the U.S. Department of Energy.
Co-reporter:Y. F. Zhu, J. S. Lian and Q. Jiang
The Journal of Physical Chemistry C 2009 Volume 113(Issue 39) pp:16896-16900
Publication Date(Web):September 10, 2009
DOI:10.1021/jp902097f
The size-dependences of the melting point, Debye temperature, thermal expansion coefficient, and the specific heat of nanostructured materials have been modeled free of adjustable parameters. The melting point and Debye temperature drop while the thermal expansion coefficient and specific heat rise when the grain size is decreased. Relative to nanoparticles, however, the variation of the above parameters of nanostructured material is weak, dominated by the ratio of the grain boundary energy to the surface energy. Our theoretical predictions agree fairly well with available experimental and computer simulation results for semiconductors and metals.
Co-reporter:D. Liu, Y. F. Zhu and Q. Jiang
The Journal of Physical Chemistry C 2009 Volume 113(Issue 25) pp:10907-10912
Publication Date(Web):May 28, 2009
DOI:10.1021/jp901797w
The cohesive energy of Ag clusters at any site x with the magic number N [Ecx(N)] is determined through calculating the vacancy formation energy Evx(N) using density functional theory and theoretical modeling. It is found that Ecx(N) is quite distinct at different surface and interior atomic sites within the same cluster. Ecx(N) is also structure dependent. Ecx(N) values of the core atoms with an icosahedron structure are much larger than the corresponding bulk value Ec(∞) due to the pressure-induced d−d shells repulsion and the sp−d hybridization weakening.
Co-reporter:R. Q. Zhang, W. T. Zheng and Q. Jiang
The Journal of Physical Chemistry C 2009 Volume 113(Issue 24) pp:10384-10389
Publication Date(Web):May 27, 2009
DOI:10.1021/jp809455w
The effects of external electric field F on band gap Eg(D, F) of silicon nanowires (SiNWs) in a diameter range of D = 0.45−1.79 nm are quantitatively calculated using density functional theory. The results show that Eg(D, F) decreases with increasing F due to the rapid drop of the conduction band maximum of SiNWs. As F increases, Eg(D, F) → 0 except at D = 0.45 nm. Further increasing of F results in breakdown of the geometry structure of SiNWs. In addition, the bond lengths and angles of SiNWs are also functions of F. These findings imply that Eg(D, F) functions of SiNWs can be modulated by manipulating D and F.
Co-reporter:D. Liu, J. S. Lian and Q. Jiang
The Journal of Physical Chemistry C 2009 Volume 113(Issue 4) pp:1168-1170
Publication Date(Web):2017-2-22
DOI:10.1021/jp810220f
Size-dependent surface energy associated with atomic number N, γ(N), of Ag quasicrystal clusters was investigated using density functional theory and broken-bond theory. It is found that the value of γ(N) is 0.55−0.66 eV/atom, similar to the value of their counterparts in bulk. This is due to the increase of cohesive energy Ec(N) and the decrease of surface coordinate number associated with the decreasing of N. As N decreases, the partial density of states shifts to higher binding energy, and there is electronic charge transfer from the sp band into the d band, which leads to the increase of cohesive energy.
Co-reporter:W. Liu, Y. H. Zhao, Y. Li, Q. Jiang and E. J. Lavernia
The Journal of Physical Chemistry C 2009 Volume 113(Issue 5) pp:2028-2033
Publication Date(Web):2017-2-22
DOI:10.1021/jp8091418
High storage capacity and a moderate binding strength are two important requirements that must be met for the successful development of hydrogen storage materials. In the present work we demonstrate that optimizing the number and position of dopants, a configuration of eight Li dispersed at the hollow sites above the hexagonal carbon rings, can lead to an extremely high H2 storage capacity of 13.45 wt %. Moreover, our local density approximation calculations predict that the average adsorption energy is −0.17 eV/H2, which is close to the lowest requirement (−0.20 eV/H2) as proposed by the U.S. Department of Energy. The electronic analysis demonstrates two salient points, namely that the best dopants are those whose bands overlap strongly with those of H2 and the nanotube simultaneously; second, all carbon atoms in the nanotube are fully ionized and thus the high capacity is attainable. These results provide insight into the binding mechanisms that govern hydrogen storage.
Co-reporter:H. Li, M. Zhao and Q. Jiang
The Journal of Physical Chemistry C 2009 Volume 113(Issue 18) pp:7594-7597
Publication Date(Web):April 8, 2009
DOI:10.1021/jp902319z
The geometrical and energetic characteristics of Wulff construction are expressed by variants δ, Ba/Bt, and Ec(N)/Eb0 in an N atom system, where δ = Ns/N is the surface/volume ratio with Ns being the surface atom number, Ba is the rest bond number, Bt denotes the total bond number without broken bonds, and Ec(N) and Eb0 are the cohesive energy values in an N atom system and in bulk. It is found that these functions of Wulff construction correspond to that of several standard clusters. Thus, Wulff construction as a first-order approximation could estimate the shape and energy of clusters without any structural consideration.
Co-reporter:Wei Liu;Yonghao Zhao Dr.;Renqin Zhang;Ying Li Dr.;Enrique J. Lavernia
ChemPhysChem 2009 Volume 10( Issue 18) pp:3295-3302
Publication Date(Web):
DOI:10.1002/cphc.200900431
Abstract
Adsorption ability and reaction rate are two essential parameters that define the efficiency of a catalyst. Herein, we implement density functional theory (DFT) and report that CO can be oxidized by a pyramidal Cu cluster with an associated reaction barrier Eb=1.317 eV. In this case, our transition state calculations reveal that the barrier can be significantly lowered after superimposing a negative electric field. Moreover, when the field intensity corresponds to F=−0.010 au, the magnitude of Eb=0.698 eV is equivalent to—or lower than—those of typical catalysts such as Pt, Rh, and Pd. The superimposition of a positive field is found to enhance the release of the nascent CO2 molecule. Our study demonstrates that small Cu clusters have better adsorption ability than the corresponding flat surface while the field can be used to enhance the purification of the exhaust gas.
Co-reporter:Yong Fu Zhu;Xing You Lang
Advanced Functional Materials 2008 Volume 18( Issue 9) pp:1422-1429
Publication Date(Web):
DOI:10.1002/adfm.200700857
Abstract
Based on a model for the size-dependent bandgap energy of low-dimensional semiconductor compounds, the alloying effect on the bandgap of nanoscale semiconductors is modeled without any adjustable parameter. The model predicts not only a trend of increasing bandgap with decreasing nanocrystal size but also Végard¢s relationship between the bandgap and the alloy composition when the size drops close to twice that of the critical size for the nanocrystals. The model predictions agree with available experimental results for bandgap changes of pseudo-binary IIB–VIB chalcogenide semiconductor nanocrystals.
Co-reporter:Q. Jiang, H.M. Lu
Surface Science Reports 2008 Volume 63(Issue 10) pp:427-464
Publication Date(Web):31 October 2008
DOI:10.1016/j.surfrep.2008.07.001
Reducing the sizes of low dimensional materials leads to dramatic increase in the portion of surface/interface atoms. The properties of a solid are essentially controlled by related surface/interface energies. Although such changes are believed to dominate behaviors of nanoscale structures, little experience or intuition for the expected phenomena, especially for the size-dependence of the energies and their practical implications, are modeled analytically. In this contribution, the classic thermodynamics as a powerful traditional theoretical tool is used to model different bulk interface energies and the corresponding size dependences. During the modeling, an emphasis on size dependences of the interface energies is given, which is induced by size dependence of coherent energy of atoms within nanocrystals. It is found that solid–vapor interface energy, liquid–vapor interface energy, solid–liquid interface energy, and solid–solid interface energy of nanoparticles and thin films fall as their diameters or thickness decrease to several nanometers while the solid–vapor interface energy ratio between different facets is size-independent and equals to the corresponding bulk value. The predictions of the established analytic models without any free parameters, such as size and temperature, dependences of these four kinds of interface energies and related surface stress, correspond to experimental or other theoretical results. The above established models are suitable for low-dimensional materials with different dimensions and different chemical bond natures. Moreover, several related applications in the fields of nanophase transitions, nanocrystal growth, and self-diffusion of liquids are provided.
Co-reporter:S. Li, Z. Wen, Q. Jiang
Scripta Materialia 2008 Volume 59(Issue 5) pp:526-529
Publication Date(Web):September 2008
DOI:10.1016/j.scriptamat.2008.04.046
After considering the effects of surface energy and surface-stress-induced pressure on the total Gibbs free energy of nanocrystals, the size-dependent solid transition pressures for CdSe and ZnO nanocrystals have been determined quantitatively. It is found that the transition pressure increases as the nanocrystals become smaller. The transition pressure change is dominated by surface-stress for CdSe, while surface energy dominates for ZnO. The calculated results are supported by the corresponding experimental results.
Co-reporter:Z.M. Ao, J. Yang, S. Li, Q. Jiang
Chemical Physics Letters 2008 Volume 461(4–6) pp:276-279
Publication Date(Web):20 August 2008
DOI:10.1016/j.cplett.2008.07.039
Abstract
A principle of the enhancement of CO adsorption was developed theoretically by using density functional theory through doping Al into graphene. The results show that the Al doped graphene has strong chemisorption of CO molecule by forming Al–CO bond, where CO onto intrinsic graphene remains weak physisorption. Furthermore, the enhancement of CO sensitivity in the Al doped graphene is determined by a large electrical conductivity change after adsorption, where CO absorption leads to increase of electrical conductivity via introducing large amount of shallow acceptor states. Therefore, this newly developed Al doped graphene would be an excellent candidate for sensing CO gas.
Co-reporter:T.H. Wang, Y.F. Zhu, Q. Jiang
Materials Chemistry and Physics 2008 Volume 111(2–3) pp:293-295
Publication Date(Web):15 October 2008
DOI:10.1016/j.matchemphys.2008.04.010
Based on our model for size-dependent cohesive energy, the size-dependent evaporation temperature of nanocrystals has been modeled without any adjustable parameter. The model predicts a decrease of the evaporation temperature of nanocrystals with decreasing size. The model predictions are in good agreement with available experimental results for Ag, Au and PbS nanocrystals.
Co-reporter:H. Li, Z. Wen, Q. Jiang
Solid State Communications 2008 Volume 147(7–8) pp:250-253
Publication Date(Web):August 2008
DOI:10.1016/j.ssc.2008.06.004
According to the classical nucleation theory, an estimation for homogeneous nucleation temperature of liquid from nanovoids within a surface-free bulk material is developed by considering energetic contributions of surface (interface) energy and surface (interface) stress on total Gibbs free energy. The model predicts a kinetic superheating limit temperature TmaxTmax, which is larger than the corresponding bulk value of Tm0 and is a function of void size. The increase of TmaxTmax is enhanced as the nanovoid size decreases, which can well explain the molecular dynamics simulation results of melting points TmTm of argon crystal.
Co-reporter:W. Liu ; Y. H. Zhao ; E. J. Lavernia ;Q. Jiang
The Journal of Physical Chemistry C 2008 Volume 112(Issue 20) pp:7672-7677
Publication Date(Web):April 30, 2008
DOI:10.1021/jp800441w
Density functional calculations are implemented to study the interaction of CO, H, and C with a sequential growth of Cu clusters with a special structure (5 ≤ n ≤ 140, where n is the number of atoms). The cohesive energy Ec and average bond length dave of the relaxed Cu clusters increase monotonically as the layer number of the clusters l increases. The adsorption energy Ead values have a sequence of C/Cu < H/Cu < CO/Cu (adsorbate/substrate). The Ead(l) functions are found to be parabola-like for all adsorption systems, with the maximum values at l = 5−6 where dave ≈ 2.56 Å, which is approximately equal to the atomic distance of Cu in bulk crystals. The binding strength between the adsorbate and substrate, or −Ead(l), is inversely proportional to their corresponding bond length d.
Co-reporter:C. He ; P. Zhang ; Y. F. Zhu ;Q. Jiang
The Journal of Physical Chemistry C 2008 Volume 112(Issue 24) pp:9045-9049
Publication Date(Web):May 22, 2008
DOI:10.1021/jp800855r
The ballistic transport properties of Cu nanowires (NWs) under electric fields are investigated using first-principles density function theory for future application as interconnects in microelectronics. It is found that as electric field strength increases, the amount of quantum conduction of a nonhelical atomic strand decreases, while that of a helical atomic strand is in an opposite tendency. The changes are decided by the changes of atomic layer distance of the NWs and the related electronic distribution along the axis of the NWs.
Co-reporter:W. Liu, D. Liu, W. T. Zheng and Q. Jiang
The Journal of Physical Chemistry C 2008 Volume 112(Issue 48) pp:18840-18845
Publication Date(Web):2017-2-22
DOI:10.1021/jp7114143
The cohesive energy of Cu clusters (Ec) containing different numbers of atoms (n) in the metastable structures of pyramids, nanotubes, nanorods, films, and icosahedrons is determined using ab initio density functional theory (DFT). Modeling of Ec(n) functions is also implemented and discussed. Both theoretical and simulation results show that Ec(n) is a function of the surface bond deficit, and Ec(n) increases monotonically as n decreases, as follows: EcNanotube(n) > EcPyramid(n) > EcIcosahedron(n) > EcNanorod(n) > EcFilm(n) for a given n. This observed continuity of the Ec(n) functions implies that the quantum effect of Ec(n < nc) is not influenced by n or a size effect but instead by a structural effect, where nc denotes a critical value of n when the bulk crystalline structure is no longer stable for n < nc. This suggestion is in good agreement with the results obtained from the observed distributions of the density of states (DOS).
Co-reporter:Wang Gao Dr.;Ming Zhao
ChemPhysChem 2008 Volume 9( Issue 14) pp:2092-2098
Publication Date(Web):
DOI:10.1002/cphc.200800150
Abstract
The non-CO-involved oxidation of methanol (NCOIOM) on a Pt(111) surface is investigated by using density functional theory. Relative energy diagrams for the NCOIOM are established in which the reaction mechanisms for a catalytic cycle—including the associated barriers, the reactive energies, the intermediates, and the transient states—are shown. The results indicate that the reaction proceeds via the kinetically favored pathways: A) HCOHHC(OH)2HCOOHHCOO- [-COOH]CO2 and B) CHOHCOOHHCOO- [-COOH]CO2, with OH playing a key role in the entire process. The vibrational frequencies of the intermediate states derived from the calculations are in agreement with the experimental measurements.
Co-reporter:H.M. Lu;Z. Wen;Q. Jiang
Journal of Physical Organic Chemistry 2007 Volume 20(Issue 4) pp:236-240
Publication Date(Web):12 APR 2007
DOI:10.1002/poc.1136
A simple thermodynamic model, originally developed for metals based on the Gibbs–Thomson equation and related considerations for homogeneous nucleation, has been extended to predict the solid–liquid interface energy γsl of organic crystals. The model predictions correspond to available experimental and other theoretical results for 38 organic crystals. Copyright © 2007 John Wiley & Sons, Ltd.
Co-reporter:D. Liu, Y.F. Zhu, Q. Jiang
Materials Letters 2007 Volume 61(Issue 30) pp:5199-5201
Publication Date(Web):December 2007
DOI:10.1016/j.matlet.2007.04.029
Based on the classical elastic theory and a thermodynamic model for surface energy, the critical layer number nc of Stranski–Krastanov growth mode epitaxial growth for bcc metallic thin films is calculated. nc is determined by the consideration that the sum of the surface energy of a film and the lattice mismatch elastic energy between a substrate and the film is equal to the surface energy of the substrate. When the film layer number n is larger than nc, a flat growth of the film on the substrate will transform to an island growth. Our predictions on several metallic films are in agreement with experimental results.
Co-reporter:X. Liu, P. Yang, Q. Jiang
Materials Chemistry and Physics 2007 Volume 103(Issue 1) pp:1-4
Publication Date(Web):15 May 2007
DOI:10.1016/j.matchemphys.2007.01.014
This study was conducted to predict the size-dependent melting temperatures of nanostructured griseofulvin (C17H17ClO6) and nifedipine (C17H18N2O6) drugs in their stable states embedded in polymer matrix based on a previous model for melting temperatures of nanocrystals. It is found that when the size of the drugs drops to several nanometers, the drops of the corresponding melting temperatures are more than 10%. Available experimental evidences support the model predictions.
Co-reporter:X.Y. Lang;Q. Jiang
Journal of Nanoparticle Research 2007 Volume 9( Issue 4) pp:595-603
Publication Date(Web):2007 August
DOI:10.1007/s11051-005-9066-1
A simple and unified model, without any adjustable parameter, is established for size effect on Curie temperature of low-dimensional ferroelectrics (thin films, nanowires and nanoparticles), Tc(D), where D denotes size of low-dimensional ferroelectrics. Tc(D) function is based on consideration on the size dependence of spontaneous polarization of low-dimensional ferroelectrics Ps(D), which is determined by the misfit strain at the ferroelectrics/substrate interface. It is shown that Ps(D) and Tc(D) functions decrease or increase when the misfit strain is tensile or compressive. The numerically predicted results are in agreement with the available experimental results of BaTiO3 and PbTiO3 nanoparticles and thin films.
Co-reporter:S. Li, W.T. Zheng, Q. Jiang
Scripta Materialia 2006 Volume 54(Issue 12) pp:2091-2094
Publication Date(Web):June 2006
DOI:10.1016/j.scriptamat.2006.03.002
Transition temperatures between tetragonal and monoclinic polymorphs of ZrO2 nanoparticles, thin films and nanostructured materials are calculated by considering energetic contributions of surface (interface) energy and surface stress on total Gibbs free energy. The transition temperatures drop as the size of the nanocrystals decreases, which is consistent with available results.
Co-reporter:W. Liu, X. Liu, W.T. Zheng, Q. Jiang
Surface Science 2006 Volume 600(Issue 2) pp:257-264
Publication Date(Web):15 January 2006
DOI:10.1016/j.susc.2005.10.035
Co-reporter:C.C. Yang, M.X. Xiao, W. Li, Q. Jiang
Solid State Communications 2006 Volume 139(Issue 4) pp:148-152
Publication Date(Web):July 2006
DOI:10.1016/j.ssc.2006.05.035
Based on a size-dependent root of mean square amplitude (rms) model, the size-dependent Debye temperatures of nanocrystals are modeled without any adjustable parameter by considering both Lindemann’s criterion and Mott’s equation. In terms of this model, the Debye temperatures depend on both size and interface conditions, which lead to related applications on size effects of the Einstein temperature and the volume thermal expansion coefficient. It is found that the model’s predictions are in good agreement with available experimental and computer simulation results.
Co-reporter:X.Y. Lang, G.H. Zhang, J.S. Lian, Q. Jiang
Thin Solid Films 2006 Volume 497(1–2) pp:333-337
Publication Date(Web):21 February 2006
DOI:10.1016/j.tsf.2005.10.001
A simple and unified model, without any adjustable parameter, is developed for size and pressure effects on glass transition temperatures of nanopolymers. The model is based on a model for size dependent glass transition temperature of nanopolymer glasses under ambient pressure, and a pressure-dependent function of the root of mean-square displacement of atom vibration. It is found that the size- and pressure-dependent glass transition temperatures of free-standing films or supported films having weak interaction with substrates decreases with decreasing of pressure and size. However, the glass transition temperature of supported films having strong interaction with substrates increases with the increase of pressure and the decrease of size. The predicted results correspond with available experimental evidences for atactic-Poly (methyl methacrylate) thin films under hydrostatic pressure or under the pressure induced by supercritical fluid CO2. In addition, the predicted glass transition temperature of isotactic-Poly (methyl methacrylate) thin films under ambient pressure is consistent with available experimental evidences.
Co-reporter:C.C. Yang, Q. Jiang
Materials Science and Engineering: B 2006 Volume 131(1–3) pp:191-194
Publication Date(Web):15 July 2006
DOI:10.1016/j.mseb.2006.04.016
Based on a model for size-dependent cohesive energy, the size-dependent bandgap of II–VI semiconductor nanocrystals are modeled without any adjustable parameter. The model predicts an increase of the bandgap of semiconductors with decreasing of crystalline sizes. The model predictions are supported by the available experimental results.
Co-reporter:B. Q. Chi;Q. Jiang
Advanced Engineering Materials 2005 Volume 7(Issue 6) pp:
Publication Date(Web):1 JUL 2005
DOI:10.1002/adem.200400158
Co-reporter:J.C. Li, W. Liu, Q. Jiang
Materials Letters 2005 Volume 59(14–15) pp:1907-1909
Publication Date(Web):June 2005
DOI:10.1016/j.matlet.2005.02.008
According to known analytical models for surface stress f and surface energy γ, f and γ of some metals have been calculated. In terms of the calculations, the reconstruction possibility associated with the quantity of (f−γ) for (111) facet of nine fcc metals is predicted. The results are in agreement with other theoretical and the experimental results.
Co-reporter:X.Y. Lang, Q. Jiang
Solid State Communications 2005 Volume 134(Issue 12) pp:797-801
Publication Date(Web):June 2005
DOI:10.1016/j.ssc.2005.03.039
A simple and unified model is developed for finite size effect on the critical transition temperature of superconductive nanosolids, which is based on the size-dependent Debye temperature of crystals within the McMillan expression. In the model, two material and structure dependent parameters of D0 and α are used, which, respectively, are the critical size at which all atoms of a low-dimensional material are located on its surface, and the ratio of the mean square vibrational amplitude between surface atoms and interior atoms, In light of this model, the critical transition temperatures of superconductive nanosolids can decrease or increase with the dropping size of nanosolids depending on the bond strength changes of interfacial atoms. The predicated results are consistent with the available experimental results for superconductors MgB2 and Nb thin films, Bi and Pb granular thin films and nanoparticles, Al thin films and nanoparticles.
Co-reporter:X.F. Cui, M. Zhao, Q. Jiang
Thin Solid Films 2005 Volume 472(1–2) pp:328-333
Publication Date(Web):24 January 2005
DOI:10.1016/j.tsf.2004.07.063
Through extending a model for size-dependent glass transition temperature (Tg), the size-dependent Curie temperature of low-dimensional ferromagnetic metals (particles, wires and thin films) with different morphologies in full size range (Tc) is modeled. Based on energetic and thermodynamic approaches, the critical size and morphology of the metals are considered. It is found that Tc drops as size decreases, which corresponds to the experimental results of Ni particles and wires, as well as Fe, Co and Ni thin films.
Co-reporter:Qing Jiang;Xing You Lang
Macromolecular Rapid Communications 2004 Volume 25(Issue 7) pp:825-828
Publication Date(Web):23 MAR 2004
DOI:10.1002/marc.200300274
Summary: A unified model is developed for the finite size-effect on the glass-transition temperature of polymers, Tg(D), where D denotes the diameter of particles or thickness of films. In terms of this model, Tg depends on both the size and interface conditions. The predicted results are consistent with the experimental evidence for polystyrene (PS) particles and films with different interface situations.
Co-reporter:Z.K. Zhao;J.C. Li;Q. Jiang
Advanced Engineering Materials 2004 Volume 6(Issue 5) pp:
Publication Date(Web):24 MAY 2004
DOI:10.1002/adem.200300578
Co-reporter:Z.P. Chen, Z. Wen, Q. Jiang
Solid State Communications 2004 Volume 132(Issue 11) pp:747-750
Publication Date(Web):December 2004
DOI:10.1016/j.ssc.2004.09.061
A model for the equilibrium transition size and temperature between hcp and fcc structure of nanocrystals Ti has been established in terms of the effect of surface stress on the internal pressure of nanocrystals. It was found that as size and temperature decreased, the relative stability of fcc structure in comparison with hcp structure increased. The obtained result is consistent with other theoretical and experimental data.
Co-reporter:M. Zhao, Q. Jiang
Solid State Communications 2004 Volume 130(1–2) pp:37-39
Publication Date(Web):April 2004
DOI:10.1016/j.ssc.2004.01.016
Undercooling, superheating, surface melting temperatures and melting enthalpies of low-dimensional In crystals are predicted by a unified model. A good agreement between the model predictions and experimental results are found.
Co-reporter:C.C. Yang, J.C. Li, Q. Jiang
Solid State Communications 2004 Volume 129(Issue 7) pp:437-441
Publication Date(Web):February 2004
DOI:10.1016/j.ssc.2003.11.020
The temperature–pressure phase diagram [T–P] for silicon (Si) is predicted through the Clapeyron equation where the pressure-dependent volume difference is modeled and the corresponding thermodynamic amount of solid transition enthalpy is calculated by introducing the effect of surface stress induced pressure. The model prediction is found to be consistent with the present experimental results and other theoretical predictions.
Co-reporter:Q. Jiang, H.M. Lu, M. Zhao
Scripta Materialia 2003 Volume 49(Issue 6) pp:547-550
Publication Date(Web):September 2003
DOI:10.1016/S1359-6462(03)00355-5
Interface stress and interface free energy models are introduced into phase equilibrium conditions of a binary phase diagram. The existence of the interface stress leads to shifts of the Gibbs free energy curve of a second compressible phase upwards and rightwards in comparison with that of the corresponding incompressible phase.
Co-reporter:Q Jiang, S Zhang, M Zhao
Materials Chemistry and Physics 2003 Volume 82(Issue 1) pp:225-227
Publication Date(Web):28 September 2003
DOI:10.1016/S0254-0584(03)00201-3
A simple model, without any free parameter, is introduced to predict the size-dependent melting temperature of noble metals in this contribution. It is found that the model predictions for the melting point depression of both Au and Ag nanoparticles correspond to the experimental and computer simulation results well.
Co-reporter:H.M. Lu;W.X. Zhang;Q. Jiang
Advanced Engineering Materials 2003 Volume 5(Issue 11) pp:
Publication Date(Web):2 DEC 2003
DOI:10.1002/adem.200300359
Co-reporter:J.C. Li;Z.K. Zhao;Q. Jiang
Advanced Engineering Materials 2003 Volume 5(Issue 3) pp:
Publication Date(Web):18 MAR 2003
DOI:10.1002/adem.200390017
Co-reporter:Qing Jiang;Chun Cheng Yang;Jian Chen Li
Macromolecular Theory and Simulations 2003 Volume 12(Issue 1) pp:57-60
Publication Date(Web):13 MAR 2003
DOI:10.1002/mats.200390003
A general model for all kinds of size-dependent melting points, free of any adjustable parameter, is extended to illustrate the size-dependence of the melting temperature of polyethylene (PE). The model prediction for the depression of the melting temperature of PE is consistent with the calorimetric experimental results as shown in the Figure where the melting temperature of lamellae PE crystals as a function of the thickness of the crystals is presented.
Co-reporter:Z Wen, M Zhao, Q Jiang
Materials Letters 2003 Volume 57(16–17) pp:2515-2518
Publication Date(Web):May 2003
DOI:10.1016/S0167-577X(02)01303-4
Surface melting of polycrystals Pb and In within 1 K below the melting temperature is measured and interpreted based on our model for size dependence of melting temperature. It found that the thickness of liquid skin on the surface of the polycrystals below the melting temperature is dependent on temperature.
Co-reporter:Q. Jiang, L.H. Liang, J.C. Li
Vacuum 2003 Volume 72(Issue 3) pp:249-255
Publication Date(Web):24 November 2003
DOI:10.1016/S0042-207X(03)00148-9
A simple model for size-dependent melting temperature and melting entropy of nanocrystals embedded in a matrix is introduced to interpret the superheating phenomenon. The model predicts not only melting temperature and the melting entropy increase for embedded nanocrystals as the size of the nanocrystals decreases, but also melting temperature and the melting entropy depression for free-standing nanocrystals with reducing size. The model is supported by available experimental results of nanoparticles and thin films.
Co-reporter:J.C. Li, Z.K. Zhao, Q. Jiang
Materials Research Bulletin 2002 Volume 37(Issue 2) pp:297-304
Publication Date(Web):1 February 2002
DOI:10.1016/S0025-5408(01)00783-8
Using hot pressing powder metallurgy technique, high strength bulk Al85La10Ni5 alloy in a size of ∅ mm with porosity of less than 3% has been obtained when the hot pressing temperatures are 753–773 K, pressing time is 30 min and pressure is 1.2 GPa. The highest compression strength of 950 MPa of the alloy after the hot pressing at 773 K have been obtained. The strength increasing of the alloy is interpreted by second-phase strengthening and fine-grain strengthening.
Co-reporter:L.H Liang, J.C Li, Q Jiang
Solid State Communications 2002 Volume 121(Issue 8) pp:453-455
Publication Date(Web):1 March 2002
DOI:10.1016/S0038-1098(02)00026-1
A model for size-dependent elastic modulus of Cu and Au thin films is established based on consideration of size-dependent atomic distance and bond energy. The predictions of the model for the enhancement of the elastic modulus of Cu and Au thin films correspond to the results of computer simulations well.
Co-reporter:Mei Xia Xiao, Yong Fu Zhu, Qing Jiang
Solid State Communications (February 2012) Volume 152(Issue 3) pp:210-214
Publication Date(Web):1 February 2012
DOI:10.1016/j.ssc.2011.11.006
The atomic structures of α-Al2O3-coated Cu films doped with different concentrations of Al under external electric field F are investigated using density-functional theory. As F reaches 0.040 au (1 au=51.4 V/Å), large deformation is observed for pure Cu films, indicating the occurrence of electromigration (EM) in the Cu slabs. Under the same or even larger F, in contrast, almost no deformation occurs for the α-Al2O3-coated Cu(Al) films, except that a slight change is found at the Cu(Al)/α-Al2O3 interfaces. The main reason for this stability should be attributed to the existence of Cu–O covalent–ionic and Al–O ionic bonds at the interface, suggesting that the EM reliability of Cu atoms can be effectively improved by the strong bonding strength.Highlights► We investigate the changes of four atomic structures under external electric fields. ► The Cu films undergo large deformation, indicating that electromigration occurs, as F reaches 0.040 au (1 au = 51.4 V/Å). ► The Cu(Al) films at Cu(Al)/-Al2O3 interfaces change slightly under the same and larger F. ► Cu–O covalent–ionic and Al–O ionic bonds exist at the Cu(Al)/-Al2O3 interfaces. ► The stronger bonding strength effectively improves the EM reliability of Cu atoms.
Co-reporter:B. B. Xiao, X. B. Jiang, X. L. Yang, Q. Jiang and F. Zheng
Physical Chemistry Chemical Physics 2016 - vol. 18(Issue 43) pp:NaN30182-30182
Publication Date(Web):2016/10/10
DOI:10.1039/C6CP05869H
Pt1ML/Pd3Al, which comprises a Pd3Al core protected by a Pt monolayer, may experience Al dealloying because of the strong affinity of Al toward O. To circumvent this issue, the Pt2ML/Os/Pd3Al catalyst has been designed to suppress the migration of Al by inserting an Os monolayer at the interface between the Pd3Al core and two Pt monolayers. On the basis of segregation energies, Al leaching from the core to the 1st layer is determined to be endothermic even under O coverage, indicating an energetic preference for Al to reside in the core structure. The Pt2ML/Os/Pd3Al catalyst benefits from the energetic disadvantage of the inward movement of Os and the presence of the 2 ML Pt layer. As an ORR electrocatalyst, the relatively weak adsorption ability of Pt2ML/Os/Pd3Al suggests improved ORR activity. Finally, a representative OOH association mechanism with low reaction barriers of 0.46, 0.31, 0.38 and 0.41 eV for the OOH formation, OOH dissociation, OH formation and H2O formation steps suggests that the catalyst can effectively activate the O–O bond and eliminate OH, which can act as a catalytic poison. These findings suggest the design of stable sandwich catalysts as potential candidates for ORR electrocatalysis.
Co-reporter:Cang Lang Yao, Jian Chen Li, Wang Gao and Qing Jiang
Physical Chemistry Chemical Physics 2017 - vol. 19(Issue 23) pp:NaN15072-15072
Publication Date(Web):2017/05/15
DOI:10.1039/C7CP01881A
The urgent need for artificially fixing CO2 calls for catalysts of high efficiency. The transition metal functionalized porphyrin (TMP) is one of the most important types of organic catalysts for CO2 reduction. However, the catalytic mechanisms of TMP in CO2 reduction still remain controversial. Starting from the previously neglected catalyst self-protonation model, we uncover a new CO2 reduction mechanism on cobalt-porphine, which involves an indirect proton transfer step occurring at the beginning of the reduction cycle. Based on this protonation mechanism, we demonstrate the different correlations between producing rate and pH for the formation of CO and methane, in good agreement with available experimental observations. Our results reveal how pH and potential affect the CO2 reduction process, providing important clues and insights for further optimization of TMP catalysts.
Co-reporter:W. Liu, Y. H. Zhao, Y. Li, E. J. Lavernia and Q. Jiang
Physical Chemistry Chemical Physics 2009 - vol. 11(Issue 40) pp:NaN9240-9240
Publication Date(Web):2009/08/17
DOI:10.1039/B907591G
Implementation of hydrogen storage systems requires moderate bonding strength. However, this goal has remained a challenge, either due to the weak physisorption or extremely strong chemisorption. Here, we report on a new phenomenon, namely that H2 binding can be externally enhanced (or weakened) via superimposition of a positive (or negative) electric field. We demonstrate this concept using an 8-Li-doped carbon nanotube. The calculated adsorption energy Ead = −0.58 eV/H2 under F = +0.010 au is 93.33% lower than that under 0.000 au (F indicates the field intensity). This is because the positive field produces an extra dipole moment. In contrast, Ead increases from −0.30 to −0.20 eV/H2 when F = −0.010 au. In view of the fact that storage systems are insensitive to small unexpected field fluctuations, the application of the electric field as a reversible switch makes practical sense.
Co-reporter:Chun Cheng Yang, Chang Chun Wang, Miao Miao Li and Qing Jiang
Journal of Materials Chemistry A 2017 - vol. 5(Issue 3) pp:NaN1152-1152
Publication Date(Web):2016/12/08
DOI:10.1039/C6TA09736G
Nickel metal hydride (Ni-MH) batteries have demonstrated key technology advantages for applications in new-energy vehicles, while the main challenge derives from the insufficient cycle lives (about 500 cycles) of their negative electrode materials—hydrogen storage alloys. As a result, progress in their development has been very limited over the past decades. Here we propose a theoretical framework to design a series of long-life and low-cost hydrogen storage alloys, by considering the electronegativities of the elements to enhance the alloys' corrosion resistance. Two novel candidate alloys, La0.6Ce0.3Y0.1Ni3.7Co0.75Mn0.3Al0.35 and La0.55Ce0.3Y0.15Ni3.7Co0.75Mn0.3Al0.35, show ultra-long cycle lives of 1325 and 1407 cycles, respectively, which are almost triple that of the commercial alloy (MmNi3.55Co0.75Mn0.4Al0.3) that is used in Ni-MH batteries. The usage costs of Ni-MH batteries based on these two alloys are only 1/4 of that of the lithium-ion battery, showing better market prospects for large-scale applications.
Co-reporter:Yong-Fu Zhu, Ning Zhao, Bo Jin, Ming Zhao and Qing Jiang
Physical Chemistry Chemical Physics 2017 - vol. 19(Issue 13) pp:NaN9260-9260
Publication Date(Web):2017/03/10
DOI:10.1039/C6CP08061H
Nanoscale core/shell structures are of interest in catalysis due to their superior catalytic properties. Here we investigated the thermal stability of the coherent core–shell structures in a thermodynamic way by considering the impact from the core with the bulk melting point Tm(∞) lower or higher than the shell. When a low-Tm(∞) core is adopted, core–shell melting induced by the melting depression of the core does not occur upon heating because of the superheating, although the melting depression of the core can be triggered ultimately by the preferential melting of the high-Tm(∞) shell for small cores. The superheating of the core is contributed by the negative solid–solid interface energy, while the depression is originated from the positive solid–liquid interface energy. Owing to the presence of the negative interface energy, moreover, the low-Tm(∞)-core structure possesses a low difference in thermal expansion between the core and the shell, high activation energy of outward atomic diffusion from the core to shell, and low heat capacity. This result is beneficial for the core–shell structure design for its application in catalysis.
Co-reporter:N. Gao, Y. F. Zhu and Q. Jiang
Journal of Materials Chemistry A 2017 - vol. 5(Issue 29) pp:NaN7290-7290
Publication Date(Web):2017/06/23
DOI:10.1039/C7TC01972F
Arsenene-based device applications such as transistors and photodetectors benefit from precise control over the carrier type and concentration as well as a combination of both high-quality p-doped and n-doped components to form p–n junctions. Here, it is demonstrated using first-principles calculations that selective organic molecular adsorption allows us to effectively control the carrier type in arsenene. Moreover, upon applying an in-plane tensile strain, the carrier concentration effectively increases. Furthermore, the BN substrate can increase the structural stability without any impact on the doping character of the arsenene sheet. This opens the possibility of creating arsenene p–n junctions.
Co-reporter:N. Gao, G. Y. Lu, Z. Wen and Q. Jiang
Journal of Materials Chemistry A 2017 - vol. 5(Issue 3) pp:NaN633-633
Publication Date(Web):2016/12/14
DOI:10.1039/C6TC04943E
The potential of silicene-based integrated electronics originates from its extremely high carrier mobility, whereas the lack of a band gap impedes its application. Thus, opening a sizeable band gap without degrading its carrier mobility is a significant challenge for application in logic circuits. In this study, a sizable band gap is created in silicene by the dual effect of organic molecule adsorption and a substrate. As an electron donor molecule, tetrathiafulvalene (TTF) is found to non-covalently functionalize the silicene sheet. As a result, silicene with adsorbed TTF exhibits an open band gap. When silicane (hydrogenated silicene) substrate is applied, the band gap further widens. Moreover, the high carrier mobility is largely retained. These results provide effective and reversible routes for engineering the band gap of silicene.
Co-reporter:Chao Hou, Xiang-Mei Shi, Chen-Xu Zhao, Xing-You Lang, Lin-Lin Zhao, Zi Wen, Yong-Fu Zhu, Ming Zhao, Jian-Chen Li and Qing Jiang
Journal of Materials Chemistry A 2014 - vol. 2(Issue 37) pp:NaN15526-15526
Publication Date(Web):2014/07/25
DOI:10.1039/C4TA02604G
Nanostructured SnO2 is an attractive anode material for high-energy-density lithium-ion batteries because of the fourfold higher theoretical charge capacity than commercially used graphite. However, the poor capacity retention at high rates and long-term cycling have intrinsically limited applications of nanostructured SnO2 anodes due to large polarization and ∼300% volume change upon lithium insertion/extraction. Here we report the design of a SnO2-based anode, which is constructed by embedding SnO2 nanoparticles into a seamlessly integrated 3D nanoporous/solid copper current collector (S/NP Cu/SnO2), with an aim at tackling both problems for the high-performance reversible lithium storage. As a result of the unique hybrid architecture that enhances electron transfer and rapid access of the lithium ion into the particle bulk, the S/NP Cu/SnO2 anode can store charge with a capacity density as high as ∼3695 mA h cm−3 and an exceptional rate capability. Even when the discharge rate is increased by a factor of 160 (12 A g−1), it still retains ∼1178 mA h cm−3, one order of magnitude higher than that of a traditional SnO2-based electrode (∼111.6 mA h cm−3), which is assembled by mixing SnO2 nanoparticles with conductive carbon black and a polymeric binder and coating on flat Cu foil. In addition, not only do the rigid Cu skeleton and the stable Cu/SnO2 interface improve the microstructural stability, but also the pore channels accommodate the large SnO2 volume changes, enlisting the S/NP Cu/SnO2 anode to exhibit high specific capacity over 1000 cycles at a high rate.
Co-reporter:Jun-Min Yan, Zhi-Li Wang, Hong-Li Wang and Qing Jiang
Journal of Materials Chemistry A 2012 - vol. 22(Issue 22) pp:NaN10993-10993
Publication Date(Web):2012/03/29
DOI:10.1039/C2JM31042B
A general and energy-efficient strategy has been successfully applied for synthesis of a graphene–CuCo nanohybrid, which leads to the highest catalytic activity of Cu-based catalysts up to now toward the dehydrogenation of ammonia borane, and also the excellent activity for electrochemical hydrogen evolution reaction. Moreover, this general method can be easily extended to facile preparation of other graphene–metal systems.
Co-reporter:B. B. Xiao, X. B. Jiang and Q. Jiang
Physical Chemistry Chemical Physics 2016 - vol. 18(Issue 21) pp:NaN14243-14243
Publication Date(Web):2016/04/20
DOI:10.1039/C6CP01066K
Developing efficient catalysts for the oxygen reduction reaction (ORR) to reduce cathode Pt loading without sacrificing the performance has been under intensive research. Herein, by using density functional theory calculations, the activity and stability of a Pt monolayer supported on Pd3Al(111) as the ORR catalyst have been systematically studied. The simulations demonstrate that due to alloying, the ORR intermediates bind weakly on Pt/Pd3Al(111) with optimal adsorption energy of O and OH. By considering the elemental ORR steps, the ORR mechanism is predicted to be an OOH dissociation mechanism. The rate determining step is OOH dissociation with a reaction barrier of 0.37 eV, lower than the corresponding value on Pt/Pt3Al(111) and Pt(111), indicating the superior activity of Pt/Pd3Al(111). Even considering the unfeasible H adsorption under high potential, the ORR mechanism on Pt/Pd3Al(111) would proceed via O2 hydration, OOH hydration, H2O formation, and H2O desorption, indicating a good ORR electrocatalyst. Furthermore, stability was evaluated by calculating the alloy formation energy and the electrochemical potential shift of surface Pt dissolution. The exceptionally negative alloy formation energy of Pd3Al and the positive dissolution potential shift of the surface Pt atoms show the enhanced durability of Pt/Pd3Al(111). The improved activity, in combination with its enhanced stability, makes the novel ternary alloy electrocatalyst very promising for development of new cathode catalysts for fuel cells.
Co-reporter:Y. F. Zhu, Q. Q. Dai, W. T. Zheng and Q. Jiang
Physical Chemistry Chemical Physics 2014 - vol. 16(Issue 12) pp:NaN5604-5604
Publication Date(Web):2014/02/11
DOI:10.1039/C3CP55222E
Based on the size-dependent cohesive energy formula for two-dimensional materials, we investigate the gap openings in graphene layers regarding distinct interfacial interaction from substrates. Depending on the interfacial physicochemical nature, the gap is opened weakly induced by the van der Waals interaction but readily by the chemical bonding. Relative to the former, in essence, the distinct opening behavior for the latter comes from the substantial change in atomic cohesive energy of graphene associated with the coordination imperfection. Our predictions agree with the available experimental or computer simulation results for graphene layers on layered BN or bulk truncated SiC. The present work is of benefit for the application of graphene in electronics.
Co-reporter:N. Gao, J. C. Li and Q. Jiang
Physical Chemistry Chemical Physics 2014 - vol. 16(Issue 23) pp:NaN11678-11678
Publication Date(Web):2014/03/24
DOI:10.1039/C4CP00089G
The geometric and electronic properties of silicene paired with a MoS2 substrate are studied systematically by using density functional theory with van der Waals corrections. It is found that the nearly linear band dispersions can be preserved in the heterobilayers due to the weak interface interactions. Meanwhile, the band gap is opened because of the sublattice symmetry broken by the intrinsic interface dipole. Moreover, the band gap values could be effectively modulated under an external electric field. Therefore, a way is paved for silicene–MoS2 heterobilayers to be candidate materials for logic circuits and photonic devices.
Co-reporter:Z. M. Ao, S. Li and Q. Jiang
Physical Chemistry Chemical Physics 2009 - vol. 11(Issue 11) pp:NaN1687-1687
Publication Date(Web):2009/01/29
DOI:10.1039/B812188E
The thermal stability of interaction between CO molecules and Al doped graphene is studied using ab initio molecular dynamics calculations to reveal the adsorption/desorption behavior of the system. With these results, an adsorption–desorption phase diagram was established with atomic thermodynamics. The temperature (T) dependent desorption time τ(T) was determined with a thermal desorption method. The results show that the optimal desorption temperature is 400 K. The effect of T on atomic structure parameters and electrical properties were analyzed. It shows that the maximum variation of electrical conductivity induced by the adsorption occurs at 400 K, indicating that the best sensing performance of the devices should be at this particular temperature.
Co-reporter:Y. F. Zhu, W. T. Zheng and Q. Jiang
Physical Chemistry Chemical Physics 2011 - vol. 13(Issue 48) pp:NaN21332-21332
Publication Date(Web):2011/10/31
DOI:10.1039/C1CP22748C
Young's modulus (Y) of nanostructured materials (NSs) free of porosity is modeled with regard to the coordination number imperfection at grain boundaries. In light of it, Y of NSs is suppressed substantially in the whole solid temperature range, differing from the case of nanocrystals (NCs) where Y is enhanced at lower temperature (T) but weakened at higher T. It is found that, similar to NCs, the thermally-driven decline associated with the melting point depression plays an increasing role in suppressing Y of NSs on raising T. On the other hand, the lattice expansion and the bond weakening lead to a further suppression in Y of NSs independent of T, while the lattice contraction and the reinforced bonding strength result in an enhancement in Y of NCs, which should be responsible for the distinction in Y between NSs and NCs. The established functions were supported by available experimental and computer simulation results.
Co-reporter:Grégory Guisbiers, Di Liu, Qing Jiang and Lionel Buchaillot
Physical Chemistry Chemical Physics 2010 - vol. 12(Issue 26) pp:NaN7210-7210
Publication Date(Web):2010/05/19
DOI:10.1039/C002496A
In this paper, top-down and bottom-up approaches are used to predict material properties of group III-nitride nanostructures. The first approach calculates the melting temperature, melting enthalpy, Debye temperature and energy bandgap of InN, GaN and AlN through classical thermodynamics. The second approach calculates the surface energies in the liquid and solid states of the considered nitrides materials through molecular dynamics. Moreover, the liquid and solid surface energies of the zinc-blende and wurtzite III–V materials are compared. Finally, the phase diagram of a ternary III-nitride nanomaterial, AlGaN, is presented and the variation of its energy bandgap with composition is predicted.
Co-reporter:Z. W. Zhang, W. T. Zheng and Q. Jiang
Physical Chemistry Chemical Physics 2011 - vol. 13(Issue 20) pp:NaN9489-9489
Publication Date(Web):2011/04/12
DOI:10.1039/C0CP02917C
The adsorption of H2 on Ce doped single-walled carbon nanotubes (SWCNT) and graphene are investigated by using density functional theory. For both systems, it is found that Ce preferentially occupies the hollow site on the outside. The results indicate that Ce/SWCNT system is a good candidate for hydrogen storage where six H2 per Ce can be adsorbed and 5.14 wt% H2 can be stored in the Ce3/SWCNT system. Among metal-doped SWCNTs, Ce exhibits the most favorable hydrogen adsorption characteristics in terms of the adsorption energy and the uptake capacity. The hybridization of the Ce-4f and Ce-5d orbitals with the H orbital contributes to the H2 binding where Ce-4f electrons participate in the hybridization due to the instability of the 4f state. The interaction between H2 and Ce/SWCNT is balanced by the electronic hybridization and electrostatic interactions. Curvature of SWCNT changes the size of the binding energy of Ce and C and the adsorption energy of H2 on Ce.
Co-reporter:P. Zhang, J. S. Lian and Q. Jiang
Physical Chemistry Chemical Physics 2012 - vol. 14(Issue 33) pp:NaN11723-11723
Publication Date(Web):2012/07/09
DOI:10.1039/C2CP40087A
Nitrogen-doped carbon nanotubes (NCNTs) are attractive for electrocatalytic applications in fuel cells due to their low cost and high electrocatalytic activity. By using density functional theory calculations, the electrocatalytic mechanisms of the oxygen reduction reaction (ORR) under electrochemical conditions are studied at graphite-like N groups (NG) and pyridine-like N groups (NP) of NCNTs, in which the effect of electrode potentials on the activation energy (Ea) and reaction energy (Er) is taken into account. The ORR occurs at both NG and NP defect sites via two different four-electron OOH and two-electron H2O2 mechanisms. At the lower potential region, both mechanisms are simultaneously responsible for the reaction at NG and NP defect sites; while at higher potentials, the four-electron mechanism becomes dominant and the ORR at NP defect sites is more energetically favorable than that at NG defect sites.
Co-reporter:Q. Q. Dai, Y. F. Zhu and Q. Jiang
Physical Chemistry Chemical Physics 2012 - vol. 14(Issue 3) pp:NaN1261-1261
Publication Date(Web):2011/12/01
DOI:10.1039/C1CP22866H
Stability, electronic and magnetic properties of triangular graphene nanoflakes embedded in graphane (graphane-embedded TGNFs) are investigated by density functional theory. It is found that the interface between the embedded TGNF and graphane is stable since the diffusion of H atoms from the graphane region to the embedded TGNF is energetically unfavorable with high energy barriers. The electronic and magnetic properties of the system completely depend on the embedded TGNF. The band gaps of graphane-embedded ATGNFs (armchair-edged TGNFs) arise due to the quantum confinement, while the special characteristics of nonbonding states of graphane-embedded ZTGNFs (zigzag-edged TGNFs) play an important role in their electronic properties. As the edge sizes increase, the differences of band gaps between graphane-embedded TGNFs and the isolated ones decrease. Furthermore, owing to the partially paired pz orbitals of edge C atoms, graphane-embedded ZTGNFs exhibit a ferrimagnetic ground state with size-dependant total spin being consistent with Lieb's theorem. Our work provides a possible way to obtain TGNFs without physical cutting.
Co-reporter:Nan Gao, Wei Tao Zheng and Qing Jiang
Physical Chemistry Chemical Physics 2012 - vol. 14(Issue 1) pp:NaN261-261
Publication Date(Web):2011/11/14
DOI:10.1039/C1CP22719J
The electronic structures and band gaps of silicene (the Si analogue of graphene) adsorbed with halogen elements are studied using the density functional theory based screened exchange local density approximation method. It is found that the band gaps of silicene adsorbed with F, Cl, Br and I have a nonmonotonic change as the periodic number of the halogen elements increases. This is attributed to the transfer of contributions to band gaps from Si–Si bonding to Si–halogen bonding.
Co-reporter:Q. G. Jiang, Z. M. Ao, W. T. Zheng, S. Li and Q. Jiang
Physical Chemistry Chemical Physics 2013 - vol. 15(Issue 48) pp:NaN21022-21022
Publication Date(Web):2013/10/07
DOI:10.1039/C3CP52976B
To facilitate the dissociative adsorption of H2 molecules on pristine graphene, the addition of a mono-atom-vacancy to graphene is proposed. This leads to reduction of the dissociative energy barrier for a H2 molecule on graphene from 3.097 to 0.805 eV for the first H2 and 0.869 eV for the second, according to first principles calculations. As a result, two H2 molecules can be easily dissociatively adsorbed on this defected graphene at room temperature. The electronic structure and conductivity of the graphene change significantly after H2 adsorption. In addition, the related dissociative adsorption phase diagrams under different temperatures and partial pressures show that this dissociative adsorption at room temperature is very sensitive (10−35 mol L−1). Therefore, this defected graphene is promising for ultra-sensitive room temperature hydrogen sensing.
Co-reporter:Q. G. Jiang, Z. M. Ao and Q. Jiang
Physical Chemistry Chemical Physics 2013 - vol. 15(Issue 26) pp:NaN10865-10865
Publication Date(Web):2013/04/23
DOI:10.1039/C3CP00128H
The effect of the Al dopant on the dissociative adsorption of a H2O molecule on graphene is investigated using first principles calculations. It is found that doping Al into graphene can facilitate the dissociative adsorption of H2O molecules. The dissociative energy barrier is reduced from 3.609 eV on pristine graphene to 0.456 eV on Al-doped graphene and the reaction releases an energy of 0.413 eV, which indicates a smooth dissociative adsorption on Al-doped graphene at room temperature. In addition, the dissociative adsorption of H2O molecules can convert the Al-doped graphene from hydrophobic to hydrophilic while obtaining conductive graphene with doping concentration higher than 5.56%. This hydrophilic and conductive graphene has potential applications in supercapacitors and biomaterial supports.
Co-reporter:Q. Q. Dai, Y. F. Zhu and Q. Jiang
Physical Chemistry Chemical Physics 2014 - vol. 16(Issue 22) pp:NaN10613-10613
Publication Date(Web):2014/03/31
DOI:10.1039/C4CP00868E
Grain boundaries (GBs) that inevitably appear in CVD-grown graphene affect the electronic properties of graphene-based nanomaterials. In this paper, we introduce 558 GB (composed of a pair of pentagons and one octagon alternately) into armchair graphene nanoribbons (AGNRs) and divide them into three groups in light of the end configurations of 558 GB at the ribbon edges. By using first-principles calculations, the variations of electronic and magnetic properties with two adjustable parameters W (ribbon widths) and NZ (the distances between 558 GBs) are systematically investigated for each group. The results show that different electronic and magnetic behaviors versus W and NZ are presented for varying end configurations of 558 GB, including nonmagnetic metals, ferromagnetic metals and nonmagnetic semiconductors. By introducing 558 GB into AGNRs, the impurity states that are completely contributed by 558 GB appear around the Fermi level. Furthermore, a ferromagnetic ordering on the two zigzag chains of 558 GB occurs for the ferromagnetic metals due to the spin splitting energy bands near the Fermi level. These unique electronic and magnetic properties of AGNRs with 558 GB would find their potential applications in electronic and spintronic devices.
Co-reporter:Hong-Ying Fu, Xing-You Lang, Chao Hou, Zi Wen, Yong-Fu Zhu, Ming Zhao, Jian-Chen Li, Wei-Tao Zheng, Yong-Bing Liu and Qing Jiang
Journal of Materials Chemistry A 2014 - vol. 2(Issue 35) pp:NaN7222-7222
Publication Date(Web):2014/07/08
DOI:10.1039/C4TC00603H
There is a strong interest in plasmonic nanostructures that uniformly enhance Raman signals of chemical and biological molecules using surface-enhanced Raman spectroscopy (SERS) for trace detection. Although the resonant excitation of localized surface plasmons of single or assembled metallic nanoparticles can generate large electromagnetic fields, their SERS effects suffer from poor reproducibility and uniformity, limiting their highly reliable and stable applications. Here, we report self-supported large-scale nanoporous hybrid films with high density and uniform hot spots, produced by the implantation of SnO nanoparticles into nanoporous Au/Ag bimetallic films (NP Au/SnO/Ag) for the trace detections of both resonant and non-resonant molecules. The NP Au/SnO/Ag films exhibit extraordinary SERS enhancements, which increase with the increasing density of Au/SnO/Ag sandwich protrusions, as a result of the formation of abundant and uniform hot spots. The nanogaps in their wrinkled films further improve the capability to detect molecules at single molecular levels, making the hybrid films promising SERS-active substrates with superior reproducibility and reliability for applications in life science and environment protection.
Co-reporter:Chao Hou, Xing-You Lang, Zi Wen, Yong-Fu Zhu, Ming Zhao, Jian-Chen Li, Wei-Tao Zheng, Jian-She Lian and Qing Jiang
Journal of Materials Chemistry A 2015 - vol. 3(Issue 46) pp:NaN23419-23419
Publication Date(Web):2015/10/14
DOI:10.1039/C5TA05335H
Transition-metal hydroxides (TMHOs) or oxides (TMOs) with layered crystalline structures are attractive electrode materials for high-density charge storage in electrochemical supercapacitors. However, their randomly stacked nanostructures on conductive reinforcements, typically carbon materials, exhibit only modest enhancement of rate capability because of poor electron and ion transports that are limited by highly anisotropic conductivity, excessive grain boundaries and weak TMHO or TMO/C interfaces. Here we report a hybrid electrode design to tackle all three of these problems in layered Ni(OH)2 for high-performance asymmetric supercapacitors, wherein the single-crystalline Ni(OH)2 nanosheets are vertically aligned on a three-dimensional bicontinuous nanoporous gold skeleton with epitaxial Au/Ni(OH)2 interfaces (NP Au/VA Ni(OH)2). As a result of the unique nanoarchitecture, the pseudocapacitive behavior of Ni(OH)2 is dramatically enhanced for ensuring a volumetric capacitance as high as ∼2911 F cm−3 (∼2416 F g−1 for the constituent Ni(OH)2) in the NP Au/VA Ni(OH)2 electrode with excellent rate capability. Asymmetric supercapacitors assembled with this NP Au/VA Ni(OH)2 electrode and activated carbon have a high gravimetric energy of 31.4 W h kg−1 delivered at an exceptionally high power density of 100 kW kg−1 with excellent cycling stability.
Co-reporter:Tonghui Wang, Yongfu Zhu and Qing Jiang
Chemical Science (2010-Present) 2012 - vol. 3(Issue 2) pp:NaN536-536
Publication Date(Web):2011/10/13
DOI:10.1039/C1SC00681A
The device performance of organic field-effect transistors depends strongly on the morphology and molecular orientation of the first few molecular layers near gate dielectrics, which are in turn governed by the initial growth stage. In this work, we establish a unified thermodynamic model to characterize the initial growth stage of disk-like and rod-like organic molecules during an organic vapor deposition process. Under a high substrate temperature and low deposition rate, the initially grown parallel cluster can transfer to the normal one at a critical molecular number Nc, which is determined by the competition between the surface energy of the molecule γf (surface energy of the molecular surface normal to the π–π interaction direction for a disk-like molecule or parallel to the molecular axis for a rod-like molecule) and that of the substrate γsub. By thermodynamic analyses and molecular dynamics simulations, we further confirm this transformation from disk-like phthalocyanine. When N < Nc, a parallel cluster is grown by self-assembly of individual lying down molecules driven by γf. At N ≥ Nc, together with γf > (5/7)γsub, the grown parallel cluster tilts down to form a normal one where Nc ≈ γfW/γlH (γl is the surface energy of the molecular surface parallel to the π–π interaction direction. W and H denote the molecular width and the intermolecular distance in the π–π interaction direction).