Hong-liang Xu

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Organization: Northeast Normal University
Department: Institute of Functional Material Chemistry, Faculty of Chemistry
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Co-reporter:Feng-Wei Gao, Rong-Lin Zhong, Hong-Liang Xu, and Zhong-Min Su
The Journal of Physical Chemistry C November 16, 2017 Volume 121(Issue 45) pp:25472-25472
Publication Date(Web):October 30, 2017
DOI:10.1021/acs.jpcc.7b08172
Based on s-indaceno[1,2,3-cd;5,6,7-c′d′]diphenalene (1) consisting of two phenalenyl moieties, the monomer 2 and its dimer 22 are designed by boron and nitrogen atoms substituting the central carbon atoms of phenalenyl moieties. Calculated energy decompose analysis (EDA) shows that the orbital interaction for 22 possesses a large attractive contribution of −18.31 kcal mol–1, which is dominated by the π–π stacking interaction between the upper and the lower π-conjugated units. Interestingly, the natural population analysis (NPA) charge and the transition density matrix (TDM) show that both intramolecular charge transfer and intermolecular charge transfer (CT) exist in 22. Further, the first hyperpolarizability (βtot = 4.56 × 104 au) of 2 with intramolecular CT is greatly larger than that of reported molecule 3 (5.45 × 103 au) with intermolecular CT. Significantly, 22 exhibits the largest βtot value to be 1.42 × 105 au, which is caused by combining the intra- and intermolecular CT transitions (βx = 1.40 × 105 au and βz = 2.27 × 104 au). Correspondingly, highest occupied molecular orbital (HOMO) → lowest unoccupied molecular orbital (LUMO) (intramolecular CT) in the low-energy electronic transition of 22 is 68%, while HOMO → LUMO + 1 (intermolecular CT) is 18%, which demonstrates that the intramolecular CT effect on the βtot value is stronger than the case of the intermolecular CT effect. The present work might provide rich insight into designing and developing potential second-order optical nonlinearity materials with inter- and intramolecular CT characters.
Co-reporter:Feng-Wei Gao, Feng-Yi Zhang, Rong-Lin Zhong, Hong-Liang Xu, Shi-Ling Sun, Zhong-Min Su
Dyes and Pigments 2017 Volume 145(Volume 145) pp:
Publication Date(Web):1 October 2017
DOI:10.1016/j.dyepig.2017.05.039
•PLY and its isomer 1 radicals can form stable hetero-dimers.•The effect of boron and nitrogen substitution induces intermolecular charge-transfer.•Larger intermolecular charge-transfer significantly enhance second-order NLO properties.•The first hyperpolarizability density study clearly substantiates the difference in their βzzz values.Recently, the structure-property relationships of an attractive isomeric radical 1 (Phys. Chem. Chem. Phys., 2016, 18, 29041–29044) with famous phenalenyl (PLY) was investigated. Can PLY and 1 form stable π-dimers? The single point energy scan result shows that the staggered π-dimer (2) has the lowest energy. In order to explore intermolecular charge-transfer and nonlinear optical property, two π-dimers (2a and 2b by boron and nitrogen atoms substituting the central carbon atoms of 2) are designed. 2 has smaller intermolecular charge-transfer (0.020) and the first hyperpolarizability (βtot, 3.18 × 102 au). However, boron and nitrogen substitution effect can greatly enhance intermolecular charge-transfer (0.215 for 2a and 0.181 for 2b) and the βtot values (6.32 × 103 for 2a and 6.80 × 103 for 2b). Interestingly, the βtot values of 2a and 2b are close to each other, but their βz components and the NBO charge analysis show that 2a and 2b have opposite direction of charge transfer, which can be well explained by the difference of the dipole moment component (Δμz) between the ground and the excited states. Further, the first hyperpolarizability density study clearly substantiates the difference in their βzzz values: negative contribution for 2a is much larger than positive contribution, while the first hyperpolarizability density for 2b shows much larger positive contribution. Thus, the primary component of βzzz is negative value for 2a and βzzz is positive value for 2b. Combining with the frontier molecular orbital (FMO) and the electron density difference map (EDDM), intermolecular charge-transfer transition from B substituted fragment to N substituted fragment for 2a and 2b is concluded. The significant structure-property relationships in present π-dimers are beneficial for further theoretical and experimental investigations of high-performance nonlinear optical materials.The effect of boron and nitrogen substitution induces intermolecular charge-transfer, which significantly enhance second-order NLO properties of hetero-dimers with the aid of the DFT calculations.Download high-res image (266KB)Download full-size image
Co-reporter:Feng-Wei Gao, Rong-Lin Zhong, Hong-Liang XuZhong-Min Su
The Journal of Physical Chemistry C 2017 Volume 121(Issue 7) pp:
Publication Date(Web):February 7, 2017
DOI:10.1021/acs.jpcc.6b11732
Phenalenyl π-dimer (PLY2) has recently attracted intensive research interest due to its unique structure and binding characteristics (two-electron/12-center bonding). The directional transfer of electron or electron pair under the external electric field can produce a new structure with interesting properties. In the present work, we investigate for the first time the effect of the external electric field along the main molecule axis on PLY2. Two unpaired electrons between two layers are gradually shifted to the upper layer with increasing of the external electric field strength (Fext): the weaker the two-electron/12-center bonding, the stronger the electrostatic interaction between two layers. Significantly, a small increment of Fext makes a big difference: the interlayer distance in the PLY2 is sharply elongated from 3.241 Å (Fext = 203 × 10–4 au) to 3.485 Å (Fext = 204 × 10–4 au), which leads to the two-electron/12-center bonding breaking at 204 × 10–4 au. Therefore, the Fext = 204 × 10–4 au is regarded as the critical electric field. In this case, the interaction between two layers in PLY2 is exclusively governed by the electrostatic interaction. Besides this, the effect of the external electric field brings some distinctive changes in its diradical character (y0), the Wiberg bond index (WBI), the interaction energy (Eint), and the frontier molecular orbital (FMO) that can be used to explore the conversion between bonding and electrostatic interactions. This study can deepen the understanding for the effect of the external electric field on structures and electric properties for molecule and be an open a door for the discovery and development of new switching devices.
Co-reporter:Feng-Wei Gao;Zhong-Min Su
Physical Chemistry Chemical Physics 2017 vol. 19(Issue 47) pp:31958-31964
Publication Date(Web):2017/12/06
DOI:10.1039/C7CP06412H
In this work, we applied an external electric field (F) to a biphenalenyl derivative (BN-PLY2) in the direction of the negative z-axis (F−z) and the positive z-axis (F+z), respectively. The influence of the two directions of F on the molecular structures and electronic properties is investigated, which gives interesting results. Density functional theory (DFT) calculations show that the application of F−z (F−z = 0 to −190 × 10−4) is an advantage toward improving π-dimer stability, which is attributed to an increase in bonding and attractive electrostatic interactions. Interestingly, a large amount of negative charge is induced by applying F−z to the upper layer, resulting in an increase in the electron density in the upper layer, which is the main factor for the formation of a symmetric highest occupied molecular orbital (HOMO) at F−z = −180 × 10−4 au (−9.26 × 109 V m−1). Moreover, when F+z is applied, the HOMO and HOMO−1 undergo orbital interchange in the π-dimer at F+z = 100/110 × 10−4 au. Significantly, the effect of the external electric field effectively regulates the first hyperpolarizabilities (βtot). When the F+z ranges from 0 to 140 × 10−4 au, the βtot values slightly decrease to 0 au. Note that, upon increasing F+z, the βtot values sharply increase to 6.67 × 103 au (F+z = 190 × 10−4 au). Furthermore, the evolutions of the absorption spectra under F might well explain the trend of βtot values. When the F+z ranges from 0 to 140 × 10−4 au, the broad absorption spikes with a low-energy are significantly blue-shifted, while only absorption spikes with a high-energy are significantly red-shifted (F+z = 140 to 190 × 10−4 au). The present work not only provides a deeper understanding of the relationships between the molecular structure and the electronic properties of a π-dimer system, but can also be developed for designing highly efficient nonlinear optical materials through the influence of an external electric field.
Co-reporter:Rong-Lin Zhong, Hong-Liang Xu and Zhong-Min Su  
Physical Chemistry Chemical Physics 2016 vol. 18(Issue 20) pp:13954-13959
Publication Date(Web):20 Apr 2016
DOI:10.1039/C6CP00647G
Carbon–boron–nitride heteronanotubes (BNCNT) have attracted a lot of attention because of their adjustable properties and potential applications in many fields. In this work, a series of CA, PA and HA armchair BNCNT models were designed to explore their nonlinear optical (NLO) properties and provide physical insight into the structure–property relationships; CA, PA and HA represent the models that are obtained by doping the carbon segment into pristine boron nitride nanotube (BNNT) fragments circularly around the tube axis, parallel to the tube axis and helically to the tube axis, respectively. Results show that the first hyperpolarizability (β0) of an armchair BNCNT model is dramatically dependent on the connecting patterns of carbon with the boron nitride fragment. Significantly, the β0 value of PA-6 is 2.00 × 104 au, which is almost two orders of magnitude larger than those (6.07 × 102 and 1.55 × 102 au) of HA-6 and CA-6. In addition, the β0 values of PA and CA models increase with the increase in carbon proportion, whereas those of HA models show a different tendency. Further investigations on transition properties show that the curved charge transfer from N-connecting carbon atoms to B-connecting carbon atoms of PA models is essentially the origin of the big difference among these models. This new knowledge about armchair BNCNTs may provide important information for the design and preparation of advanced NLO nano-materials.
Co-reporter:Rong-Lin Zhong, Hong-Liang Xu, Zhong-Min Su
Chemical Physics Letters 2016 Volume 658() pp:230-233
Publication Date(Web):1 August 2016
DOI:10.1016/j.cplett.2016.06.054
•The physical properties of Li@BCN models are dependent on the different chemical environment of the tube termination.•The crucial electron population in the BCNs of Li@B-BCN and Li@N-BCN series is significantly different.•The first hyperpolarizabilities of Li@N-BCN series are dramatically larger than that of Li@B-BCN series.A series of Li@BCN models were systematically investigated to explore the physical origin of the interaction between lithium atoms and BCNs. Theoretical results show that the crucial electron population in the BCNs of Li@B-BCN and Li@N-BCN series is dramatically different. As results, the first hyperpolarizability of Li@B-BCN series increases with the increase of carbon proportion whereas that of Li@N-BCN series significantly decreases with the increase of carbon proportion. The results indicate that the physical properties of Li@BCN models are significantly dependent on the different chemical environment of the tube termination.
Co-reporter:Xue Zhang, Shi-Ling Sun, Hong-Liang Xu and Zhong-Min Su  
RSC Advances 2015 vol. 5(Issue 81) pp:65991-65997
Publication Date(Web):24 Jul 2015
DOI:10.1039/C5RA10156E
It is well known that ammonia borane (BH3NH3) is one of the simplest donor–acceptor complexes. The donor–acceptor bond (B–N bond) is formed by sharing lone pair electrons between BH3 and NH3 groups. In the present work, different strengths of external electric fields (Eext) are applied along the Z-axis direction to investigate the electric field induced effect on the BH3NH3 structure and properties. Interestingly, we have found that the lone pair electrons can be gradually moved in the “channel” between the BH3 and NH3 groups by modulating Eext. The donor–acceptor bond (B–N bond) is gradually elongated until it breaks when the Eext ranges from 0.0000 to 0.0321 au. The B–N bond is the shortest at Eext = −0.0519 au. Interestingly, the negative charge on BH3 groups sharply decreases from 0.161 to 0.005 (for NH3 groups decreases from 0.161 to 0.005) and the electron cloud of HOMO−2 exhibits an obvious transformation at “broking bonding” Eext ranging from 0.0320 to 0.0321 au, indicating the electron movement induced by the electric-field is the main reason to change the structure and stability of BH3NH3. Further, atoms in molecules (AIM) analysis shows that the B⋯N interactions are similar to that of hydrogen bonds at Eext = −0.0767 au and the iconicity of B–N bond in BH3NH3 is confirmed by its low electron density for B–N ρ(B–N) (0.103–0.073) in the region of Eext (0–0.025 au).
Co-reporter:Ying Gao, Rong-Lin Zhong, Hong-Liang Xu, Shi-Ling Sun and Zhong-Min Su  
RSC Advances 2015 vol. 5(Issue 38) pp:30107-30119
Publication Date(Web):23 Mar 2015
DOI:10.1039/C5RA01145K
In 2003, a novel compound 2 containing the benzo-15-crown-5 moiety was synthesized and described. In the present work, we have designed two compounds 1 (benzo-12-crown-4) and 3 (benzo-18-crown-6) on the basis of compound 2. Further, nine configurations N*M (N = 1, 2 and 3; M = Li+, Na+ and K+) are designed by the compounds 1, 2 and 3 complexing alkali metal cations. Density functional calculation is performed to investigate the effect of ring size and the nature of the alkali metal cations on the interaction energy, charge transfer and nonlinear optical properties. The results indicate that the interaction energy of N*M depends on both the ring size and the nature of the alkali metal cations. Moreover, the amount of net charge transfer is related to the diameters of the alkali metal cations. In addition, the calculated nonlinear optical properties reveal that compound 2 has the largest first hyperpolarizability among the three compounds 1, 2 and 3. However, the alkali metal cations give rise to different effects on the nonlinear optical properties. Significantly, the order of the first hyperpolarizability can be explained by the transition energy and the dipole moment variation within the two-state approximation.
Co-reporter:Feng-Wei Gao;Rong-Lin Zhong;Shi-Ling Sun
Journal of Molecular Modeling 2015 Volume 21( Issue 10) pp:
Publication Date(Web):2015 October
DOI:10.1007/s00894-015-2808-9
Very recently, two new cage-like radicals (C59B and C59N) formed by a boron or nitrogen atom substituting one carbon atom of C60 were synthesized and characterized. In order to explore the structure–property relationships of combination the cage-like radical and alkali metal, the endohedral Li@C59B and Li@C59N are designed by lithium (Li) atom encapsulated into the cage-like radicals C59B and C59N. Further, the structures, natural bond orbital (NBO) charges, and nonlinear optical (NLO) responses of C59B, C59N, Li@C59B, and Li@C59N were investigated by quantum chemical method. Three density functional methods (BHandHLYP, CAM-B3LYP, and M05-2X) were employed to estimate their first hyperpolarizabilities (βtot) and obtained the same trend in the βtot value. The βtot values by BHandHLYP functional of the pure cage-like radicals C59B (1.30 × 103 au) and C59N (1.70 × 103 au) are close to each other. Interestingly, when one Li atom encapsulated into the electron-rich radical C59N, the βtot value of the Li@C59N increases to 2.46 × 103 au. However, when one Li atom encapsulated into the electron-deficient radical C59B, the βtot value of the Li@C59B sharply decreases to 1.54 × 102 au. The natural bond orbital analysis indicates that the encapsulated Li atom leads to an obvious charge transfer and valence electrons distribution plays a significant role in the βtot value. Further, frontier molecular orbital explains that the interesting charge transfer between the encapsulated Li atom and cage-like radicals (C59B and C59N) leads to differences in the βtot value. It is our expectation that this work will provide useful information for the design of high-performance NLO materials.
Co-reporter:Feng-Wei Gao;Ying Gao;Li-Jie Wang
Journal of Molecular Modeling 2015 Volume 21( Issue 10) pp:
Publication Date(Web):2015 October
DOI:10.1007/s00894-015-2803-1
Recently, the crystal structures and electrochemical properties of the isomers (Sc2S “trapped” in C82) have been reported, in which the Sc2S is located inside the different positions of the C82 cage. In the present work, three isomers of endohedral metallofullerenes Sc2S@C3v(8)-C82 (A, B, and C) have been designed to explore the effect of the position of Sc2S on their interaction energies and nonlinear optical properties. Among three isomers, the Sc2S is located in different positions of the C82 cage: the angles of Sc–S–Sc in A, B, and C are 104.9, 114.8, and 115.7°, respectively. Furthermore, the analysis of natural bond orbital (NBO) charge indicates that the electron-transfer is from the Sc2S to the adjacent carbon atoms of the C82 cage. The interaction energy of B is the smallest among three isomers which is −226.2 kcal mol-1. It was worth mentioning that their first hyperpolarizabilities (βtot) were studied, we found that their βtot values were related to the positions of Sc2S: C (2100) > B (1191) > A (947 au). We hope that the present work can provide a new strategy to promote the nonlinear optical properties of endohedral metallofullerenes by changing the positions of the encapsulated molecular.
Co-reporter:Rong-Lin Zhong; Hong-Liang Xu; Zhi-Ru Li;Zhong-Min Su
The Journal of Physical Chemistry Letters 2015 Volume 6(Issue 4) pp:612-619
Publication Date(Web):January 28, 2015
DOI:10.1021/jz502588x
The excess electron is a kind of special anion with dispersivity, loosely bounding and with other fascinating features, which plays a pivotal role (promote to about 106 times in (H2O)3{e}) in the large first hyperpolarizabilities (β0) of dipole-bound electron clusters. This discovery opens a new perspective on the design of novel nonlinear optical (NLO) molecular materials for electro-optic device application. Significantly, doping alkali metal atoms in suitable complexants was proposed as an effective approach to obtain electride and alkalide molecules with excess electron and large NLO responses. The first hyperpolarizability is related to the characteristics of complexants and the excess electron binding states. Subsequently, a series of new strategies for enhancing NLO response and electronic stability of electride and alkalide molecules are exhibited by using various complexants. These strategies include not only the behaviors of pushed and pulled electron, size, shape, and number of coordination sites of complexants but also the number and spin state of excess electrons in these unusual NLO molecules.
Co-reporter:Xue Zhang, Heng-Qing Wu, Hong-Liang Xu, Shi-Ling Sun, and Zhong-Min Su
The Journal of Physical Chemistry A 2015 Volume 119(Issue 4) pp:767-773
Publication Date(Web):December 23, 2014
DOI:10.1021/jp5103127
Very recently, the investigation of an Li atom doped effect on the “through-space” electronic interaction (S) of a donor–S–acceptor (D–S–A, 1) shows that the Li-doping effect can modulate the first hyperpolarizability of 1 ( Dyes Pigm. 2014, 106, 7−13). Can we further enhance the first hyperpolarizability (βtot) of 1 by modulating the charge transfer of D–S–A molecules? The present work indicates that the βtot value can be successfully modulated by replacing the sp2-hybridized CH═CH moiety connected with substituted para-cyclophane (PCP). On the other hand, the NO2 contributes more than NH2 to the βtot value. The results of time-dependent density functional theory (TD-DFT) provide a good explanation for the variation in the βtot value. Interestingly, the βtot value of 3 (4.09 × 103 au) is larger than 1.52 × 103 au of 4, while the difference between the dipole moments (Δμ) of the ground state and the crucial excited state of 3 (2.93 D) is smaller than that of 4 (7.79 D). Further, the charge-transfer excitation length (DCT) of 3 (1.41 Å) is smaller than that of 4 (2.89 Å). Therefore, DCT is the major factor in determining the Δμ value.
Co-reporter:Sa Chen;Shi-Ling Sun;Liang Zhao
Journal of Molecular Modeling 2015 Volume 21( Issue 8) pp:
Publication Date(Web):2015 August
DOI:10.1007/s00894-015-2750-x
Due to unpaired electrons, both radicals and superalkali are investigated widely. In this work, two interesting complexes (Li3O-PLY and Li3-PLY) were constructed by phenalenyl radical and superalkali atoms. Why are they interesting? Firstly, for Li3O-PLY and Li3-PLY, although the charge transfer between superalkali atoms and PLY is similar, the sandwich-like charge distribution for Li3O-PLY causes a smaller dipole moment than that of Li3-PLY. Secondly, their UV–vis absorption show that the maximum wavelengths for Li3O-PLY and Li3-PLY display a bathochromic shift compared to PLY. Moreover, Li3-PLY has two new peaks at 482 and 633 nm. Significantly, the β0 values of Li3-PLY (4943–5691 a.u.) are much larger than that of Li3O-PLY (225–347 a.u.). Further, the βHRS values of Li3O-PLY decrease slightly while βHRS of Li3-PLY increase dramatically with increasing frequency. It is our expectation that these results might provide beneficial information for theoretical and experimental studies on complexes with superalkali and PLY radicals.
Co-reporter:Li-Jie Wang, Rong-Lin Zhong, Shi-Ling Sun, Hong-Liang Xu, Xiu-Mei Pan and Zhong-Min Su  
Dalton Transactions 2014 vol. 43(Issue 25) pp:9655-9660
Publication Date(Web):10 Mar 2014
DOI:10.1039/C3DT53329H
Recently, a new sulfide cluster fullerene, Sc2S@Cs (10528)-C72 containing two pairs of fused pentagons has been isolated and characterized (Chen et al., J. Am. Chem. Soc., 2012, 134, 7851). Inspired by this investigation, we propose a question: what properties will be influenced by the interaction between the encapsulated V-shaped polar molecule and C72? To answer this question, four encapsulated metallic fullerenes (EMFs) M2N@C72 (M = Sc or Y, N = S or O) along with pristine Cs-C72 (10528) were investigated by quantum chemistry methods. The results show that the Egap (3.01–3.14 eV) of M2N@C72 are significantly greater than that of pristine Cs-C72 (10528) (2.34 eV). This indicates that the stabilities of these EMFs increase by encapsulating the V-shaped polar molecule into the fullerene. Furthermore, the natural bond orbital (NBO) charge analysis indicates electron transfer from M2N to C72 cage, which plays a crucial role in enhancing first hyperpolarizability (βtot). The βtot follows the order of 1174 au (Y2O@C72) ≈ 1179 au (Sc2O@C72) > 886 au (Y2S@C72) ≈ 864 au (Sc2S@C72) > 355 au (C72). This indicates that the βtot of M2N@C72 is more remarkable than that of pristine Cs-C72 (10528) due to the induction effect of the encapsulated molecule. Compared with sulfide cluster fullerenes (Y2S@C72 and Sc2S@C72), oxide cluster fullerenes (Sc2O@C72 and Y2O@C72) show much larger βtot due to the small ionic radius and the large electronegativity of oxygen. In contrast, the metal element (scandium and yttrium) has a slight influence on the βtot. Thus, oxide cluster fullerenes are candidates to become promising nonlinear optical materials with higher performance.
Co-reporter:Heng-Qing Wu, Hong-Liang Xu, Shi-Ling Sun, Zhong-Min Su
Dyes and Pigments 2014 Volume 106() pp:7-13
Publication Date(Web):July 2014
DOI:10.1016/j.dyepig.2014.01.031
•Three complexes were designed by doping Li atom into D-S-A(1) for the first time.•In 1-Li-Mid, intermediate cavity hinders the polarization of Li atom.•The most negative NICS value of 1-Li-Mid is −52.0 ppm.•The direction of crucial transition is the important factor for βtot value.•Resonances in Li-doped D-S-A molecules resulting in huge βHRS(−2ω;ω,ω) value.In the present work, three complexes(1-Li–NO2, 1-Li-Mid and 1-Li–NH2) were designed by doping Li atom into the different location(above, middle and below) of the novel noncovalent “through-space” electronic interaction (S) of Donor-S-Acceptor (1) to explore their structure-property relationships. The results show that doping Li atom can obviously enhance the first hyperpolarizability (βtot) of 1. Interestingly, the crucial transition direction of 1-Li–NH2 is from donor group to acceptor group, which is opposite to those of 1-Li–NO2 and 1-Li-Mid. The highest occupied molecular orbital (HOMO) of 1-Li–NH2 shows that doping one Li atom enhances the π–π interaction resulting in the largest βtot value (1.50 × 105) which is about 16 times larger than that of 1(9.13 × 103) and is also obviously larger than those of 1-Li-Mid(5.81 × 104) and 1-Li–NO2(6.45 × 104 au). The results indicate that 1-Li–NH2 can be considered as a novel high-performance NLO material and the location of Li atom can modulate NLO response.In the present work, three complexes (1-Li–NO2, 1-Li-Mid and 1-Li–NH2) were designed by doping Li atom into the location (above, middle and below) of the S of 1 to explore their structures, aromaticities and nonlinear optical properties.
Co-reporter:Sa Chen, Shi-Ling Sun, Heng-Qing Wu, Hong-Liang Xu, Liang Zhao and Zhong-Min Su  
Dalton Transactions 2014 vol. 43(Issue 33) pp:12657-12662
Publication Date(Web):02 Jun 2014
DOI:10.1039/C4DT01240B
Recently, the well-known phenalenyl radical π-dimer with its fascinating 2-electron/12-center (2e/12c) bond has attracted our attention. In this work, we designed two molecules, Li3O⋯C13H9 (1a) and BeF3⋯C13H9 (1b). Interestingly, owing to the inductive effect of superatoms, an electron is transferred from Li3O to phenalenyl in 1a, while an electron is transferred from phenalenyl to BeF3 in 1b. Further, we employed 1a and 1b as building blocks to assemble two novel molecules with 2e/12c bonds: Li3O⋯(C13H9)2⋯BeF3 (2a) and Li3O⋯(C13H9)2⋯BeF3 (2b). Remarkably, 2a and 2b with novel 2e/12c bonds exhibit a dramatic interlayer charge-transfer character, which results in a significant difference of dipole moments (Δμ: 2.6804 for 2a and 3.8019 Debye for 2b) between the ground state and the crucial excited state. As a result, the static first hyperpolarizabilities (β0: 5154 for 2a and 12500 au for 2b) are considerably larger than the values of 347 for 1a and 328 au for 1b. It is our expectation that the results of the present work might provide beneficial information for further theoretical and experimental studies on the fascinating properties of molecules with interlayer charge-transfer character.
Co-reporter:Ying Gao, Shi-Ling Sun, Hong-Liang Xu, Liang Zhao and Zhong-Min Su  
RSC Advances 2014 vol. 4(Issue 47) pp:24433-24438
Publication Date(Web):13 May 2014
DOI:10.1039/C4RA02238F
In this work, the 1-Li+, 1-Na+ and 1-K+ complexes formed by N-methylbenzoaza-18-crown-6-ether derivatives (1) with one alkali metal cation (Li+, Na+ and K+) were investigated. Significantly, the dipole moments of 1-Li+, 1-Na+ and 1-K+ enhance with increasing atomic number. However, their first hyperpolarizabilities (β0) decrease with increasing the atomic number. Further results show that the interaction energies increase in the order of 1-Li+ > 1-Na+ > 1-K+. Moreover, the transition energies of 1-Li+, 1-Na+ and 1-K+ are inversely proportional to the β0 values. Therefore, the interaction energy and transition energy are the major factors determining the β0 values of 1-Li+, 1-Na+ and 1-K+. The combining of large variations of the dipole moment and the first hyperpolarizability can be used as a detection sensor for alkali metal cations. We hope that this work will provide valuable knowledge for designing alkali metal cation sensors by electro-optical properties.
Co-reporter:Rong-Lin Zhong;Dr. Shi-Ling Sun;Dr. Hong-Liang Xu; Yong-Qing Qiu ; Zhong-Min Su
ChemPlusChem 2014 Volume 79( Issue 5) pp:732-736
Publication Date(Web):
DOI:10.1002/cplu.201300381

Abstract

Carbon–boron–nitride heteronanotubes have attracted much interest owing to their adjustable properties and wide applications in many fields. In this work, the structures and first hyperpolarizabilities (β0) of a series of HA-n and isoelectronic PA-n heteronanotubes are investigated, in which HA-n is composed of a helical C segment and BN segment, and PA-n is composed of an arc C segment and BN segment. Interestingly, the helix C segment in HA-9 leads to a fascinating long-range charge-transfer character. As a result, the β0 value of HA-9 is 1.80×104 a.u., which is much larger than that of PA-9 (4.99×103 a.u.). Significantly, the β0 value of the C segment in HA-9 is 1.72×104 a.u., whereas that of the BN segment in HA-9 is much smaller (7.48×102 a.u.). In this context, the larger β0 value of HA-9 is essentially induced by the helix topological effect of the C segment. It is our expectation that this new knowledge about heteronanotubes might provide more ideas for further exploration of sp2-hybridized carbon segments with special topologies.

Co-reporter:Ying Gao, Shi-Ling Sun, Hong-Liang Xu, Zhong-Min Su
Chemical Physics Letters 2014 600() pp: 123-127
Publication Date(Web):
DOI:10.1016/j.cplett.2014.03.037
Co-reporter:Yang-Yang Hu;Dr. Shi-Ling Sun;Wen-Tao Tian; Wei Quan Tian;Dr. Hong-Liang Xu; Zhong-Min Su
ChemPhysChem 2014 Volume 15( Issue 5) pp:929-934
Publication Date(Web):
DOI:10.1002/cphc.201301149

Abstract

A series of spiral donor–π–acceptor frameworks (i.e. 22, 33, 44, and 55) based on 4-nitrophenyldiphenylamine with π-conjugated linear acenes (naphthalenes, anthracenes, tetracenes, and pentacenes) serving as the electron donor and nitro (NO2) groups serving as the electron acceptor were designed to investigate the relationships between the nonlinear optical (NLO) responses and the spirality in the frameworks. A parameter denoted as D was defined to describe the extent of the spiral framework. The D value reached its maximum if the number of NO2 groups was equal to the number of fused benzene rings contained in the linear acene. A longer 4-nitrophenyldiphenylamine chain led to a larger D value and, further, to a larger first hyperpolarizability. Different from traditional NLO materials with charge transfer occurring in the one-dimensional direction, charge transfer in 22, 33, 44, and 55 occur in three-dimensional directions due to the attractive spiral frameworks, and this is of great importance in the design of NLO materials. The origin of such an enhancement in the NLO properties of these spiral frameworks was explained with the aid of molecular orbital analysis.

Co-reporter:Yang-Yang Hu;Dr. Shi-Ling Sun;Wen-Tao Tian; Wei Quan Tian;Dr. Hong-Liang Xu; Zhong-Min Su
ChemPhysChem 2014 Volume 15( Issue 5) pp:
Publication Date(Web):
DOI:10.1002/cphc.201490021
Co-reporter:Heng-Qing Wu ; Rong-Lin Zhong ; Shi-Ling Sun ; Hong-Liang Xu ;Zhong-Min Su
The Journal of Physical Chemistry C 2014 Volume 118(Issue 13) pp:6952-6958
Publication Date(Web):March 17, 2014
DOI:10.1021/jp410560j
Adamantane (Ad) is the parent molecule of diamondoids, which has been the subject of much chemical interest because of its highly symmetric cage structure. Many valuable papers demonstrated that the H atom of the methine position in Ad is highly reactive. Compared with highly symmetric carbon structures such as graphene and single-walled carbon nanotubes (SWCNTs), Ad only possesses σ bonds. In this work, we report a quantum chemical calculation on three complexes (Ad-Li, Ad-Na, and Ad-K), which were obtained by substituting the H atom of methine position in Ad with alkali metal (Li, Na, and K). Interestingly, the substitution by alkali metals leads to absorption within the visible region. The maximum absorption wavelengths of the complexes show a red shift trend from the Li to the K complex. This trend indicates that the crucial transition energy becomes smaller, which might lead to a larger nonlinear optical response. Among the three structures, the largest first static hyperpolarizability (βtot) of the K complex was 76626 au, which is about 45 times larger than a prototypical second-order nonlinear optical (NLO) molecule of p-nitroaniline (βtot = 1679 au). Therefore, our results show that alkali metal substituted Ads may be novel potential candidates for high-performance NLO materials.
Co-reporter:Rong-Lin Zhong ; Shi-Ling Sun ; Hong-Liang Xu ; Yong-Qing Qiu ;Zhong-Min Su
The Journal of Physical Chemistry C 2014 Volume 118(Issue 26) pp:14185-14191
Publication Date(Web):June 4, 2014
DOI:10.1021/jp503281q
Recently, the N-connecting pattern of the BN-segment has been shown as a suitable strategy to enhance the static first hyperpolarizability (β0) of carbon–boron–nitride heterojunction nanotubes (J. Phys. Chem. C 2013, 117, 10039–10044). In this work, we report a quantum chemical investigation on the lithiation effect to further reveal the mechanism of modification. Interestingly, the lithiation effect is significantly dependent on the activating segment of the heterojunction nanotubes. For lithiation on the BN-segment, the β0 (3.22 × 104 au) of Li5–BN-1a is larger than that (1.42 × 104 au) of Li5–BN-2a, which shows that the N-connecting pattern of the BN-segment linking to the C-segment is an efficient way to enhance the β0 of heterojunction nanotubes. However, for lithiation on the C-segment, the β0 (6.03 × 104 au) of Li5–BN-1b is even slightly smaller than that (6.97 × 104 au) of Li5–BN-2b. Besides, results show that activating the C-segment is a more effective strategy than activating the BN-segment for enhancing the β0 of carbon–boron–nitride heterojunction nanotubes by lithiation. The new knowledge about heterojunction nanotubes might provide important information for designing nonlinear optical molecules by rationally introducing lithium atoms on carbon–boron–nitride heterojunction nanotubes.
Co-reporter:Fang Ma, Dong-Sheng Bai, Hong-Liang Xu
Journal of Molecular Graphics and Modelling 2014 Volume 53() pp:161-167
Publication Date(Web):September 2014
DOI:10.1016/j.jmgm.2014.07.015
•One-dimensional polymeric structure by hydrogen-bond-directed-linking is constructed.•The transparency-efficiency tradeoff is modulated.•Double-degenerated charge transitions contribute to the hyperpolarizabilities in an additive fashion.It is well known that settling transparency-efficiency tradeoff is important to design nonlinear optical (NLO) materials. In this work, we constructed one-dimensional polymeric cyanoacetylene (NCCCH)n by hydrogen-bond-directed-linking to understand this tradeoff from molecular level. Results show that the first hyperpolarizability of (NCCCH)n (n = 2–8) gradually increased with the increase of n, and what is more important is that the red-shifts, associated with the increase of n, were very little. It is proposed that these polymeric structures possess double-degenerated charge transitions, which contribute to the hyperpolarizability in an additive fashion, and that the coupled oscillators are gradually improved, which lead to the increase of the first hyperpolarizability. Therefore, we propose the hydrogen-bond-directed-linking idea is helpful to develop the potential high-performance NLO materials.An attractive hydrogen-bond-directed-linking approach practically solves transparency-efficiency tradeoff and contributes to the development of potential high-performance NLO materials.
Co-reporter:Li-Jie Wang, Shi-Ling Sun, Rong-Lin Zhong, Yan Liu, Dong-Lai Wang, Heng-Qing Wu, Hong-Liang Xu, Xiu-Mei Pan and Zhong-Min Su  
RSC Advances 2013 vol. 3(Issue 32) pp:13348-13352
Publication Date(Web):10 May 2013
DOI:10.1039/C3RA40909K
Recently, C60Cl8 (C2v) has been experimentally synthesized (Y.-Z. Tan, et al., Nat. Mater., 2008, 7, 790) by the addition of eight chlorine atoms to C60 (C2v), which is associated with a Stone–Wales transformation of C60 (Ih). In this work, the first hyperpolarizabilities (βtot) of C60 (C2v) and C60Cl8 (C2v) are investigated. After the Stone–Wales transformation and chlorine addition reaction, the βtot values slightly increase from 0 for C60 (Ih) to 60 au for C60 (C2v) and 502 au for C60Cl8 (C2v), respectively. To further enhance the first hyperpolarizability, the endohedral fullerene derivative, Li@C60Cl8, formed by encapsulating a lithium (Li) atom inside the C60Cl8, has been designed. Interestingly, the electron transfer between Li and C60Cl8 leads to an extremely large βtot value of 25569 au, which is considerably larger (51 times) than the 502 au of C60Cl8. It shows that the encapsulated Li effect plays an important role in enhancing the first hyperpolarizability, so the Li@C60Cl8 can be considered as a candidate for high-performance nonlinear optical materials.
Co-reporter:Rong-Lin Zhong, Shi-Ling Sun, Hong-Liang Xu, Yong-Qing Qiu, and Zhong-Min Su
The Journal of Physical Chemistry C 2013 Volume 117(Issue 19) pp:10039-10044
Publication Date(Web):April 22, 2013
DOI:10.1021/jp402561h
An increasing number of scientists have focused on carbon–boron-nitride heteronanotubes because of their particularly adjustable properties, as shown in many fields. In this work, four isoelectronic models (BN-n, n = 1–4) were systematically investigated to explore the crucial factor for enhancing the static first hyperpolarizibility by doping the BN segment into the carbon nanotube (CNT) with differently connecting patterns. Theoretical results show that the N-connecting pattern might increase the contribution of the BN segment to the crucial transition states, which obviously increases the occupied orbital energy while the unoccupied orbital energy is slightly influenced. Correspondingly, the transition energy of BN-1 is smaller than that of BN-2. As a result, the static first hyperpolarizability of BN-1 is 1.05 × 104 au, which is remarkably larger than the 4.37 × 102 au of BN-2. The results indicate that, compared to the B-connecting pattern, the N-connecting pattern of the BN segment linking to the conjugated CNT segment is a more efficient way to enhance the first hyperpolarizability of heteronanotubes. It is our expectation that the new knowledge about the carbon–boron-nitride heteronanotubes could provide valuable information for scientists to develop the potential nonlinear optical nanomaterials by introducing BN segments into suitable positions of CNTs.
Co-reporter:Rong-Lin Zhong, Hong-Liang Xu, Shabbir Muhammad, Ji Zhang and Zhong-Min Su  
Journal of Materials Chemistry A 2012 vol. 22(Issue 5) pp:2196-2202
Publication Date(Web):15 Dec 2011
DOI:10.1039/C1JM14358A
Excess electron compounds have been proposed to be novel candidates of high-performance nonlinear optical (NLO) materials because of their large static first hyperpolarizabilities (β0). To enhance the stability of an unstable excess electron compound (LiCN⋯Li) with an extremely large β0 value (310196 a.u.), we designed a boron nitride nanotube (BNNT) as a protective shield molecule to encapsulate it (in theory). The stability of LiCN⋯Li was enhanced: the vertical ionization potentials (VIP) of LiCN⋯Li increased after encapsulating. Therefore, by comparison with LiCN⋯Li, the encapsulated complexes are more difficult to oxidize. Significantly, the BNNT encapsulated LiCN⋯Li complex exhibits a considerable β0 value (10645 a.u.), which is significantly (almost 380 times) larger than 28 a.u. of BNNT. Our further investigations into the intrinsic hyperpolarizabilites (βint) of these compounds show that there are clearly dependencies of the NLO response on the transition energy. Furthermore, it is easy to encapsulate LiCN⋯Li from the B-rich edge rather than N-rich edge of BNNT due to the lower energy barrier, which makes our calculations more useful to experimentalists who may try to synthesize these compounds. Knowledge of the encapsulation process of LiCN⋯Li within BNNT provides a new strategy for the design and synthesis of stable high-performance NLO materials.
Co-reporter:Dr. Dong-Lai Wang ;Dr. Hong-Liang Xu; Zhong-Min Su;Dr. Shabbir Muhammad;Dr. Dong-Yan Hou
ChemPhysChem 2012 Volume 13( Issue 5) pp:1232-1239
Publication Date(Web):
DOI:10.1002/cphc.201100774

Abstract

Drying-tube-shaped single-walled carbon nanotubes (SWCNTs) with multiple carbon ad-dimer (CD) defects are obtained from armchair (n,n,m) SWCNTs (n=4, 5, 6, 7, 8; m=7, 13). According to the isolated-pentagon rule (IPR) the drying-tube-shaped SWCNTs are unstable non-IPR species, and their hydrogenated, fluorinated, and chlorinated derivatives are investigated. Interestingly, chemisorptions of hydrogen, fluorine, and chlorine atoms on the drying tube-shaped SWCNTs are exothermic processes. Compared to the reaction energies for binding of H, F, and Cl atoms to perfect and Stone–Wales-defective armchair (5,5) nanotubes, binding of F with the multiply CD defective SWCNTs is stronger than with perfect and Stone–Wales-defective nanotubes. The reaction energy for per F2 addition is between 85 and 88 kcal mol−1 more negative than that per H2 addition. Electronic structure analysis of their energy gaps shows that the CD defects have a tendency to decrease the energy gap from 1.98–2.52 to 0.80–1.17 eV. After hydrogenation, fluorination, and chlorination, the energy gaps of the drying-tube-shaped SWCNTs with multiple CD defects are substantially increased to 1.65–3.85 eV. Furthermore, analyses of thermodynamic stability and nucleus-independent chemical shifts (NICS) are performed to analyze the stability of these molecules.

Co-reporter:Rong-Lin Zhong;Dr. Hong-Liang Xu; Zhong-Min Su; Zhi-Ru Li;Dr. Shi-Ling Sun; Yong-Qing Qiu
ChemPhysChem 2012 Volume 13( Issue 9) pp:
Publication Date(Web):
DOI:10.1002/cphc.201290042
Co-reporter:Rong-Lin Zhong;Dr. Hong-Liang Xu; Zhong-Min Su; Zhi-Ru Li;Dr. Shi-Ling Sun; Yong-Qing Qiu
ChemPhysChem 2012 Volume 13( Issue 9) pp:2349-2353
Publication Date(Web):
DOI:10.1002/cphc.201200213

Abstract

Much effort has been devoted to investigating the unusual properties of the π electrons in Möbius cyclacenes, which are localized in a special region. However, the localized π electrons are a disadvantage for applications in optoelectronics, because intramolecular charge transfer is limited. This raises the question of how the intramolecular charge transfer of a Möbius cyclacene with clearly localized π electrons can be enhanced. To this end, [8]Möbius cyclacene ([8]MC) is used as a conjugated bridge in a donor–π-conjugated bridge–acceptor (D–π–A) system, and NH2-6-[8]MC-10-NO2 exhibits a fascinating spiral charge-transfer transition character that results in a significant difference in dipole moments Δμ between the ground state and the crucial excited state. The Δμ value of 6.832 D for NH2-6-[8]MC-10-NO2 is clearly larger than that of 0.209 D for [8]MC. Correspondingly, the first hyperpolarizability of NH2-6-[8]MC-10-NO2 of 12 467 a.u. is dramatically larger than that of 261 a.u. for [8]MC. Thus, constructing a D–π–A framework is an effective strategy to induce greater spiral intramolecular charge transfer in MC although the π electrons are localized in a special region. This new insight into the properties of π electrons in Möbius cyclacenes may provide valuable information for their applications in optoelectronics.

Co-reporter:Heng-Qing Wu;Shi-Ling Sun;Rong-Lin Zhong
Journal of Molecular Modeling 2012 Volume 18( Issue 11) pp:4901-4907
Publication Date(Web):2012 November
DOI:10.1007/s00894-012-1478-0
In the present work, Li@porphyrins and their derivatives were designed in order to explore the effect of dehydrogenation/hydrogenation on linear and nonlinear optical properties. Their stable structures were obtained by the M06-2X method. Moreover, the M06-2X method showed that dehydrogenation/hydrogenation has greatly influences polarizabilities (α0 values) and hyperpolarizabilities (βtot and γtot values): α0 values ranged from 331 to 389 au, βtot values from 0 to 2465 au, and γtot values from −21.2 × 104 to 21.4 × 104 au. This new knowledge of the effect of dehydrogenation/hydrogenation on nonlinear optical properties may prove beneficial to the design and development of high-performance porphyrin materials.
Co-reporter:Rong-Lin Zhong;Dr. Hong-Liang Xu;Dr. Shi-Ling Sun; Yong-Qing Qiu ; Zhong-Min Su
Chemistry - A European Journal 2012 Volume 18( Issue 36) pp:11350-11355
Publication Date(Web):
DOI:10.1002/chem.201201570

Abstract

The unusual properties of species with excess electrons have attracted a lot of interest in recent years due to their wide applications in many promising fields. In this work, we find that the excess electron could be effectively bound by the B atoms of boron nitride nanotube (BNNT), which is inverted pyramidally distributed from B-rich edge to N-rich edge. Further, Li@B-BNNT and Li@N-BNNT are designed by doping the Li atom to the two edges of BNNT, respectively. Because of the interaction between the Li atom and BNNT, the 2s valence electron of Li becomes a loosely bound excess electron. Interestingly, the distribution of the excess electron in Li@N-BNNT is more diffuse and pyramidal from B-rich edge to N-rich edge, which is fascinating compared with Li@B-BNNT. Correspondingly, the transition energy of Li@N-BNNT is 0.99 eV, which is obviously smaller than 2.65 eV of Li@B-BNNT. As a result, the first hyperpolarizability (3.40×104 a.u.) of Li@N-BNNT is dramatically larger (25 times) than 1.35×103 a.u. of Li@B-BNNT. Significantly, we find that the pyramidal distribution of the excess electron is the key factor to determine the first hyperpolarizability, which reveals useful information for scientists to develop new electro-optic applications of BNNTs.

Co-reporter:Rong-Lin Zhong;Dr. Hong-Liang Xu;Dr. Shi-Ling Sun; Yong-Qing Qiu ; Zhong-Min Su
Chemistry - A European Journal 2012 Volume 18( Issue 36) pp:
Publication Date(Web):
DOI:10.1002/chem.201290154
Co-reporter:Yang-Yang Hu ; Shi-Ling Sun ; Rong-Lin Zhong ; Hong-Liang Xu ;Zhong-Min Su
The Journal of Physical Chemistry C 2011 Volume 115(Issue 38) pp:18545-18551
Publication Date(Web):August 24, 2011
DOI:10.1021/jp2069336
Trumpet-shaped carbon nanocone (CNC) is used as a π-conjugated bridge to design high-performance nonlinear optical (NLO) material. Owing to the attractive trumpet-shaped structure, O2N–CNC–NH2 exhibits nonlinear optical behavior that is both surprisingly and qualitatively distinct from conventional π-conjugated organic species. It has been shown that the electron-acceptor nitryl (−NO2) at the apex of the trumpet and the electron-donor amino (−NH2) at the bottom edge of the trumpet to form O2N–CNC–NH2 is beneficial to improve the NLO response of CNC. Significantly, the first hyperpolarizabilities (βtot) of O2N–CNC–NH2 show an arc-shaped change as −NH2 substituting different H atoms along the arc-shaped bottom edge of CNC. Interestingly, the βtot values of H–CNC–NH2 also show an arc-shaped change. By comparison of the βtot values of O2N–CNC–NH2 and H–CNC–NH2, it has been found that no matter which bottom H of H–CNC–H is substituted by NH2, the βtot value of H–CNC–NH2 will be increased about 1.6 times after substituting the top H with −NO2 into the corresponding molecule. This study may stimulate the search for new types of NLO materials based on CNC for application.
Co-reporter:Dr. Rong-Lin Zhong;Dr. Ji Zhang;Dr. Shabbir Muhammad;Dr. Yang-Yang Hu;Dr. Hong-Liang Xu; Zhong-Min Su
Chemistry - A European Journal 2011 Volume 17( Issue 42) pp:11773-11779
Publication Date(Web):
DOI:10.1002/chem.201101430

Abstract

On the basis of the famous staggered biphenalenyl diradical π dimer 1, the eclipsed biphenalenyl (1 a), with no centrosymmetry, was obtained by rotating a layer of 1 by 60° around its central axis. Furthermore, the central carbon atoms of 1 and 1 a were substituted by boron and nitrogen atoms to form 2 and 2 a with a novel 2e–12c bond. We found that the novel 2e–12c bond is formed by the electron pair of the occupied orbital of the phenalenyl monomer substituted by the nitrogen atom and the unoccupied orbital of the phenalenyl monomer substituted by the boron atom. As a result of the novel 2e–12c bond, 2 and 2 a exhibit a fascinating interlayer charge-transfer transition character, which results in a significant difference in the dipole moments (Δμ) between the ground state and the crucial excited state. The values of Δμ for 2 and 2 a are 6.4315 and 6.9253 Debye, clearly larger than the values of 0 and 0.0015 Debye for 1 and 1 a. Significantly, the boron/nitrogen substitution effect can greatly enhance the first hyperpolarizabilities (β0) of 2 and 2 a with a novel 2e–12c bond compared with 1 and 1 a with a traditional 2e–12c bond: 0 and 19 a.u. for 1 and 1 a are much lower than 3516 and 12272 a.u. for 2 and 2 a. Furthermore, the interaction energies (Eint)of 2 and 2 a are larger than those of 1 and 1 a, which could be considered as a signature of reliability for the newly designed dimers. Our present work will be beneficial for further theoretical and experimental studies on the properties of molecules with the novel 2e–12c bond.

Co-reporter:Shabbir Muhammad, Abdullah G. Al-Sehemi, Zhongmin Su, Hongliang Xu, Ahmad Irfan, Aijaz Rasool Chaudhry
Journal of Molecular Graphics and Modelling (March 2017) Volume 72() pp:58-69
Publication Date(Web):March 2017
DOI:10.1016/j.jmgm.2016.12.009
Co-reporter:Rong-Lin Zhong, Hong-Liang Xu, Shabbir Muhammad, Ji Zhang and Zhong-Min Su
Journal of Materials Chemistry A 2012 - vol. 22(Issue 5) pp:NaN2202-2202
Publication Date(Web):2011/12/15
DOI:10.1039/C1JM14358A
Excess electron compounds have been proposed to be novel candidates of high-performance nonlinear optical (NLO) materials because of their large static first hyperpolarizabilities (β0). To enhance the stability of an unstable excess electron compound (LiCN⋯Li) with an extremely large β0 value (310196 a.u.), we designed a boron nitride nanotube (BNNT) as a protective shield molecule to encapsulate it (in theory). The stability of LiCN⋯Li was enhanced: the vertical ionization potentials (VIP) of LiCN⋯Li increased after encapsulating. Therefore, by comparison with LiCN⋯Li, the encapsulated complexes are more difficult to oxidize. Significantly, the BNNT encapsulated LiCN⋯Li complex exhibits a considerable β0 value (10645 a.u.), which is significantly (almost 380 times) larger than 28 a.u. of BNNT. Our further investigations into the intrinsic hyperpolarizabilites (βint) of these compounds show that there are clearly dependencies of the NLO response on the transition energy. Furthermore, it is easy to encapsulate LiCN⋯Li from the B-rich edge rather than N-rich edge of BNNT due to the lower energy barrier, which makes our calculations more useful to experimentalists who may try to synthesize these compounds. Knowledge of the encapsulation process of LiCN⋯Li within BNNT provides a new strategy for the design and synthesis of stable high-performance NLO materials.
Co-reporter:Li-Jie Wang, Rong-Lin Zhong, Shi-Ling Sun, Hong-Liang Xu, Xiu-Mei Pan and Zhong-Min Su
Dalton Transactions 2014 - vol. 43(Issue 25) pp:NaN9660-9660
Publication Date(Web):2014/03/10
DOI:10.1039/C3DT53329H
Recently, a new sulfide cluster fullerene, Sc2S@Cs (10528)-C72 containing two pairs of fused pentagons has been isolated and characterized (Chen et al., J. Am. Chem. Soc., 2012, 134, 7851). Inspired by this investigation, we propose a question: what properties will be influenced by the interaction between the encapsulated V-shaped polar molecule and C72? To answer this question, four encapsulated metallic fullerenes (EMFs) M2N@C72 (M = Sc or Y, N = S or O) along with pristine Cs-C72 (10528) were investigated by quantum chemistry methods. The results show that the Egap (3.01–3.14 eV) of M2N@C72 are significantly greater than that of pristine Cs-C72 (10528) (2.34 eV). This indicates that the stabilities of these EMFs increase by encapsulating the V-shaped polar molecule into the fullerene. Furthermore, the natural bond orbital (NBO) charge analysis indicates electron transfer from M2N to C72 cage, which plays a crucial role in enhancing first hyperpolarizability (βtot). The βtot follows the order of 1174 au (Y2O@C72) ≈ 1179 au (Sc2O@C72) > 886 au (Y2S@C72) ≈ 864 au (Sc2S@C72) > 355 au (C72). This indicates that the βtot of M2N@C72 is more remarkable than that of pristine Cs-C72 (10528) due to the induction effect of the encapsulated molecule. Compared with sulfide cluster fullerenes (Y2S@C72 and Sc2S@C72), oxide cluster fullerenes (Sc2O@C72 and Y2O@C72) show much larger βtot due to the small ionic radius and the large electronegativity of oxygen. In contrast, the metal element (scandium and yttrium) has a slight influence on the βtot. Thus, oxide cluster fullerenes are candidates to become promising nonlinear optical materials with higher performance.
Co-reporter:Rong-Lin Zhong, Hong-Liang Xu and Zhong-Min Su
Physical Chemistry Chemical Physics 2016 - vol. 18(Issue 20) pp:NaN13959-13959
Publication Date(Web):2016/04/20
DOI:10.1039/C6CP00647G
Carbon–boron–nitride heteronanotubes (BNCNT) have attracted a lot of attention because of their adjustable properties and potential applications in many fields. In this work, a series of CA, PA and HA armchair BNCNT models were designed to explore their nonlinear optical (NLO) properties and provide physical insight into the structure–property relationships; CA, PA and HA represent the models that are obtained by doping the carbon segment into pristine boron nitride nanotube (BNNT) fragments circularly around the tube axis, parallel to the tube axis and helically to the tube axis, respectively. Results show that the first hyperpolarizability (β0) of an armchair BNCNT model is dramatically dependent on the connecting patterns of carbon with the boron nitride fragment. Significantly, the β0 value of PA-6 is 2.00 × 104 au, which is almost two orders of magnitude larger than those (6.07 × 102 and 1.55 × 102 au) of HA-6 and CA-6. In addition, the β0 values of PA and CA models increase with the increase in carbon proportion, whereas those of HA models show a different tendency. Further investigations on transition properties show that the curved charge transfer from N-connecting carbon atoms to B-connecting carbon atoms of PA models is essentially the origin of the big difference among these models. This new knowledge about armchair BNCNTs may provide important information for the design and preparation of advanced NLO nano-materials.
Co-reporter:Sa Chen, Shi-Ling Sun, Heng-Qing Wu, Hong-Liang Xu, Liang Zhao and Zhong-Min Su
Dalton Transactions 2014 - vol. 43(Issue 33) pp:NaN12662-12662
Publication Date(Web):2014/06/02
DOI:10.1039/C4DT01240B
Recently, the well-known phenalenyl radical π-dimer with its fascinating 2-electron/12-center (2e/12c) bond has attracted our attention. In this work, we designed two molecules, Li3O⋯C13H9 (1a) and BeF3⋯C13H9 (1b). Interestingly, owing to the inductive effect of superatoms, an electron is transferred from Li3O to phenalenyl in 1a, while an electron is transferred from phenalenyl to BeF3 in 1b. Further, we employed 1a and 1b as building blocks to assemble two novel molecules with 2e/12c bonds: Li3O⋯(C13H9)2⋯BeF3 (2a) and Li3O⋯(C13H9)2⋯BeF3 (2b). Remarkably, 2a and 2b with novel 2e/12c bonds exhibit a dramatic interlayer charge-transfer character, which results in a significant difference of dipole moments (Δμ: 2.6804 for 2a and 3.8019 Debye for 2b) between the ground state and the crucial excited state. As a result, the static first hyperpolarizabilities (β0: 5154 for 2a and 12500 au for 2b) are considerably larger than the values of 347 for 1a and 328 au for 1b. It is our expectation that the results of the present work might provide beneficial information for further theoretical and experimental studies on the fascinating properties of molecules with interlayer charge-transfer character.
Copper tin zinc sulfide
3H-Indole, 3,3-dimethyl-2-[(1E)-2-(2,3,5,6,8,9,11,12-octahydro-1,4,7,10,13-benzopentaoxacyclopentadecin-15-yl)ethenyl]-
Lithium oxide (Li3O)(9CI)
ACETYLENE
Phenalenyl