Co-reporter:Jessica L. Davis, Aaron M. Chalifoux, and Stephanie L. Brock
Langmuir September 19, 2017 Volume 33(Issue 37) pp:9434-9434
Publication Date(Web):June 21, 2017
DOI:10.1021/acs.langmuir.7b01118
Oxidative assembly of metal chalcogenide nanocrystals (NCs) enables the formation of 2-D (dense) and 3-D porous structures without the presence of intervening ligands between particles that can moderate transport properties. This route has been demonstrated to be successful for a range of single-component structures including CdQ, PbQ, and ZnQ (Q = S, Se, Te). En route to the controllable assembly of multicomponent nanostructures, the roles of Q redox properties (2Q2– → Q22– + 2e) responsible for particle cross-linking and the native structure (cubic zinc blende vs hexagonal wurtzite) in the kinetics of assembly in single-component CdQ NCs are evaluated using time-resolved dynamic light scattering (TR-DLS). For wurtzite CdQ, the rates follow the ease of oxidation, with telluride as the fastest, followed by selenide and sulfide. However, when comparing CdS wurtzite (w) and zinc blende (zb), the cubic NCs exhibit surprisingly slow kinetics. NMR studies reveal the zb structure to have lower ligand coverage (by a factor of 4) relative to that of w, and the formation of free disulfide (the product of ligand oxidation) is slow. This is attributed to differences in the surface energies of w and zb facets, with w having polar (0001) facets of high energy compared to the neutral facets of the zb structure. The zb-CdS NCs prepared by low-temperature synthesis methods are likely to suffer from surface defects that may moderate reactivity. EPR studies suggest that zb-CdS has paramagnetic sulfur vacancies not present in w-CdS. These data suggest that structure plays an unexpectedly large role in the kinetics of CdQ NC oxidative assembly, providing a useful lever to moderate activities in multicomponent assemblies.
Co-reporter:Indika K. Hewavitharana and Stephanie L. Brock
ACS Nano November 28, 2017 Volume 11(Issue 11) pp:11217-11217
Publication Date(Web):October 16, 2017
DOI:10.1021/acsnano.7b05534
This study demonstrates that ligand exchange of nanocrystals (NCs) is not always an innocuous process, but can lead to facile (room temperature) ion exchange, depending on the surface crystal faceting. Rock salt PbTe NCs prepared as cubes with neutral facets undergo room-temperature ligand exchange with sulfide ions, whereas cuboctahedron-shaped particles with neutral {100} and polar {111} facets are transformed to PbS, driven by ion exchange along the ⟨111⟩ direction. Likewise, cation exchange (with Ag+) occurs rapidly for cuboctahedra, whereas cubes remain inert. This dramatic difference is attributed to the relative surface area of {111} facets that promote rapid ion exchange and shows how facet engineering is a powerful knob for the control of reaction pathways in nanoparticles.Keywords: cube-shape; cuboctahedron-shape; fcc; lead telluride; reaction control; surface energy;
Co-reporter:D. Ruchira Liyanage;Da Li;Quintin B. Cheek;Habib Baydoun
Journal of Materials Chemistry A 2017 vol. 5(Issue 33) pp:17609-17618
Publication Date(Web):2017/08/22
DOI:10.1039/C7TA05353C
Aiming to create an efficient, less-expensive catalyst for the oxygen evolution reaction (OER), a synthetic protocol is developed to prepare ternary metal phosphide nanoparticles, Ni2−xRuxP, incorporating Ru, a traditional catalyst for OER, and Ni, a highly active but inexpensive metal. Using solution-phase arrested-precipitation reactions, crystalline Ni2−xRuxP particles could be realized for compositions up to x ≤ 1, whereas more Ru-rich compositions, including Ru2P, were amorphous. For x ≤ 1, particles are spherical, of sizes that vary between 5 and 10 nm in diameter (with a clear decreasing trend as the Ru amount is increased), and samples exhibit narrow size distributions (polydispersity < 15%). In contrast, amorphous Ru-rich phases exhibit worm-like morphologies. ICP-MS data indicate the actual metal ratio closely follows the target ratio employed in the synthesis. OER electrocatalytic activity was evaluated for selected compositions over the entire synthesis range (0 ≤ x ≤ 2). Intriguingly, Ru2P proved to be the least active phase (overpotential of 0.56 V at 10 mA cm−2 in 1.0 M KOH) with the best performance observed for the bimetallic Ni1.25Ru0.75P phase (overpotential of 0.34 V). The augmented activity at x = 0.75 is attributed, at least in part, to electronic activation of Ni by Ru, facilitating Ni oxidation and thus decreasing the kinetic barrier for OER.
Co-reporter:Lasantha Korala;Jason R. Germain;Erica Chen;Irina R. Pala;Da Li
Inorganic Chemistry Frontiers 2017 vol. 4(Issue 9) pp:1451-1457
Publication Date(Web):2017/09/12
DOI:10.1039/C7QI00140A
Synthesis of efficient photocatalysts based on CdS nanomaterials for oxidative decomposition of organic effluents typically focuses on (a) enhancement of surface area of the catalysts and (b) promotion of the separation of photogenerated electron–hole pairs. CdS aerogel, which are synthesized by simple sol–gel assembly of discrete nanocrystals (NCs) into a porous network followed by supercritical drying, could provide higher surface area for photocatalytic reactions along with facile charge separation due to direct contact between NCs via covalent bonding. We evaluated the efficiency of CdS aerogel materials for degradation of organic dyes using methylene blue (MB) and methyl orange (MO) as test cases. CdS aerogel materials exhibited remarkable photocatalytic activity for dye degradation compared to typical, ligand-capped CdS NCs. The catalytic efficiency of CdS aerogels was further improved by decreasing the chain-length and extent of surface organics, leading to higher, and more hydrophilic, accessible surface area. The use of porous, chalcogenide-based solid state architectures for photocatalysis enables easy separation of catalyst while ensuring a high-interfacial surface area for analyte reactivity and visible light activation.
Co-reporter:Roshini Pimmachcharige;Yanhua Zhang;Rajesh Regmi;Gavin Lawes
Journal of Materials Chemistry C 2017 vol. 5(Issue 13) pp:3352-3358
Publication Date(Web):2017/03/30
DOI:10.1039/C7TC00579B
MnAs exhibits a large magnetocaloric effect associated with the first-order phase transition at 315 K, making it a promising phase for near-room-temperature magnetic refrigeration technologies. Optimization of the properties to expand the temperature range of operation (by adjusting the phase transition temperature) and reduce hysteresis losses can be achieved by phosphorus-doping and nanostructuring, respectively. The synthesis of P-doped MnAs as discrete nanoparticles by rapid injection synthesis has been previously reported, but suffers from extensive polydispersity and an inability to independently control size and dopant concentration. In the present work, a kinetic analysis of the P-doped MnAs nanoparticle formation by temporal correlation of particle volume, P-dopant concentration, and particle size to monomer concentration, is undertaken. Narrow polydispersity samples can only be obtained by rapid quenching from the reaction temperature, achieved by injection of the hot solution into cold chloroform; cooling in the flask leads to polydispersity characteristic of Ostwald ripening. When isolated at high temperature, particles initially grow at high monomer concentrations, achieving volumes of ca. 740 nm3 by 10 min, and then decrease in volume by more than a factor of two by 30 min reaction time, at which point both the size and residual monomer concentration (ca. 20%) remain constant, suggesting formation of an equilibrium or an unreactive byproduct. Simultaneously, the concentration of P incorporated is found to decrease over the time of the reaction from 5–7% initially to a nearly constant concentration of <2% by 60 min. These data suggest that P is incorporated preferentially at the nucleation stage, but is lost over time. This detailed understanding of MnAs particle formation and P-inclusion enables independent assessment of the role of size, polydispersity, and dopant concentration on magnetic properties.
Co-reporter:Da Li; Habib Baydoun; Cláudio N. Verani
Journal of the American Chemical Society 2016 Volume 138(Issue 12) pp:4006-4009
Publication Date(Web):March 13, 2016
DOI:10.1021/jacs.6b01543
The development of efficient water oxidation catalysts based on inexpensive and Earth-abundant materials is a prerequisite to enabling water splitting as a feasible source of alternative energy. In this work, we report the synthesis of ternary cobalt manganese phosphide nanoparticles from the solution-phase reaction of manganese and cobalt carbonyl complexes with trioctylphosphine. The CoMnP nanoparticles (ca. 5 nm in diameter) are nearly monodisperse and homogeneous in nature. These CoMnP nanoparticles are capable of catalyzing water oxidation at an overpotential of 0.33 V with a 96% Faradaic efficiency when deposited as an ink with carbon black and Nafion. A slight decrease in activity is observed after 500 cycles, which is ascribed to the etching of P into solution, as well as the oxidation of the surface of the nanoparticles. Manganese-based ternary phosphides represent a promising new system to explore for water oxidation catalysis.
Co-reporter:Da Li, Maheshika P. Arachchige, Bogdan Kulikowski, Gavin Lawes, Takele Seda, and Stephanie L. Brock
Chemistry of Materials 2016 Volume 28(Issue 11) pp:3920
Publication Date(Web):May 10, 2016
DOI:10.1021/acs.chemmater.6b01185
In this work, a solution-phase method was developed for the synthesis of CoxFe2–xP nanoparticles over all x (0 ≤ x ≤ 2). The nanoparticles vary in size, ranging from 17 to 20 nm in diameter with standard deviations ≤ 14%. The synthesis involves preparation of CoxFe1–x alloy nanoparticles and high temperature conversion into crystalline ternary phosphide nanocrystals. The target composition can be controlled by the initial metal precursor ratio, and the size of CoxFe2–xP (from 12 to 22 nm) can be tuned by varying the oleylamine/metal ratio. Mössbauer data show that Fe has a strong preference for the square pyramidal site over the tetrahedral site. Magnetic measurements on CoxFe2–xP nanoparticles showed a strong compositional dependence of the Curie temperature (TC); CoFeP and Co0.7Fe0.3P have TC’s > 340 K and are superparamagnetic at room temperature.
Co-reporter:Malsha A. Hettiarachchi, Ehab Abdelhamid, Boris Nadgorny and Stephanie L. Brock
Journal of Materials Chemistry A 2016 vol. 4(Issue 28) pp:6790-6797
Publication Date(Web):20 Jun 2016
DOI:10.1039/C6TC01478J
A solution phase methodology was developed for the formation of discrete colloidal MnSb nanoparticles using dimanganesedecacarbonyl and triphenylantimony as the main reaction components. Stoichiometric reactions result in significant Sb impurities, but these can be eliminated by the use of excess Mn reagent, limiting the reaction time, and using a lower temperature (280 °C) relative to that commonly employed for MnP or MnAs synthesis (330–360 °C). The resultant MnSb nanoparticles are, when evidenced by both powder X-ray diffraction and transmission electron microscopy, ca. 14 nm in diameter and exhibit low polydispersity (13 ± 1.7 nm). High Angle Annular Dark Field-Scanning Transmission Electron Microscopy and energy dispersive line scan data revealed that the as-synthesized MnSb nanoparticles are core–shell in nature, having a MnSb core and an amorphous manganese oxide shell. Evidence is presented supporting a pathway for decomposition of MnSb nanoparticles driven by formation of MnO2 and Sb due to reaction with adventitious O2. The MnSb nanoparticles are superparamagnetic at room temperature, and exhibit suppressed moments attributed to surface oxidation arising from the high surface area and intrinsic oxophilicity of Mn.
Co-reporter:Samuel J. Danforth, D. Ruchira Liyanage, Asha Hitihami-Mudiyanselage, Boris Ilic, Stephanie L. Brock, Mark E. Bussell
Surface Science 2016 Volume 648() pp:126-135
Publication Date(Web):June 2016
DOI:10.1016/j.susc.2015.10.005
•Encapsulated nanoparticles provide a well-defined system for probing the fundamental HDS properties of metal phosphides.•The HDS turnover frequencies of nickel-rich Ni2-xMxP@mSiO2 nanocatalysts increase with increasing Co and Fe content.•IR spectral studies of adsorbed CO on Ni2-xMxP@mSiO2 nanocatalysts indicate electron transfer from Co and Fe to Ni sites.Metal phosphide nanoparticles encapsulated in mesoporous silica provide a well-defined system for probing the fundamental chemistry of the hydrodesulfurization (HDS) reaction over this new class of hydrotreating catalysts. To investigate composition effects in bimetallic phosphides, the HDS of dibenzothiophene (DBT) was carried out over a series of Ni-rich Ni2-xMxP@mSiO2 (M = Co, Fe) nanocatalysts (x ≤ 0.50). The Ni2-xMxP nanoparticles (average diameters: 11–13 nm) were prepared by solution-phase arrested precipitation and encapsulated in mesoporous silica, characterized by a range of techniques (XRD, TEM, IR spectroscopy, BET surface area, CO chemisorption) and tested for DBT HDS activity and selectivity. The highest activity was observed for a Ni1.92Co0.08P@mSiO2 nanocatalyst, but the overall trend was a decrease in HDS activity with increasing Co or Fe content. In contrast, the highest turnover frequency (TOF) was observed for the most Co- and Fe-rich compositions based on sites titrated by CO chemisorption. IR spectral studies of adsorbed CO on the Ni2-xMxP@mSiO2 catalysts indicate that an increase in electron density occurs on Ni sites as the Co or Fe content is increased, which may be responsible for the increased TOFs of the catalytic sites. The Ni2-xMxP@mSiO2 nanocatalysts exhibit a strong preference for the direct desulfurization pathway (DDS) for DBT HDS that changes only slightly with increasing Co or Fe content.
Co-reporter:D. Ruchira Liyanage, Samuel J. Danforth, Yi Liu, Mark E. Bussell, and Stephanie L. Brock
Chemistry of Materials 2015 Volume 27(Issue 12) pp:4349
Publication Date(Web):May 20, 2015
DOI:10.1021/acs.chemmater.5b00958
A synthetic protocol developed to produce phase-pure, nearly monodisperse Ni2–xCoxP nanoparticles (x ≤ 1.7) is described. The Ni2–xCoxP particles vary in size, ranging from 9–14 nm with standard deviations of <20% (based on transmission electron microscopy analysis), and the actual metal ratios obtained from energy-dispersive spectroscopy closely follow the targeted ratios. With increasing Co, samples with larger size distributions are obtained and include particles with voids, attributed to the Kirkendall effect. To probe the mechanism of ternary phosphide particle formation, detailed studies were conducted for Ni:Co = 1:1 as a representative composition. It was revealed that the P:M ratio, heating temperature, and heating time have a large impact on the nature of both intermediate and final crystalline particles formed. By tuning these conditions, nanoparticles can be produced with different sizes (from ca. 7–25 nm) and morphologies (hollow versus dense).
Co-reporter:Asha Hitihami-Mudiyanselage, Maheshika Palihawadana Arachchige, Takele Seda, Gavin Lawes, and Stephanie L. Brock
Chemistry of Materials 2015 Volume 27(Issue 19) pp:6592
Publication Date(Web):September 11, 2015
DOI:10.1021/acs.chemmater.5b02149
Ternary FexNi2–xP (0 < x < 2) phases exhibit a range of useful properties that can be augmented or tuned by confinement to the nanoscale including hydrotreating catalytic activity for small x and near-room temperature ferromagnetism for high x. In this work, a solution-phase arrested-precipitation method was developed for the synthesis of FexNi2–xP over all values of x (0 < x < 2). The synthesis involves preparation of Ni–P amorphous particles, introduction of the Fe precursor to form amorphous Fe–Ni–P particles, and high-temperature conversion of Fe–Ni–P particles into crystalline ternary phosphide nanocrystals. The ternary FexNi2–xP nanocrystals crystallize in the hexagonal Fe2P-type structure, and the morphology of the nanocrystals showed a distinct compositional dependence, transitioning from about 11 nm diameter spheres to rods with aspect ratios approaching 2 as the Fe fraction is increased (x ≥ 1.2). Lattice parameters do not follow Vegard’s law, consistent with Mössbauer data showing preferential site occupation by Fe of the tetrahedral over the square pyramidal sites at low Fe concentrations, and the opposite effect for x > 0.8. Magnetic measurements of FexNi2–xP (x = 1.8, 1.4, and 1.2) nanorods showed a strong compositional dependence of the Curie temperature (TC) that differs from observations in bulk phases, with the highest TC (265 K) obtained for x = 1.4.
Co-reporter:Derak J. James, Xu Lu, Donald T. Morelli, and Stephanie L. Brock
ACS Applied Materials & Interfaces 2015 Volume 7(Issue 42) pp:23623
Publication Date(Web):October 19, 2015
DOI:10.1021/acsami.5b07141
Derivatives of synthetic tetrahedrite, Cu12Sb4S13, are receiving increasing attention in the thermoelectric community due to their exploitation of plentiful, relatively nontoxic elements, combined with a thermoelectric performance that rivals that of PbTe-based compounds. However, traditional synthetic methods require weeks of annealing at high temperatures (450–600 °C) and periodic regrinding of the samples. Here we report a solvothermal method to produce tetrahedrite that requires only 1 day of heating at a relatively low temperature (155 °C). This allows preparation of multiple samples at once and is potentially scalable. The solvothermal material described herein demonstrates a dimensionless figure of merit (ZT) vs temperature curve comparable to that of solid-state tetrahedrite, achieving the same ZT of 0.63 at ∼720 K. As with the materials from solid-state synthesis, products from this rapid solvothermal synthesis can be improved by mixing in a 1:1 molar ratio with the Zn-containing natural mineral, tennantite, to achieve 0.9 mol equiv of Zn. This leads to a 36% increase in ZT at ∼720 K for solvothermal tetrahedrite, to 0.85.Keywords: Cu12Sb4S13; mineral; tennantite; zinc doping; ZT
Co-reporter:Da Li; Keerthi Senevirathne; Lance Aquilina
Inorganic Chemistry 2015 Volume 54(Issue 16) pp:7968-7975
Publication Date(Web):August 4, 2015
DOI:10.1021/acs.inorgchem.5b01125
Due to their unique catalytic, electronic, and redox processes, Ni5P4 and NiP2 nanoparticles are of interest for a wide-range of applications from the hydrogen evolution reaction to energy storage (batteries); yet synthetic approaches to these materials are limited. In the present work, a phase-control strategy enabling the arrested-precipitation synthesis of nanoparticles of Ni5P4 and NiP2 as phase-pure samples using different Ni organometallic precursors and trioctylphosphine (TOP) is described. The composition and purity of the product can be tuned by changing key synthetic levers, including the Ni precursor, the oleylamine (OAm) coordinating solvent and TOP concentrations, temperature, time, and the presence or absence of a moderate temperature soak step to facilitate formation of Ni and/or Ni–P amorphous nanoparticle intermediates. Notably, the 230 °C intermediate step favors the ultimate formation of Ni2P and hinders further phosphidation to form Ni5P4 or NiP2 as phase-pure products. In the absence of this step, increasing the P/Ni ratio (13–20), reaction temperature (350–385 °C), and time (10–48 h) favors more P-rich phases, and these parameters can be adjusted to generate either Ni5P4 or NiP2. The phase of the obtained particles can also be tuned between pure Ni2P to Ni5P4 and NiP2 by simply decreasing the OAm/TOP ratio and/or changing the nickel precursor (nickel(II)acetylacetonate, nickel(II)acetate tetrahydrate, or bis(cyclooctadiene)nickel(0)). However, at high concentrations of OAm, the product formed is the same regardless of Ni precursor, suggesting the formation of a uniform Ni intermediate (an Ni-oleylamine complex) under these conditions that is responsible for product distribution. Intriguingly, under the extreme phosphidation conditions required to favor Ni5P4 and NiP2 over Ni2P (large excess of TOP), the 20–30 nm crystallites assemble into supraparticles with diameters of 100–500 nm. These factors are discussed in light of a comprehensive synthetic scheme utilized to control P incorporation in nickel phosphides.
Co-reporter:Derak James
The Journal of Physical Chemistry C 2015 Volume 119(Issue 9) pp:4635-4644
Publication Date(Web):February 11, 2015
DOI:10.1021/jp5127046
Design of thermoelectric materials focuses on the optimization of several unfavorably coupled factors: electrical conductivity, Seebeck coefficient, and thermal conductivity. Recent work in thermoelectrics has focused on decreasing lattice thermal conductivity by nanostructuring thermoelectric materials, while recent work in photovoltaics has demonstrated ligand stripping as a means to increased electron mobility in thin films of nanoparticles. In the present work, these two features are combined. A multigram scale synthesis of dispersible, lead telluride nanocrystals (25–50 nm) is developed using hot-injection methods in common organic solvents. These nanocrystals (NCs) are ligand stripped with sulfide (PbTe-S) or iodide (PbTe-I) sources to result in p-type or n-type materials with large Seebeck coefficients at room temperature of 520 or −540 μV·K–1, respectively. Sequential stripping with sulfide and then iodide (PbTe-SI) resulted in a small Seebeck due to counter doping. PbTe-S and PbTe-SI are found to generate nanostructured composites by growth of lead sulfide nanocrystals (∼50–60 nm) in situ upon annealing. However, the electrical conductivities are low (<1 S·cm–1) due to excess doping during the ligand stripping. Intentional formation of a nanocomposite (PbTe–PbS) is achieved by combining PbTe NCs with 4–6 nm diameter lead sulfide particles via mixing by incipient wetness with a target of 8 mol % lead sulfide. The resulting nanocomposite is n-type with a Seebeck coefficient of −160 μV·K–1 and an electrical conductivity of 42 S·cm–1 at room temperature. The lattice thermal conductivities of all materials at room temperature are substantially lower than those of bulk lead telluride (2.0 W m–1·K–1). However, thermoelectric figure of merit (ZT) values are low for all samples (maximum ZT = 0.03 for PbTe–PbS), attributed primarily to the low electrical conductivities. This work underscores the importance of developing new methods for augmenting electrical conductivity if nanoparticle assemblies are to be practically employed in thermoelectrics.
Co-reporter:Asha Hitihami-Mudiyanselage, Keerthi Senevirathne, and Stephanie L. Brock
Chemistry of Materials 2014 Volume 26(Issue 21) pp:6251
Publication Date(Web):October 17, 2014
DOI:10.1021/cm5030958
The synthesis of Ni2P nanoparticle three-dimensional architectures using two different approaches is reported. The oxidation-induced sol–gel method involves chemical oxidation of surface phosphorus to form P–O–P linkages between particles in the gel network, similar to the mechanism originally reported for InP nanoparticles. The second method, metal-assisted gelation, occurs by cross-linking of pendant carboxylate functionalities on surface-bound thiolate ligands via metal ions to yield an interconnected particle network. The method of gel network formation can be tuned by changing the surface ligand terminal functionalities and the nature (oxygen-transferring or non-oxygen-transferring) of the oxidant. Both methods produce porous, high surface area materials with thermal stabilities above 400 °C.
Co-reporter:Yanhua Zhang, Rajesh Regmi, Yi Liu, Gavin Lawes, and Stephanie L. Brock
ACS Nano 2014 Volume 8(Issue 7) pp:6814
Publication Date(Web):June 3, 2014
DOI:10.1021/nn501149s
Small changes in the synthesis of MnAs nanoparticles lead to materials with distinct behavior. Samples prepared by slow heating to 523 K (type-A) exhibit the characteristic magnetostructural transition from the ferromagnetic hexagonal (α) to the paramagnetic orthorhombic (β) phase of bulk MnAs at Tp = 312 K, whereas those prepared by rapid nucleation at 603 K (type-B) adopt the β structure at room temperature and exhibit anomalous magnetic properties. The behavior of type-B nanoparticles is due to P-incorporation (up to 3%), attributed to reaction of the solvent (trioctylphosphine oxide). P-incorporation results in a decrease in the unit cell volume (∼1%) and shifts Tp below room temperature. Temperature-dependent X-ray diffraction reveals a large region of phase-coexistence, up to 90 K, which may reflect small differences in Tp from particle-to-particle within the nearly monodisperse sample. The large coexistence range coupled to the thermal hysteresis results in process-dependent phase mixtures. As-prepared type-B samples exhibiting the β structure at room temperature convert to a mixture of α and β after the sample has been cooled to 77 K and rewarmed to room temperature. This change is reflected in the magnetic response, which shows an increased moment and a shift in the temperature hysteresis loop after cooling. The proportion of α present at room temperature can also be augmented by application of an external magnetic field. Both doped (type-B) and undoped (type-A) MnAs nanoparticles show significant thermal hysteresis narrowing relative to their bulk phases, suggesting that formation of nanoparticles may be an effective method to reduce thermal losses in magnetic refrigeration applications.Keywords: anion doping; first-order phase transition; magnetic refrigeration; magnetocaloric effect; manganese arsenide
Co-reporter:Galbokka H. Layan Savithra, Elayaraja Muthuswamy, Richard H. Bowker, Bo A. Carrillo, Mark E. Bussell, and Stephanie L. Brock
Chemistry of Materials 2013 Volume 25(Issue 6) pp:825
Publication Date(Web):February 28, 2013
DOI:10.1021/cm302680j
The size-dependent catalytic activity of Ni2P for hydrodesulfurization (HDS) remains unstudied because the traditional temperature programmed reduction (TPR) method used in catalyst preparation results in highly polydisperse Ni2P particles. The ability to control the Ni2P particle size in the range 5–20 nm by varying the quantity of oleylamine in solution-phase arrested precipitation reactions is reported. Particles were introduced to a high surface area silica support (Cab-O-Sil, M-7D grade, 200 m2/g) via incipient wetness, and HDS activity was probed against dibenzothiophene (DBT). All samples were less active than TPR prepared materials, and the smallest particles were the least active, contrary to expectation. This is attributed in part to particle sintering under HDS conditions. Sintering occurs independently of wt% loading of catalyst, time, incipient wetness procedure, and ionic additives, at all temperatures greater than 200 °C. Sintering is minimized by encapsulation of Ni2P nanoparticles in a mesoporous silica shell, achieved by sol–gel silica formation around Ni2P-containing surfactant liquid crystal assemblies and subsequent calcination, resulting in a doubling of HDS activity.Keywords: hydrodesulfurization; mesoporous silica shell; Ni2P nanoparticles; sintering; supported catalyst;
Co-reporter:Galbokka H. Layan Savithra, Richard H. Bowker, Bo A. Carrillo, Mark E. Bussell, and Stephanie L. Brock
ACS Applied Materials & Interfaces 2013 Volume 5(Issue 12) pp:5403
Publication Date(Web):June 7, 2013
DOI:10.1021/am402003g
The synthesis of monodisperse 5–10 nm Pd5P2 catalytic particles by encapsulation in a mesoporous silica network, along with preliminary data on hydrodesulfurization (HDS) activity, is reported. Precursor Pd–P amorphous nanoparticles are prepared by solution-phase reaction of palladium(II) acetylacetonate with trioctylphosphine at temperatures up to 300 °C. Direct crystallization of Pd5P2 in solution by increasing the temperature to 360 °C leads to sintering, but particle size can be maintained during the transformation by encapsulation of the amorphous Pd–P particles in a mesoporous silica shell, followed by treatment of the solid at 500 °C under a reducing atmosphere, yielding Pd5P2@mSiO2. The resultant materials exhibit high BET surface areas (>1000 m2/g) and an average pore size of 3.7 nm. Access to the catalyst surface is demonstrated by dibenzodithiophene (DBT) HDS testing. Pd5P2@mSiO2 shows a consistent increase in HDS activity as a function of temperature, with DBT conversion approaching 60% at 402 °C. The ability to control particle size, phase, and sintering is expected to enable the fundamental catalytic attributes that underscore activity in Pd5P2 to be assessed.Keywords: dibenzothiophene; HDS catalysis; mesoporous silica; Pd5P2 nanoparticle synthesis; sintering prevention;
Co-reporter:Asha Hitihami-Mudiyanselage, Keerthi Senevirathne, and Stephanie L. Brock
ACS Nano 2013 Volume 7(Issue 2) pp:1163
Publication Date(Web):January 24, 2013
DOI:10.1021/nn305959q
The applicability of sol–gel nanoparticle assembly routes, previously employed for metal chalcogenides, to phosphides is reported for the case of InP. Two different sizes (3.5 and 6.0 nm) of InP nanoparticles were synthesized by solution-phase arrested precipitation, capped with thiolate ligands, and oxidized with H2O2 or O2/light to induce gel formation. The gels were aged, solvent-exchanged, and then supercritically dried to obtain aerogels with both meso- (2–50 nm) and macropores (>50 nm) and accessible surface areas of ∼200 m2/g. Aerogels showed higher band gap values relative to precursor nanoparticles, suggesting that during the process of assembling nanoparticles into 3D architectures, particle size reduction may have taken place. In contrast to metal chalcogenide gelation, InP gels did not form using tetranitromethane, a non-oxygen-transferring oxidant. The requirement of an oxygen-transferring oxidant, combined with X-ray photoelectron spectroscopy data showing oxidized phosphorus, suggests gelation is occurring due to condensation of phosphorus oxoanionic moieties generated at the interfaces. The ability to link discrete InP nanoparticles into a 3D porous network while maintaining quantum confinement is expected to facilitate exploitation of nanostructured InP in solid-state devices.Keywords: aerogels; gels; III−V semiconductors; InP; quantum confinement
Co-reporter:Lasantha Korala, Zhijie Wang, Yi Liu, Stephen Maldonado, and Stephanie L. Brock
ACS Nano 2013 Volume 7(Issue 2) pp:1215
Publication Date(Web):January 25, 2013
DOI:10.1021/nn304563j
Optoelectronic properties of quantum dot (QD) films are limited by (1) poor interfacial chemistry and (2) nonradiative recombination due to surface traps. To address these performance issues, sol–gel methods are applied to fabricate thin films of CdSe and core(shell) CdSe(ZnS) QDs. High-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM) imaging with chemical analysis confirms that the surface of the QDs in the sol–gel thin films are chalcogen-rich, consistent with an oxidative-induced gelation mechanism in which connectivity is achieved by formation of dichalcogenide covalent linkages between particles. The ligand removal and assembly process is probed by thermogravimetric, spectroscopic, and microscopic studies. Further enhancement of interparticle coupling via mild thermal annealing, which removes residual ligands and reinforces QD connectivity, results in QD sol–gel thin films with superior charge transport properties, as shown by a dramatic enhancement of electrochemical photocurrent under white light illumination relative to thin films composed of ligand-capped QDs. A more than 2-fold enhancement in photocurrent, and a further increase in photovoltage can be achieved by passivation of surface defects via overcoating with a thin ZnS shell. The ability to tune interfacial and surface characteristics for the optimization of photophysical properties suggests that the sol–gel approach may enable formation of QD thin films suitable for a range of optoelectronic applications.Keywords: ligand exchange; photocurrent; quantum dots; sol−gel methods; surface passivation
Co-reporter:Irina R. Pala and Stephanie L. Brock
ACS Applied Materials & Interfaces 2012 Volume 4(Issue 4) pp:2160
Publication Date(Web):March 15, 2012
DOI:10.1021/am3001538
ZnS nanoparticle (NP) gel networks were used as cation exchange materials for the removal of Pb2+ and Hg2+ from aqueous solutions. First, the suitability of the gel as a remediation material was studied by analyzing the mechanism of the cation exchange reaction. ZnS NP gels can exchange with other divalent cations (Pb2+, Hg2+) under mild reaction conditions. The speed of the reaction is influenced by the reduction potential of the incoming cation. The ZnS aerogels can remove Pb2+ and Hg2+ from aqueous solutions with a wide range of initial concentrations. For initial Pb2+ concentrations of 100 ppb, the Pb2+ concentration can be reduced below the action limit established by the EPA (15 ppb). Under thermodynamically forcing conditions, the water remediation capacity of the ZnS NP aerogels was determined to be 14.2 mmol Pb2+/ g ZnS aerogel, which is the highest value reported to date.Keywords: aerogel; cation exchange; metal contaminant; nanomaterials; water remediation;
Co-reporter:Lasantha Korala, Li Li and Stephanie L. Brock
Chemical Communications 2012 vol. 48(Issue 68) pp:8523-8525
Publication Date(Web):03 Jul 2012
DOI:10.1039/C2CC34188C
A method of fabricating sol–gel quantum dot (QD) films is demonstrated, and their optical, structural and electrical properties are evaluated. The CdSe(ZnS) xerogel films remain quantum confined, yet are highly conductive (10−3 S cm−1). This approach provides a pathway for the exploitation of QD gels in optoelectronic applications.
Co-reporter:Jilian N. De Freitas, Lasantha Korala, Luke X. Reynolds, Saif A. Haque, Stephanie L. Brock and Ana F. Nogueira
Physical Chemistry Chemical Physics 2012 vol. 14(Issue 43) pp:15180-15184
Publication Date(Web):12 Sep 2012
DOI:10.1039/C2CP42998E
CdSe(ZnS) core(shell) aerogels were prepared from the assembly of quantum dots into mesoporous colloidal networks. The sol–gel method produces inorganic particle interfaces with low resistance to electrical transport while maintaining quantum-confinement. The photoelectrochemical properties of aerogels and their composites with poly(3-hexylthiophene) are reported for the first time.
Co-reporter:Shreyashi Ganguly, Chen Zhou, Donald Morelli, Jeff Sakamoto, and Stephanie L. Brock
The Journal of Physical Chemistry C 2012 Volume 116(Issue 33) pp:17431-17439
Publication Date(Web):August 2, 2012
DOI:10.1021/jp3055608
The synthesis and characterization of Bi2Te3 and Bi2–xSbxTe3 aerogel materials, and the effect of gelation on thermoelectrically relevant properties, is reported. Aerogels are prepared from oxidation of discrete thiolate-capped nanoparticles to yield a wet gel, followed by supercritical CO2 drying. The resultant aerogels have surface areas between 36 and 45 m2/g. Characterization of the thermoelectric properties of hot-pressed pellets of Bi2Te3 aerogels suggested a decrease in lattice thermal conductivity with respect to the bulk materials, attributed to the effect of nanostructuring, but the power factor (S2σ) was also reduced due to the effect of adventitious doping. In the case of Bi2–xSbxTe3 aerogels, there was no change in the lattice thermal conductivity upon nanostructuring, but again the power factor was reduced with respect to bulk materials. This is attributed to the presence of excess tellurium, which led to compensation of the majority charge carriers. Proper carrier concentration optimization of the chalcogenide aerogel materials is needed if these materials are to be exploited in thermoelectrics.
Co-reporter:Lasantha Korala and Stephanie L. Brock
The Journal of Physical Chemistry C 2012 Volume 116(Issue 32) pp:17110-17117
Publication Date(Web):July 18, 2012
DOI:10.1021/jp305378u
Transparent CdSe (ZnS) core (shell) sol–gel materials have potential uses in optoelectronic applications such as light-emitting diodes (LEDs) due to their strong luminescence properties and the potential for charge transport through the prewired nanocrystal (NC) network of the gel. However, typical syntheses of metal chalcogenide gels yield materials with poor transparency. In this work, the mechanism and kinetics of aggregation of two sizes of CdSe (ZnS) core (shell) NCs, initiated by removal of surface thiolate ligands using tetranitromethane (TNM) as an oxidant, were studied by means of time-resolved dynamic light scattering (TRDLS); the characteristics of the resultant gels were probed by optical absorption, transmission electron microscopy (TEM), and small-angle X-ray scattering (SAXS). At low concentrations of NCs (ca. 4 × 10–7 M), the smaller, green-emitting NCs aggregate faster than the larger, orange-emitting NCs, for a specific oxidant concentration. The kinetics of aggregation have a significant impact on the macroscopic properties (i.e., transparency) of the resultant gels, with the transparency of the gels decreasing with the increase of oxidant concentration due the formation of larger clusters at the gel point and a shift away from a reaction-limited cluster-aggregation (RLCA) mechanism. This is further confirmed by analyses of the gel structures by SAXS and TEM. Likewise, the larger orange-emitting particles also produce larger aggregates at the gel point, leading to lower transparency. The ability to control the transparency of chalcogenide gels will enable their properties to be tuned in order to address application-specific needs in optoelectronics.
Co-reporter:Shreyashi Ganguly and Stephanie L. Brock
Journal of Materials Chemistry A 2011 vol. 21(Issue 24) pp:8800-8806
Publication Date(Web):12 May 2011
DOI:10.1039/C1JM11015B
The synthesis and characterization of lead telluride (PbTe) gels and aerogels with nanostructured features of potential benefit for enhanced thermoelectrics is reported. In this approach, discrete thiolate-capped PbTe nanoparticles were synthesized by a solution-based approach followed by oxidation-induced nanoparticle assembly with tetranitromethane or hydrogen peroxide to form wet gels. Drying of the wet gels by supercritical CO2 extraction yielded aerogels, whereas xerogels were produced by ambient pressure bench top drying. The gels consist of an interconnected network of colloidal nanoparticles and pores with surface areas up to 74 m2 g−1. The thermal stability of the nanostructures relative to nanoparticles was probed with the help of in situtransmission electron microscopy (TEM), thermogravimetric analysis (TGA) and differential scanning calorimetry (DSC). The aerogels were observed to sublime at a higher temperature and over a larger range (425–500 °C) relative to the precursor nanoparticles. TGA-DSC suggests that organic capping groups can be removed in the region 250–450 °C, and melting of PbTe nanoparticles occurs near the temperature for bulk materials (ca. 920 °C). The good thermal stability combined with the presence of nanoscale interfaces suggests PbTe gels may show promise in thermoelectric devices.
Co-reporter:Elayaraja Muthuswamy and Stephanie L. Brock
Chemical Communications 2011 vol. 47(Issue 45) pp:12334-12336
Publication Date(Web):21 Oct 2011
DOI:10.1039/C1CC15198C
Conversion of Ni12P5 nanoparticles to Ni2P is demonstrated to occur via a solid-state, rather than a solution dissolution, process. The templated transformation is employed to make monodisperse hollow or solid particles of the catalytically active phase Ni2P with surface areas of ∼17 m2 g−1.
Co-reporter:Qinghong Yao and Stephanie L. Brock
Inorganic Chemistry 2011 Volume 50(Issue 20) pp:9985-9992
Publication Date(Web):September 28, 2011
DOI:10.1021/ic201333y
Highly porous CdTe nanoarchitectures (aerogels) were prepared by sol–gel assembly of discrete nanocrystals followed by supercritical CO2 drying. CdTe nanocrystal surface functionalization (either phosphine oxide or thiolate) is found to be immaterial to oxidation induced gel formation suggesting that the standard thiolate capping procedure is not a necessary step in the gelation process. On the basis of this observation, and reduction induced dispersion of the gel network, the exposure of reactive sites and the subsequent surface oxidation reaction to form polychalcogenide linkages are key steps in the gelation mechanism. Consequently, CdTe aerogels exhibit similar physicochemical properties, regardless of original ligating functionality. The aerogels are mesoporous, with surface area >100 m2/g, and exhibit an optical bandgap of 1.92 eV, consistent with quantum confinement within the 3-D linked network. Photoluminescence is suppressed in the aerogels, but can be partially recovered upon heating.
Co-reporter:Shreyashi Ganguly, Chen Zhou, Donald Morelli, Jeffrey Sakamoto, Ctirad Uher, Stephanie L. Brock
Journal of Solid State Chemistry 2011 Volume 184(Issue 12) pp:3195-3201
Publication Date(Web):December 2011
DOI:10.1016/j.jssc.2011.09.031
Heterogeneous nanocomposites of p-type bismuth antimony telluride (Bi2−xSbxTe3) with lead telluride (PbTe) nanoinclusions have been prepared by an incipient wetness impregnation approach. The Seebeck coefficient, electrical resistivity, thermal conductivity and Hall coefficient were measured from 80 to 380 K in order to investigate the influence of PbTe nanoparticles on the thermoelectric performance of nanocomposites. The Seebeck coefficients and electrical resistivities of nanocomposites decrease with increasing PbTe nanoparticle concentration due to an increased hole concentration. The lattice thermal conductivity decreases with the addition of PbTe nanoparticles but the total thermal conductivity increases due to the increased electronic thermal conductivity. We conclude that the presence of nanosized PbTe in the bulk Bi2−xSbxTe3 matrix results in a collateral doping effect, which dominates transport properties. This study underscores the need for immiscible systems to achieve the decreased thermal transport properties possible from nanostructuring without compromising the electronic properties.Graphical abstractPbTe nanoparticles introduced into p-type Bi2Te3 by incipient wetness results in decreased lattice thermal conductivity, but also acts as an electronic dopant, resulting in an overall decrease in thermoelectric performance.Highlights► Composites of PbTe nanoparticles in Bi2−xSbxTe3 were formed by incipient wetness. ► PbTe nanoparticles leads to decreased κl, consistent with phonon scattering. ► PbTe nanoparticles lead to decreased S and ρ, due to increased carriers. ► Collateral doping from PbTe leads to decreased ZT with increasing concentration. ► Immiscible systems are preferred for improved ZT.
Co-reporter:Elayaraja Muthuswamy, Galbokka H. Layan Savithra, and Stephanie L. Brock
ACS Nano 2011 Volume 5(Issue 3) pp:2402
Publication Date(Web):March 7, 2011
DOI:10.1021/nn1033357
Simultaneous control of phase, size, and morphology in nanoscale nickel phosphides is reported. Phase-pure samples of discrete nanoparticles of Ni12P5 and Ni2P in hollow and solid morphologies can be prepared in a range of sizes (10−32 nm) by tuning key interdependent synthetic levers (P:Ni precursor ratio, temperature, time, oleylamine quantity). Size and morphology are controlled by the P:Ni ratio in the synthesis of the precursor particles, with large, hollow particles formed at low P:Ni and small, solid particles formed at high P:Ni. The P:Ni ratio also impacts the phase at the crystallization temperature (300−350 °C), with metal-rich Ni12P5 generated at low P:Ni and Ni2P at high P:Ni. Moreover, the product phase formed can be decoupled from the initial precursor ratio by the addition of more “P” at the crystallization temperature. This enables formation of hollow particles (favored by low P:Ni) of Ni2P (favored by high P:Ni). Increasing temperature and time also favor formation of Ni2P, by generating more reactive P and providing sufficient time for conversion to the thermodynamic product. Finally, increasing oleylamine concentration allows Ni12P5 to be obtained under high P:Ni precursor ratios that favor solid particle formation. Oleylamine concentration also acts to “tune” the size of the voids in particles formed at low P:Ni ratios, enabling access to Ni12P5 particles with different void sizes. This approach enables an unprecedented level of control over phase and morphology of nickel phosphide nanoparticles, paving the way for systematic investigation of the impact of these parameters on hydrodesulfurization activities of nickel phosphides.Keywords: morphology control; nanoparticles; nickel phosphides; phase control
Co-reporter:Peng Tian, Yanhua Zhang, Keerthi Senevirathne, Stephanie L. Brock, Ambesh Dixit, Gavin Lawes, and Simon J. L. Billinge
ACS Nano 2011 Volume 5(Issue 4) pp:2970
Publication Date(Web):March 2, 2011
DOI:10.1021/nn200020r
Discrete nanoparticles of MnAs with distinct magnetostructural properties have been prepared by small modifications of solution-phase arrested precipitation reactions. Rietveld and X-ray atomic pair distribution function based approaches were used to explore the evolution of the structure of the samples with temperature, and these data were compared to the magnetic response measured with ac susceptibility. Relative to a bulk standard, one type of MnAs nanoparticles was found to demonstrate similar but smaller structural transitions and corresponding magnetic changes. However, both magnetic and structural transitions in the second type of nanoparticles are strongly suppressed.Keywords: magnetic; MnAs; nanoparticle; PDF; structure
Co-reporter:Elayaraja Muthuswamy
Journal of the American Chemical Society 2010 Volume 132(Issue 45) pp:15849-15851
Publication Date(Web):October 21, 2010
DOI:10.1021/ja106397b
Unexpected reactivity on the part of oxide nanoparticles that enables their transformation into phosphides or sulfides by solution-phase reaction with trioctylphosphine (TOP) or sulfur, respectively, at temperatures of ≤370 °C is reported. Impressively, single-phase phosphide products are produced, in some cases with controlled anisotropy and narrow polydispersity. The generality of the approach is demonstrated for Ni, Fe, and Co, and while manganese oxides are not sufficiently reactive toward TOP to form phosphides, they do yield MnS upon reaction with sulfur. The reactivity can be attributed to the small size of the precursor particles, since attempts to convert bulk oxides or even particles with sizes approaching 50 nm were unsuccessful. Overall, the use of oxide nanoparticles, which are easily accessed via reaction of inexpensive salts with air, in lieu of organometallic reagents (e.g., metal carbonyls), which may or may not be transformed into metal nanoparticles, greatly simplifies the production of nanoscale phosphides and sulfides. The precursor nanoparticles can easily be produced in large quantities and stored in the solid state without concern that “oxidation” will limit their reactivity.
Co-reporter:Kanchana Somaskandan, Georgiy M. Tsoi, Lowell E. Wenger and Stephanie L. Brock
Journal of Materials Chemistry A 2010 vol. 20(Issue 2) pp:375-380
Publication Date(Web):09 Nov 2009
DOI:10.1039/B919447A
Magnetic MnP nanoparticles have been overcoated with the III–V semiconductor InP (MnP@InP nanoparticles) to create all-phosphide heterostructured nanoparticles. MnP nanoparticles are prepared by reaction of Mn2(CO)10 with P(SiMe3)3 in trioctylphosphine oxide–myristic acid at 220–250 °C for 36–48 h, and successful overcoating was achieved by injection of InCl3 and P(SiMe3)3 followed by heating at 260 °C for 30 min to 4 h. The resultant nanoparticles are spherical, with sizes on the order of 5 to 5.5 nm in diameter and narrow polydispersities (ca. 10%). InP shell thicknesses are estimated to be 0.35–0.55 nm based on the size increase upon addition of the InP precursor mixture relative to primary MnP particles. X-Ray powder diffraction patterns indicate the presence of both MnP and InP crystalline phases. Magnetic susceptibility measurements are consistent with previous data acquired on MnP nanoparticles, indicating that the overlayer does not impact the intrinsic magnetic properties; however, diffuse reflectance UV-visible spectroscopy shows that the optical band gap of InP is completely suppressed. These data are consistent with the formulation of MnP nanoparticles with a distinct InP overlayer in which the semiconducting properties are compromised by the proximity of the metallic core.
Co-reporter:IrinaR. Pala;IndikaU. Arachchige Dr.;DanielG. Georgiev Dr.;StephanieL. Brock Dr.
Angewandte Chemie 2010 Volume 122( Issue 21) pp:3743-3747
Publication Date(Web):
DOI:10.1002/ange.201000034
Co-reporter:StephanieL. Brock
Angewandte Chemie 2010 Volume 122( Issue 7) pp:
Publication Date(Web):
DOI:10.1002/ange.201090013
No abstract is available for this article.
Co-reporter:Shane Pawsey, Kennedy K. Kalebaila, Igor Moudrakovski, John A. Ripmeester and Stephanie L. Brock
The Journal of Physical Chemistry C 2010 Volume 114(Issue 31) pp:13187-13195
Publication Date(Web):July 19, 2010
DOI:10.1021/jp103157t
Metal chalcogenide aerogels and xerogels are unique materials that combine semiconducting nanostructures with porosity and are thus of interest for photocatalysis and sensing. To assess the feasibility for applications dependent on molecular transport, the pore structure and interconnectivity in CdS aerogels and xerogels were probed by a combination of conventional techniques and hyperpolarized (HP) 129Xe NMR. HP 129Xe NMR of the aerogels was consistent with two distinct types of accessible pores (adsorption sites), and 2-D EXSY NMR data suggest that these are connected. In contrast, a single resonance of low intensity with a temperature dependence consistent with the dissolution of Xe within a polymer matrix, that is, transport facilitated at high temperatures due to chain motion, is observed in xerogels. 13C NMR and thermal gravimetric analysis data reveal the presence of residual organics in both xerogels and aerogels, but a relatively higher proportion in the former, due, in part, to the surfactant used in their preparation. These data, combined with the absence of any meaningful adsorption isotherm for N2 at 77 K (where limited thermal chain motion precludes gas adsorption) are consistent with a dynamic blocking of the xerogel pores. The results reveal the important role of residual organics and drying regimens on the accessibility of pores in metal chalcogenide gel architectures.
Co-reporter:StephanieL. Brock
Angewandte Chemie International Edition 2010 Volume 49( Issue 7) pp:
Publication Date(Web):
DOI:10.1002/anie.201090013
No abstract is available for this article.
Co-reporter:IrinaR. Pala;IndikaU. Arachchige Dr.;DanielG. Georgiev Dr.;StephanieL. Brock Dr.
Angewandte Chemie International Edition 2010 Volume 49( Issue 21) pp:3661-3665
Publication Date(Web):
DOI:10.1002/anie.201000034
Co-reporter:StephanieL. Brock
Angewandte Chemie International Edition 2009 Volume 48( Issue 41) pp:7484-7486
Publication Date(Web):
DOI:10.1002/anie.200903989
Co-reporter:Keerthi Senevirathne, Ronald Tackett, Parashu Ram Kharel, Gavin Lawes, Kanchana Somaskandan and Stephanie L. Brock
ACS Nano 2009 Volume 3(Issue 5) pp:1129
Publication Date(Web):April 9, 2009
DOI:10.1021/nn900194f
Nanocrystals of thermodynamically stable α-MnAs (hexagonal NiAs-type) and metastable β-MnAs (orthorhombic MnP-type) have been synthesized by the reaction of triphenylarsine oxide (Ph3AsO) and dimanganesedecacarbonyl (Mn2CO10) at temperatures ranging from 250 to 330 °C in the presence of the coordinating solvent trioctylphosphine oxide (TOPO). Morphologically, both α- and β-MnAs nanoparticles adopt a core−shell type structure with a crystalline core and low-contrast noncrystalline shell. In contrast to prior studies on MnAs particles, disks, and films, the present bottom-up synthesis yields discrete, dispersible MnAs nanoparticles without a structural support. Even in the absence of epitaxial strain, the lattice parameters of the nanocrystals are decreased relative to bulk MnAs, resulting in a volume decrease of 0.35% in α-MnAs and 0.38% in β-MnAs nanoparticles. In contrast to bulk MnAs, where the ferromagnetic phase transition upon warming through 313−317 K is concomitant with a structure change from ferromagnetic α- to paramagnetic β-MnAs, powder X-ray diffraction studies suggest there is no conversion of α-MnAs to β over the temperature range 298−343 K. Moreover, magnetic measurements suggest that both α- and β-MnAs are ferromagnetic with TC ≈ 315 K. Partial phase transformation of β-MnAs nanoparticles into thermodynamically stable α-MnAs occurs slowly over time (i.e., months) at room temperature. However, there is no associated change in magnetization, suggesting the ferromagnetism observed in β-MnAs is intrinsic and cannot be attributed to α-MnAs impurities.Keywords: magnetism; manganese arsenide; nanoparticles; phase change; synthesis
Co-reporter:Elayaraja Muthuswamy, Parashu Ram Kharel, Gavin Lawes and Stephanie L. Brock
ACS Nano 2009 Volume 3(Issue 8) pp:2383
Publication Date(Web):August 4, 2009
DOI:10.1021/nn900574r
The transformation of Fe nanoparticles by trioctylphosphine (TOP) to phase-pure samples of either Fe2P or FeP is reported. Fe nanoparticles were synthesized by the decomposition of Fe(CO)5 in a mixture of octadecene and oleylamine at 200 °C and were subsequently reacted with TOP at temperatures in the region of 350−385 °C to yield iron phosphide nanoparticles. Shorter reaction times favored an iron-rich product (Fe2P), and longer reaction times favored a phosphorus-rich product (FeP). The reaction temperature was also a crucial factor in determining the phase of the final product, with higher temperatures favoring FeP and lower temperatures Fe2P. We also observe the formation of hollow structures in both FeP spherical nanoparticles and Fe2P nanorods, which can be attributed to the nanoscale Kirkendall effect. Magnetic measurements conducted on phase-pure samples suggest that ∼8 × 70 nm Fe2P rods are ferromagnetic with a Curie temperature between 215 and 220 K and exhibit a blocking temperature of 179 K, whereas FeP is metamagnetic with a Néel temperature of ∼120 K. These data agree with the inherent properties of bulk-phase samples and attest to the phase purity that can be achieved by this method.Keywords: iron phosphides; magnetic properties; nanoparticles; structure transformation; synthesis
Co-reporter:Hongtao Yu, Yi Liu and Stephanie L. Brock
ACS Nano 2009 Volume 3(Issue 7) pp:2000
Publication Date(Web):July 2, 2009
DOI:10.1021/nn900456f
The effect of bulk network density on the extent of quantum confinement (probed by optical band gap) in CdSe quantum dot gels is evaluated. The CdSe gels were produced from controlled removal of surface thiolate ligands from CdSe quantum dots by adding 3% tetranitromethane. Two main techniques were employed to systematically vary the bulk density. First, different amounts of oxidizing agent were added to change the monolith density of the wet gel, followed by supercritical CO2 drying to yield CdSe aerogels with different bulk densities. Experimental results suggest that a gradual and almost linear band gap decrease is observed when increasing the bulk density at the aerogel level. The fact that quantum confinement effects are largely preserved in aerogel constructs is consistent with SAXS data revealing the fractal nature of the network. Second, for a constant amount of oxidant, different drying techniques were used to yield CdSe gels with a larger density variation: aerogels (supercritical CO2 dried), ambigels (hexane dried), and xerogels (acetone dried). A nonlinear trend for band gap decrease was found when comparing CdSe aerogels, ambigels, and xerogels, and the more dense ambi- and xerogels have broader absorption edges, suggestive of resonance transfer effects due to dipole−dipole interactions in non-homogeneous interacting systems. This is attributed to increased aggregation in the denser constructs (supported by TEM and SAXS data). Together, these data suggest that highly porous architectures, such as aerogels, are best suited for maintaining localized quantum confinement effects in 3D connected nanoparticle networks.Keywords: aerogel; CdSe; chalcogenide gels; density; dimensionality; quantum confinement; quantum dots; xerogel
Co-reporter:StephanieL. Brock
Angewandte Chemie 2009 Volume 121( Issue 41) pp:7620-7622
Publication Date(Web):
DOI:10.1002/ange.200903989
Co-reporter:Ye-Zi You, Kennedy K. Kalebaila, Stephanie L. Brock and David Oupický
Chemistry of Materials 2008 Volume 20(Issue 10) pp:3354
Publication Date(Web):April 25, 2008
DOI:10.1021/cm703363w
Temperature-dependent uptake and release of small molecules within porous silica nanoparticles has been achieved by treatment of preformed, thiol-functionalized micro-to-mesoporous silica nanoparticles (MSN) with pyridyl disulfide-terminated poly(N-isopropylacrylamide) (PNIPAM−S−S−Py). The resulting nanoparticle−polymer composites show uptake and release of fluorescein at room temperature (below the lower critical solution temperature, LCST, of the polymer) and a low level of leakage at 38 °C (above LCST, <2% after 2 h). The data are consistent with a mode of action in which fluorescein diffusion occurs readily when the polymer is in the random coil conformation but is significantly retarded when the polymer adopts the globule conformation. This mode of action is opposite to that observed for systems in which the PNIPAM is grown from the porous silica surface or co-condensed with silica and is accompanied by a greater than 10-fold improvement in fluorescein retention in the “pore-closed” conformation.
Co-reporter:Hongtao Yu ; Yi Liu
Inorganic Chemistry 2008 Volume 47(Issue 5) pp:1428-1434
Publication Date(Web):February 8, 2008
DOI:10.1021/ic701020s
MoS2 nanoparticles of size <5 nm have been synthesized via the reaction of Mo(CO)6 with elemental sulfur in trioctylphosphine oxide and 1-octadecene at temperatures from 270 to 330 °C. The MoS2 nanoparticles are discrete and dispersible in a variety of nonpolar organic solvents, including toluene, chloroform, and pyridine. The size of the particles can be effectively tuned by varying the temperature, yielding nearly monodisperse samples (<10% standard deviation) as evidenced by transmission electron microscopy (TEM). Additionally, larger (20–50 nm) onion- and tube-shaped MoS2 nanoparticles can be obtained by decreasing the amount of the coordinating solvent (trioctylphosphine oxide) relative to 1-octadecene. As-prepared samples are poorly crystalline, showing only weak contrast in the TEM and an absence of the first-order (00l) reflection in powder X-ray diffraction that is indicative of regular MoS2 stacking. Samples heated in situ in the TEM are observed to develop contrast and lattice fringes as the temperature is raised to 550 °C. Ex-situ heated samples show the appearance of the first order (00l) reflection at temperatures >870 °C.
Co-reporter:Stephanie L. Brock, Keerthi Senevirathne
Journal of Solid State Chemistry 2008 Volume 181(Issue 7) pp:1552-1559
Publication Date(Web):July 2008
DOI:10.1016/j.jssc.2008.03.012
Recent advances in synthetic methods have led to the preparation of a wide array of transition metal phosphide nanoparticles, and characterization of these materials has provided insight into nanoscale magnetic and catalytic properties. This review highlights advances in the field that have been made since the time of the last review [S.L. Brock, S.C. Perera, K.L. Stamm, Chem. Eur. J. 10(2004)3364–3371]. Synthetic methods include solvothermal, solution-phase arrested precipitation, metal nanoparticle conversion, and phosphate reduction. Magnetic properties of FeP, Fe2P and MnP nanoparticles and nanorods (among others), and recent data on thiophene hydrodesulfurization catalyzed by discrete, unsupported Ni2P particles, is presented. Finally, the future prospects for the field are discussed.Recent advances in synthetic methods have led to the preparation of a wide array of transition metal phosphide nanoparticles, and characterization of these materials has provided insight into nanoscale magnetic and catalytic properties. This paper highlights advances in the field that have been made since 2004.
Co-reporter:Hongtao Yu and Stephanie L. Brock
ACS Nano 2008 Volume 2(Issue 8) pp:1563
Publication Date(Web):July 15, 2008
DOI:10.1021/nn8002295
We demonstrate the effect of differently shaped CdSe nanoscale building blocks (dots, rods, branched nanoparticles, and hyperbranched nanoparticles) on the morphologies, surface characteristics, and optical properties of resultant porous CdSe nanostructured aerogels. Monolithic CdSe aerogels were produced by controlled oxidative removal of surface thiolate ligands from differently shaped CdSe nanoparticles to yield a wet gel, followed by CO2 supercritical drying. The X-ray diffraction data show that the resultant CdSe aerogels maintain the crystalline phase of the building blocks without significant grain growth. However, the transmission electron microscopy images indicate that the morphology of CdSe aerogels changes from a colloid-type morphology to a polymer-type morphology when the building block changes from dot to rod or the branched nanoparticle. The morphology of the CdSe aerogel assembled from hyperbranched nanoparticles appears to be intermediate between the colloid-type and the polymer-type. Nitrogen physisorption measurements suggest that the surface areas and porosity are a direct function of the shape of the primary building blocks, with aerogels formed from rods or branched particles exhibiting the greatest surface areas (>200 m2/g) and those prepared from hyperbranched nanoparticles exhibiting the least (<100 m2/g). Band gap measurements and photoluminescence studies show that the as-prepared CdSe aerogels retain to a large extent the intrinsic quantum confinement of the differently shaped building blocks, despite being connected into a 3D network.Keywords: CdSe nanomaterials; colloidal aerogel; polymeric aerogel; porous structures; quantum confinement
Co-reporter:Indika U. Arachchige and Stephanie L. Brock
Accounts of Chemical Research 2007 Volume 40(Issue 9) pp:801
Publication Date(Web):April 19, 2007
DOI:10.1021/ar600028s
Sol–gel chemistry represents a powerful method for assembling metal chalcogenide quantum dots into 3D connected architectures without the presence of intervening ligands to moderate particle–particle interactions. Wet gels prepared by the oxidative loss of thiolate surface groups from chalcogenide nanoparticles can be converted to xerogels (low porosity) or aerogels (high porosity), and the quantum-confinement effects in these low-dimensional networks decrease with increasing density of the network. In this Account, we describe the application of sol–gel chemistry to the formation of CdSe architectures and discuss how surface modification can lead to highly luminous monoliths, concluding with the prospects of these unique materials for applications in sensing and photovoltaics.
Co-reporter:K. Senevirathne;A. W. Burns;M. E. Bussell;S. L. Brock
Advanced Functional Materials 2007 Volume 17(Issue 18) pp:
Publication Date(Web):28 NOV 2007
DOI:10.1002/adfm.200700758
Discrete, unsupported nanoparticles of Ni2P have been prepared by using a solution-phase method with bis(1,5-cyclooctadiene)nickel(0) [Ni(COD)2] as the nickel source and trioctylphosphine (TOP) as the phosphorus source in the presence of the coordinating solvent trioctylphosphine oxide (TOPO). Ni2P nanoparticles prepared at 345 °C have an average crystallite size of 10.2 ± 0.7 nm and are capped with TOP and/or TOPO coordinating agents. The surface of the Ni2P nanoparticles can be modified by washing with CHCl3 or by exchanging TOP/TOPO groups with mercaptoundecanoic acid (MUA). The surface areas of these nanoparticles are on the order of 30–70 m2 g–1. As-prepared and MUA-capped nanoparticles undergo a phase transformation at 370 °C under reducing conditions, but CHCl3-washed Ni2P nanoparticles retain the Ni2P structure. CHCl3-washed and MUA-capped nanoparticles exhibit higher HDS catalytic activity than as-prepared nanoparticles or unsupported Ni2P prepared by temperature-programmed reduction of a phosphate precursor. The surface modifications have a clear effect on the catalytic activity as well as the thermal stability of Ni2P nanoparticles under reducing conditions.
Co-reporter:Palaniappan Arumugam, Samuel S. Shinozaki, Ruomiao Wang, Guangzhao Mao and Stephanie L. Brock
Chemical Communications 2006 (Issue 10) pp:1121-1123
Publication Date(Web):25 Jan 2006
DOI:10.1039/B514595C
A new approach to the generation of nanoparticle arrays in periodic as well as non-periodic fashions has been discovered based on reduction of oxidized nanoscroll/nanoribbon precursors in the transmission electron microscope (carbothermal reduction) or by hydrogen annealing. Arrays consisting of nickel arsenide nanoparticles of size 3–4 nm have been generated.
Co-reporter:Kennedy K. Kalebaila, Daniel G. Georgiev, Stephanie L. Brock
Journal of Non-Crystalline Solids 2006 Volume 352(Issue 3) pp:232-240
Publication Date(Web):1 March 2006
DOI:10.1016/j.jnoncrysol.2005.11.035
The synthesis of germanium sulfide gels by thiolysis reactions of a non-aqueous solution of Ge(OEt)4, followed by supercritical fluid extraction to create aerogels, is described. Analysis of the as-prepared GeSx aerogels by powder X-ray diffraction (PXRD) and surface area analysis reveals an amorphous structure exhibiting very high surface areas, 755 m2/g, that rival those of the best SiO2 aerogels when compared on a per mole basis. Transmission electron microscopy shows that the aerogel material is composed of a continuous network of GeSx colloidal particles assembled in a three-dimensional architecture. A detailed comparison of GeSx aerogels and their xerogel (bench-top dried) counterparts in terms of the influence of the synthetic methodology on morphology and surface area is reported. In the presence of adventitious moisture, the amorphous GeSx is oxidized to a crystalline phase identified by X-ray photoelectron spectroscopy, Raman spectroscopy and PXRD cell refinement to be hexagonal GeO2.
Co-reporter:Jaya L. Mohanan;Indika U. Arachchige
Science 2005 Vol 307(5708) pp:397-400
Publication Date(Web):21 Jan 2005
DOI:10.1126/science.1104226
Abstract
Chalcogenide aerogels based entirely on semiconducting II-VI or IV-VI frameworks have been prepared from a general strategy that involves oxidative aggregation of metal chalcogenide nanoparticle building blocks followed by supercritical solvent removal. The resultant materials are mesoporous, exhibit high surface areas, can be prepared as monoliths, and demonstrate the characteristic quantum-confined optical properties of their nanoparticle components. These materials can be synthesized from a variety of building blocks by chemical or photochemical oxidation, and the properties can be further tuned by heat treatment. Aerogel formation represents a powerful yet facile method for metal chalcogenide nanoparticle assembly and the creation of mesoporous semiconductors.
Co-reporter:Jennifer Ann Aitken, Valentina Ganzha-Hazen, Stephanie L. Brock
Journal of Solid State Chemistry 2005 Volume 178(Issue 4) pp:970-975
Publication Date(Web):April 2005
DOI:10.1016/j.jssc.2004.10.004
Polycrystalline Cu3P was successfully prepared under a wide variety of solvothermal conditions. The reaction of red phosphorus with several copper sources (copper metal, copper (I) iodide, copper (I) chloride and copper (II) chloride) at 150–200 °C for 1–2 days in water produced Cu3P. Products were examined with powder X-ray diffraction, scanning electron microscopy and energy dispersive spectroscopy. Thermal analyses and optical spectroscopy were also performed. A detailed list of reaction conditions, products and impurity phases (where applicable) are reported.Just add water! Cu3P can be prepared solvothermally as pure phase material without the use of reactive yellow-phosphorus or N-donor solvents.
Co-reporter:Buddhimathie Jayasekera ;Andy Y. H. Lo;Robert W. Schurko ;Gholam-Abbas Nazri
Chemistry - A European Journal 2005 Volume 11(Issue 12) pp:
Publication Date(Web):13 APR 2005
DOI:10.1002/chem.200400727
A series of P/As mixed pnicogen phases of composition (CuI)8P12−xAsx, in which x=2.4, 4.2, 4.8, 5.4, and 6.6, have been synthesized and characterized by X-ray single crystal and powder diffraction, solid-state NMR spectroscopy, thermal gravimetric analysis, and impedance spectroscopy. These materials are isostructural to (CuI)8P12 and consist of neutral, tubular P/As mixed pnicogen chains associated with CuI and I− ions. The As is distributed throughout the pnicogen chains; however, the “roof” sites of the [P8] cage show preferred occupation by As relative to the other sites. Accordingly, the change in cell volume is not a linear function of the As incorporation. Solid-state 31P NMR spectroscopy of the 40 % As incorporated sample are consistent with the X-ray structural model, with extensive broadening due to 31P–75As coupling and site disorder, and a change in the chemical shifts of the resonances due to the As substitution into the lattice. The degree of copper ion site disorder, probed by single-crystal X-ray diffraction, increases with increasing As content. Although very little change is observed in the copper ionic conductivity of polycrystalline samples, which ranges from 1.8–5.1×10−6 S cm−1 for (CuI)8P12−xAsx, x=0, 4.2, 5.4; a single crystal (x=4.8) measured along the needle axis has a conductivity of 1.7×10−3 S cm−1 at 128 °C. This represents an order of magnitude improvement in conductivity over (CuI)8P12 at the same temperature.
Co-reporter:Stephanie L. Brock ;Susanthri C. Perera Dr.;Kimber L. Stamm
Chemistry - A European Journal 2004 Volume 10(Issue 14) pp:
Publication Date(Web):9 MAR 2004
DOI:10.1002/chem.200305775
Nanoparticulate transition-metal phosphides remain an unexplored, though emerging area of interest on the materials landscape, due principally to their promising magnetic and catalytic properties. This review describes synthetic strategies for the formation of both supported and unsupported transition-metal phosphide nanoparticles, provides a summary of their relevant magnetic and catalytic properties, and indicates new directions for exploration.
Co-reporter:Elayaraja Muthuswamy and Stephanie L. Brock
Chemical Communications 2011 - vol. 47(Issue 45) pp:NaN12336-12336
Publication Date(Web):2011/10/21
DOI:10.1039/C1CC15198C
Conversion of Ni12P5 nanoparticles to Ni2P is demonstrated to occur via a solid-state, rather than a solution dissolution, process. The templated transformation is employed to make monodisperse hollow or solid particles of the catalytically active phase Ni2P with surface areas of ∼17 m2 g−1.
Co-reporter:Shreyashi Ganguly and Stephanie L. Brock
Journal of Materials Chemistry A 2011 - vol. 21(Issue 24) pp:NaN8806-8806
Publication Date(Web):2011/05/12
DOI:10.1039/C1JM11015B
The synthesis and characterization of lead telluride (PbTe) gels and aerogels with nanostructured features of potential benefit for enhanced thermoelectrics is reported. In this approach, discrete thiolate-capped PbTe nanoparticles were synthesized by a solution-based approach followed by oxidation-induced nanoparticle assembly with tetranitromethane or hydrogen peroxide to form wet gels. Drying of the wet gels by supercritical CO2 extraction yielded aerogels, whereas xerogels were produced by ambient pressure bench top drying. The gels consist of an interconnected network of colloidal nanoparticles and pores with surface areas up to 74 m2 g−1. The thermal stability of the nanostructures relative to nanoparticles was probed with the help of in situtransmission electron microscopy (TEM), thermogravimetric analysis (TGA) and differential scanning calorimetry (DSC). The aerogels were observed to sublime at a higher temperature and over a larger range (425–500 °C) relative to the precursor nanoparticles. TGA-DSC suggests that organic capping groups can be removed in the region 250–450 °C, and melting of PbTe nanoparticles occurs near the temperature for bulk materials (ca. 920 °C). The good thermal stability combined with the presence of nanoscale interfaces suggests PbTe gels may show promise in thermoelectric devices.
Co-reporter:Kanchana Somaskandan, Georgiy M. Tsoi, Lowell E. Wenger and Stephanie L. Brock
Journal of Materials Chemistry A 2010 - vol. 20(Issue 2) pp:NaN380-380
Publication Date(Web):2009/11/09
DOI:10.1039/B919447A
Magnetic MnP nanoparticles have been overcoated with the III–V semiconductor InP (MnP@InP nanoparticles) to create all-phosphide heterostructured nanoparticles. MnP nanoparticles are prepared by reaction of Mn2(CO)10 with P(SiMe3)3 in trioctylphosphine oxide–myristic acid at 220–250 °C for 36–48 h, and successful overcoating was achieved by injection of InCl3 and P(SiMe3)3 followed by heating at 260 °C for 30 min to 4 h. The resultant nanoparticles are spherical, with sizes on the order of 5 to 5.5 nm in diameter and narrow polydispersities (ca. 10%). InP shell thicknesses are estimated to be 0.35–0.55 nm based on the size increase upon addition of the InP precursor mixture relative to primary MnP particles. X-Ray powder diffraction patterns indicate the presence of both MnP and InP crystalline phases. Magnetic susceptibility measurements are consistent with previous data acquired on MnP nanoparticles, indicating that the overlayer does not impact the intrinsic magnetic properties; however, diffuse reflectance UV-visible spectroscopy shows that the optical band gap of InP is completely suppressed. These data are consistent with the formulation of MnP nanoparticles with a distinct InP overlayer in which the semiconducting properties are compromised by the proximity of the metallic core.
Co-reporter:Lasantha Korala, Li Li and Stephanie L. Brock
Chemical Communications 2012 - vol. 48(Issue 68) pp:NaN8525-8525
Publication Date(Web):2012/07/03
DOI:10.1039/C2CC34188C
A method of fabricating sol–gel quantum dot (QD) films is demonstrated, and their optical, structural and electrical properties are evaluated. The CdSe(ZnS) xerogel films remain quantum confined, yet are highly conductive (10−3 S cm−1). This approach provides a pathway for the exploitation of QD gels in optoelectronic applications.
Co-reporter:Malsha A. Hettiarachchi, Ehab Abdelhamid, Boris Nadgorny and Stephanie L. Brock
Journal of Materials Chemistry A 2016 - vol. 4(Issue 28) pp:NaN6797-6797
Publication Date(Web):2016/06/20
DOI:10.1039/C6TC01478J
A solution phase methodology was developed for the formation of discrete colloidal MnSb nanoparticles using dimanganesedecacarbonyl and triphenylantimony as the main reaction components. Stoichiometric reactions result in significant Sb impurities, but these can be eliminated by the use of excess Mn reagent, limiting the reaction time, and using a lower temperature (280 °C) relative to that commonly employed for MnP or MnAs synthesis (330–360 °C). The resultant MnSb nanoparticles are, when evidenced by both powder X-ray diffraction and transmission electron microscopy, ca. 14 nm in diameter and exhibit low polydispersity (13 ± 1.7 nm). High Angle Annular Dark Field-Scanning Transmission Electron Microscopy and energy dispersive line scan data revealed that the as-synthesized MnSb nanoparticles are core–shell in nature, having a MnSb core and an amorphous manganese oxide shell. Evidence is presented supporting a pathway for decomposition of MnSb nanoparticles driven by formation of MnO2 and Sb due to reaction with adventitious O2. The MnSb nanoparticles are superparamagnetic at room temperature, and exhibit suppressed moments attributed to surface oxidation arising from the high surface area and intrinsic oxophilicity of Mn.
Co-reporter:Roshini Pimmachcharige, Yanhua Zhang, Rajesh Regmi, Gavin Lawes and Stephanie L. Brock
Journal of Materials Chemistry A 2017 - vol. 5(Issue 13) pp:NaN3358-3358
Publication Date(Web):2017/03/10
DOI:10.1039/C7TC00579B
MnAs exhibits a large magnetocaloric effect associated with the first-order phase transition at 315 K, making it a promising phase for near-room-temperature magnetic refrigeration technologies. Optimization of the properties to expand the temperature range of operation (by adjusting the phase transition temperature) and reduce hysteresis losses can be achieved by phosphorus-doping and nanostructuring, respectively. The synthesis of P-doped MnAs as discrete nanoparticles by rapid injection synthesis has been previously reported, but suffers from extensive polydispersity and an inability to independently control size and dopant concentration. In the present work, a kinetic analysis of the P-doped MnAs nanoparticle formation by temporal correlation of particle volume, P-dopant concentration, and particle size to monomer concentration, is undertaken. Narrow polydispersity samples can only be obtained by rapid quenching from the reaction temperature, achieved by injection of the hot solution into cold chloroform; cooling in the flask leads to polydispersity characteristic of Ostwald ripening. When isolated at high temperature, particles initially grow at high monomer concentrations, achieving volumes of ca. 740 nm3 by 10 min, and then decrease in volume by more than a factor of two by 30 min reaction time, at which point both the size and residual monomer concentration (ca. 20%) remain constant, suggesting formation of an equilibrium or an unreactive byproduct. Simultaneously, the concentration of P incorporated is found to decrease over the time of the reaction from 5–7% initially to a nearly constant concentration of <2% by 60 min. These data suggest that P is incorporated preferentially at the nucleation stage, but is lost over time. This detailed understanding of MnAs particle formation and P-inclusion enables independent assessment of the role of size, polydispersity, and dopant concentration on magnetic properties.
Co-reporter:Jilian N. De Freitas, Lasantha Korala, Luke X. Reynolds, Saif A. Haque, Stephanie L. Brock and Ana F. Nogueira
Physical Chemistry Chemical Physics 2012 - vol. 14(Issue 43) pp:NaN15184-15184
Publication Date(Web):2012/09/12
DOI:10.1039/C2CP42998E
CdSe(ZnS) core(shell) aerogels were prepared from the assembly of quantum dots into mesoporous colloidal networks. The sol–gel method produces inorganic particle interfaces with low resistance to electrical transport while maintaining quantum-confinement. The photoelectrochemical properties of aerogels and their composites with poly(3-hexylthiophene) are reported for the first time.