Co-reporter:Joseph Czekner, Ling Fung Cheung, and Lai-Sheng Wang
The Journal of Physical Chemistry C May 25, 2017 Volume 121(Issue 20) pp:10752-10752
Publication Date(Web):December 12, 2016
DOI:10.1021/acs.jpcc.6b10958
We report high-resolution photoelectron imaging of B11– and B12– at 354.7 and 532.0 nm, respectively, resolving several low-frequency vibrational modes for neutral B11 and B12. The vibrational information is highly valuable to verify the structures of the neutral clusters. Several isomers are considered, and vibrational frequencies are calculated for B11 and B12 using density functional theory. Comparisons between the experimental and calculated vibrational frequencies prove that the B11 neutral and anion both possess a perfectly planar C2v structure. The B12– anion is quasi-planar with Cs symmetry, while the experiment confirms that neutral B12 possesses C3v symmetry. The high-resolution photoelectron spectra also allow the electron affinities of B11 and B12 to be measured more accurately as 3.401 ± 0.002 and 2.221 ± 0.002 eV, respectively. It is shown that high-resolution photoelectron imaging can be an effective method to determine structures of small neutral boron clusters, complementary to infrared spectroscopy.
Co-reporter:Navneet Singh Khetrapal, Tian Jian, Gary V. Lopez, Seema Pande, Lai-Sheng Wang, and Xiao Cheng Zeng
The Journal of Physical Chemistry C August 24, 2017 Volume 121(Issue 33) pp:18234-18234
Publication Date(Web):July 26, 2017
DOI:10.1021/acs.jpcc.7b04997
We report a combined photoelectron spectroscopy and theoretical study of the structural evolution of aluminum cluster anions doped with two gold atoms, Au2Aln– (n = 3–11). Well-resolved photoelectron spectra have been obtained at several photon energies and are used to compare with theoretical calculations to elucidate the structures of the bimetallic clusters. Global minima of the Au2Aln– clusters were searched using the basin-hopping method combined with density functional theory calculations. Vertical detachment energies were computed for the low-lying isomers with the inclusion of spin–orbit effects and were used to generate simulated photoelectron spectra. Au2Al2– was previously found to exhibit a tetrahedral structure, whereas Au2Al3– is found currently to be planar. Beyond n = 3, the global minima of Au2Aln– are dominated by three-dimensional structures. A robust square-bipyramidal Al6 motif is observed for n = 6–9, leading to a highly stable tubular-like global minimum for Au2Al9–. Compact three-dimensional structures are observed for n = 10 and 11. Except for Au2Al4–, Au2Al6–, and Au2Al7–, the two gold atoms are separated in these digold-atom-doped aluminum clusters due to the strong Au–Al interactions.
Co-reporter:Wan-Lu Li;Tian Jian;Xin Chen;Hai-Ru Li;Teng-Teng Chen;Xue-Mei Luo;Si-Dian Li;Jun Li
Chemical Communications 2017 vol. 53(Issue 10) pp:1587-1590
Publication Date(Web):2017/01/31
DOI:10.1039/C6CC09570D
A tubular molecular rotor B2-Ta@B18− (1) and boron drum Ta@B20− (2) with the highest coordination number of twenty in chemistry are observed via a joint photoelectron spectroscopy and first-principles theory investigation.
Co-reporter:Tian Jian;Ling Fung Cheung;Joseph Czekner;Teng-Teng Chen;Gary V. Lopez;Wei-Li Li
Chemical Science (2010-Present) 2017 vol. 8(Issue 11) pp:7528-7536
Publication Date(Web):2017/10/23
DOI:10.1039/C7SC02881D
We report a photoelectron spectroscopy and high-resolution photoelectron imaging study of a bimetallic Nb2Au6− cluster. Theoretical calculations, in conjunction with the experimental data, reveal that Nb2Au6−/0 possess high-symmetry D6h structures featuring a Nb–Nb axis coordinated equatorially by an Au6 ring. Chemical bonding analyses show that there are two π bonds and one σ bond in the Nb2 moiety in Nb2©Au6, as well as five totally delocalized σ bonds. The NbNb triple bond is strengthened significantly by the delocalized σ bonds, resulting in an extremely short Nb–Nb bond length comparable to the quintuple bond in gaseous Nb2. The totally delocalized σ bonding in Nb2©Au6 is reminiscent of σ aromaticity, representing a new bonding mode in metal–ligand systems. The unusually short Nb–Nb bond length in Nb2©Au6 shows that the Au6 ring can serve as a bridging ligand to facilitate multiple bonding in transition metal dimers via delocalized σ bonding.
Co-reporter:Qiang Chen;Wen-Juan Tian;Lin-Yan Feng;Hai-Gang Lu;Yue-Wen Mu;Hua-Jin Zhai;Si-Dian Li
Nanoscale (2009-Present) 2017 vol. 9(Issue 13) pp:4550-4557
Publication Date(Web):2017/03/30
DOI:10.1039/C7NR00641A
Boron clusters have been found to exhibit a variety of interesting electronic, structural, and bonding properties. Of particular interest are the recent discoveries of the 2D hexagonal B36−/0 which led to the concept of borophenes and the 3D fullerene-like B40−/0 which marked the onset of borospherene chemistry. Here, we present a joint photoelectron spectroscopic and first-principles study of B37− and B38−, which are in the transition size range between the 2D borophene-type clusters and the 3D borospherenes. These two clusters are found to possess highly stable 2D global-minimum structures consisting of a double-hexagonal vacancy. Detailed bonding analyses reveal that both B37− and B38− are all-boron analogues of coronene (C24H12) with a unique delocalized π system, featuring dual π aromaticity. These clusters with double hexagonal vacancies can be viewed as molecular motifs for the χ3-borophene which is the most stable form of borophenes recently synthesized on an Ag(111) substrate.
Co-reporter:Xue-Mei Luo, Tian Jian, Long-Jiu Cheng, Wan-Lu Li, Qiang Chen, Rui Li, Hua-Jin Zhai, Si-Dian Li, Alexander I. Boldyrev, Jun Li, Lai-Sheng Wang
Chemical Physics Letters 2017 Volume 683(Volume 683) pp:
Publication Date(Web):1 September 2017
DOI:10.1016/j.cplett.2016.12.051
•Bn− monoanions have been systematically investigated up to n = 30. However, B26− has remained elusive in this size range.•Here we present a joint photoelectron spectroscopy and first-principles study on the structures and bonding of this seemingly enigmatic cluster.•Extensive global minimum searches and high-level calculations reveal that isomer I dominates the experimental spectrum and represents the smallest 2D boron cluster with a hexagonal vacancy.•Isomer III is found to contribute to the measured PE spectrum as a minor species.•Chemical bonding analyses show that isomer I can be viewed as an all-boron analog of the polycyclic aromatic hydrocarbon C17H11+.Anionic boron clusters have been systematically investigated both experimentally and theoretically up to 30 atoms and have all been proved to be planar or quasi-planar (2D) in their global minima. However, the B26− cluster has remained elusive in this size range up to now, because of its complicated potential landscape. Here we present a joint photoelectron spectroscopy (PES) and first-principles study on the structures and bonding of this seemingly enigmatic cluster. Extensive global minimum searches, followed by high-level calculations and Gibbs free energy corrections, reveal that at least three 2D isomers, I (C1, 2A), II (C1, 2A), and III (C1, 2A), could contribute to the observed PE spectrum for the B26− cluster. Isomer I, which has the lowest free energy at finite temperatures, is found to dominate the experimental spectrum and represents the smallest 2D boron cluster with a hexagonal vacancy. Distinct spectral features are observed for isomer III, which has a pentagonal hole and is found to contribute to the measured PE spectrum as a minor species. Isomer II with a close-packed triangular 2D structure, which is the global minimum at 0 K, may also contribute to the observed spectrum as a minor species. Chemical bonding analyses show that the principal isomer I can be viewed as an all-boron analog of the polycyclic aromatic hydrocarbon C17H11+ in terms of the π bonds.Download high-res image (134KB)Download full-size image
Co-reporter:Xin Chen, Ya-Fan Zhao, Lai-Sheng Wang, Jun Li
Computational and Theoretical Chemistry 2017 Volume 1107(Volume 1107) pp:
Publication Date(Web):1 May 2017
DOI:10.1016/j.comptc.2016.12.028
•We developed a global minimum search program named TGMin.•TGMin program is based on the basin hopping algorithm with several improvements.•TGMin program is highly effecient in finding the global minima of nanoclusters.•An overview of recent improvements and applications of TGMin are presented.Finding the global minima of nanoclusters is of great importance in cluster science and nanoscience. We have developed an efficient global minimum search program, named Tsinghua Global Minimum (TGMin, first released in 2012), based on the Basin-Hopping algorithm to find the global minima of nanoclusters, as well as periodic systems. We have recently made several improvements to the original Basin-Hopping algorithm, including a constrained perturbation function, a covalent-radius-based relaxation algorithm, an improved ultrafast shape recognition algorithm, and a planeness-check mechanism. The TGMin program has been successfully applied to search the global minima of a number of nanoclusters and periodic structures, including B30, B35, B36, B39, B40, CoB18−, RhB18−, MnB16−, and Au7 on the α-Al2O3(0 0 0 1) surface. An overview of the TGMin code and several of its recent applications are presented here.Download high-res image (164KB)Download full-size image
Co-reporter:Teng-Teng Chen;Wan-Lu Li;Tian Jian;Xin Chen; Dr. Jun Li; Dr. Lai-Sheng Wang
Angewandte Chemie 2017 Volume 129(Issue 24) pp:7020-7024
Publication Date(Web):2017/06/06
DOI:10.1002/ange.201703111
AbstractThe structure and bonding of a Pr-doped boron cluster (PrB7−) are investigated using photoelectron spectroscopy and quantum chemistry. The adiabatic electron detachment energy of PrB7− is found to be low [1.47(8) eV]. A large energy gap is observed between the first and second detachment features, indicating a highly stable neutral PrB7. Global minimum searches and comparison between experiment and theory show that PrB7− has a half-sandwich structure with C6v symmetry. Chemical bonding analyses show that PrB7− can be viewed as a PrII[η7-B73−] complex with three unpaired electrons, corresponding to a Pr (4f26s1) open-shell configuration. Upon detachment of the 6s electron, the neutral PrB7 cluster is a highly stable PrIII[η7-B73−] complex with Pr in its favorite +3 oxidation state. The B73− ligand is found to be highly stable and doubly aromatic with six delocalized π and six delocalized σ electrons and should exist for a series of lanthanide MIII[η7-B73−] complexes.
Co-reporter:Teng-Teng Chen;Wan-Lu Li;Tian Jian;Xin Chen; Dr. Jun Li; Dr. Lai-Sheng Wang
Angewandte Chemie International Edition 2017 Volume 56(Issue 24) pp:6916-6920
Publication Date(Web):2017/06/06
DOI:10.1002/anie.201703111
AbstractThe structure and bonding of a Pr-doped boron cluster (PrB7−) are investigated using photoelectron spectroscopy and quantum chemistry. The adiabatic electron detachment energy of PrB7− is found to be low [1.47(8) eV]. A large energy gap is observed between the first and second detachment features, indicating a highly stable neutral PrB7. Global minimum searches and comparison between experiment and theory show that PrB7− has a half-sandwich structure with C6v symmetry. Chemical bonding analyses show that PrB7− can be viewed as a PrII[η7-B73−] complex with three unpaired electrons, corresponding to a Pr (4f26s1) open-shell configuration. Upon detachment of the 6s electron, the neutral PrB7 cluster is a highly stable PrIII[η7-B73−] complex with Pr in its favorite +3 oxidation state. The B73− ligand is found to be highly stable and doubly aromatic with six delocalized π and six delocalized σ electrons and should exist for a series of lanthanide MIII[η7-B73−] complexes.
Co-reporter:Wan-Lu Li, Hong-Tao Liu, Tian Jian, Gary V. Lopez, Zachary A. Piazza, Dao-Ling Huang, Teng-Teng Chen, Jing Su, Ping Yang, Xin Chen, Lai-Sheng Wang and Jun Li
Chemical Science 2016 vol. 7(Issue 1) pp:475-481
Publication Date(Web):13 Oct 2015
DOI:10.1039/C5SC03568F
We report a joint photoelectron spectroscopy and theoretical investigation of the gaseous Au2I3− cluster, which is found to exhibit two types of isomers due to competition between Au–I covalent bonding and Au–Au aurophilic interactions. The covalent bonding favors a bent IAuIAuI− structure with an obtuse Au–I–Au angle (100.7°), while aurophilic interactions pull the two Au atoms much closer, leading to an acutely bent structure (72.0°) with an Au–Au distance of 3.08 Å. The two isomers are separated by a small barrier and are nearly degenerate with the obtuse isomer being slightly more stable. At low temperature, only the obtuse isomer is observed; distinct experimental evidence is observed for the co-existence of a combination of isomers with both acute and obtuse bending angles at room temperature. The two bond-bending isomers of Au2I3− reveal a unique example of one molecule being able to oscillate between different structures as a result of two competing chemical forces.
Co-reporter:Hou-Ji Cao, Qianyi Zhao, Qian-Fan Zhang, Jiaxuan Li, Ewan J. M. Hamilton, Jie Zhang, Lai-Sheng Wang and Xuenian Chen
Dalton Transactions 2016 vol. 45(Issue 25) pp:10194-10199
Publication Date(Web):28 Apr 2016
DOI:10.1039/C6DT01272H
Agostic interactions are often used to activate inert C–H bonds, and thus facilitate new reactions. We report the first example of designed catalysts based on the agostic interaction. Novel copper(I) complexes [BBN(pzx)2]Cu(PPh3)n (BBN = 9-borabicyclo[3.3.1]nonane; pzx = 3-substituted pyrazole; x = H, n = 2; x = Me, n = 1) and {[BBN(pziPr)2]Cu}2 have been synthesized and characterized. Single crystal studies of the three compounds show weak intramolecular C–H⋯Cu interactions which can be assigned as agostic or anagostic interactions. Catalytic studies of these complexes toward carbenoid insertion into N–H bonds indicate these weak interactions act as a “switch” which will be turned “on” if interacting with the substrate and “off” if eliminating the product and regenerating the weak interaction. The process of the “switch” turning “on” or “off”, which is related to the catalytic effect, is found to be influenced by both steric effects and the solvent: a less sterically hindered catalyst in non-coordinating benzene results in high yield, while a more sterically hindered catalyst in coordinating THF results in relatively low yield.
Co-reporter:Alexander I. Boldyrev and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2016 vol. 18(Issue 17) pp:11589-11605
Publication Date(Web):28 Jan 2016
DOI:10.1039/C5CP07465G
We describe joint experimental and theoretical studies carried out collaboratively in the authors' labs for understanding the structures and chemical bonding of novel atomic clusters, which exhibit aromaticity. The concept of aromaticity was first discovered to be useful in understanding the square-planar unit of Al4 in a series of MAl4− bimetallic clusters that led to discoveries of aromaticity in many metal cluster systems, including transition metals and similar cluster motifs in solid compounds. The concept of aromaticity has been found to be particularly powerful in understanding the stability and bonding in planar boron clusters, many of which have been shown to be analogous to polycyclic aromatic hydrocarbons in their π bonding. Stimulated by the multiple aromaticity in planar boron clusters, a design principle has been proposed for stable metal-cerntered aromatic molecular wheels of the general formula, M@Bnk−. A series of such borometallic aromatic wheel complexes have been produced in supersonic cluster beams and characterized experimentally and theoretically, including Ta@B10− and Nb@B10−, which exhibit the highest coordination number in two dimensions.
Co-reporter:Tian Jian, Gary V. Lopez, and Lai-Sheng Wang
The Journal of Physical Chemistry B 2016 Volume 120(Issue 8) pp:1635-1640
Publication Date(Web):October 5, 2015
DOI:10.1021/acs.jpcb.5b08327
Boronyl (BO) is a monovalent σ radical with a B≡O triple bond. Its chemistry has remained relatively unknown, though analogy has been established for BO with monovalent atoms, such as H or Au. Here we report a photoelectron spectroscopic study of BiAu– and BiBO–, showing further evidence of the analogy between Au and BO. The photoelectron spectra of BiAu– and BiBO– are found to be similar, suggesting that they possess similar electronic structure and chemical bonding. The electron affinities of BiAu and BiBO are measured to be 1.38(4) and 1.84(3) eV, respectively. The ground states of both BiAu and BiBO are shown to be a triplet (X 3Σ–). In addition, vibrational structures are resolved in the spectra of BiBO–. Two vibrational frequencies at 320(30) and 1860(50) cm–1 are measured for the ground state of BiBO, corresponding to the Bi–B and B–O stretching modes, respectively. The low-lying electronic excited states of BiAu and BiBO are also found to be similar: their first four excited states are A 1Δ, B 1Σ+, C 3Π, and D 1Π, with excitation energies at 0.71, 1.29, 2.54, and 2.67 eV for BiAu and 0.63, 1.26, 3.68, and 3.82 eV for BiBO, respectively, above the 3Σ– ground state. Weak photoelectron features related to two-electron detachment transitions are also observed for both anions because of strong electron correlation effects in the ground state of the anions.
Co-reporter:Jing Su, Wei-Li Li, Gary V. Lopez, Tian Jian, Guo-Jin Cao, Wan-Lu Li, W. H. Eugen Schwarz, Lai-Sheng Wang, and Jun Li
The Journal of Physical Chemistry A 2016 Volume 120(Issue 7) pp:1084-1096
Publication Date(Web):January 29, 2016
DOI:10.1021/acs.jpca.5b11354
Uranium oxide clusters UOx– (x = 3–5) were produced by laser vaporization and characterized by photoelectron spectroscopy and quantum theory. Photoelectron spectra were obtained for UOx– at various photon energies with well-resolved detachment transitions and vibrational resolution for x = 3 and 4. The electron affinities of UOx were measured as 1.12, 3.60, and 4.02 eV for x = 3, 4, and 5, respectively. The geometric and electronic structures of both the anions and the corresponding neutrals were investigated by quasi-relativistic electron-correlation quantum theory to interpret the photoelectron spectra and to provide insight into their chemical bonding. For UOx clusters with x ≤ 3, the O atoms appear as divalent closed-shell anions around the U atom, which is in various oxidation states from UII(fds)4 in UO to UVI(fds)0 in UO3. For x > 3, there are no longer sufficient valence electrons from the U atom to fill the O(2p) shell, resulting in fractionally charged and multicenter delocalized valence states for the O ligands as well as η1- or η2-bonded O2 units, with unusual spin couplings and complicated electron correlations in the unfilled poly oxo shell. The present work expands our understanding of both the bonding capacities of actinide elements with extended spdf valence shells as well as the multitude of oxygen’s charge and bonding states.
Co-reporter:Seema Pande, Wei Huang, Nan Shao, Lei-Ming Wang, Navneet Khetrapal, Wai-Ning Mei, Tian Jian, Lai-Sheng Wang, and Xiao Cheng Zeng
ACS Nano 2016 Volume 10(Issue 11) pp:10013
Publication Date(Web):October 30, 2016
DOI:10.1021/acsnano.6b04330
Gold nanoclusters have attracted great attention in the past decade due to their remarkable size-dependent electronic, optical, and catalytic properties. However, the structures of large gold clusters are still not well-known because of the challenges in global structural searches. Here we report a joint photoelectron spectroscopy (PES) and theoretical study of the structural evolution of negatively charged core–shell gold nanoclusters (Aun–) for n = 42–50. Photoelectron spectra of size-selected Aun– clusters are well resolved with distinct spectral features, suggesting a dominating structural type. The combined PES data and density functional calculations allow us to systematically identify the global minimum or candidates of the global minima of these relatively large gold nanoclusters, which are found to possess low-symmetry structures with gradually increasing core sizes. Remarkably, the four-atom tetrahedral core, observed first in Au33–, continues to be highly robust and is even present in clusters as large as Au42–. Starting from Au43–, a five-atom trigonal bipyramidal core appears and persists until Au47–. Au48– possesses a six-atom core, while Au49– and Au50– feature seven- and eight-atom cores, respectively. Notably, both Au46– and Au47– contain a pyramidal Au20 motif, which is stacked with another truncated pyramid by sharing a common 10-atom triangular face. The present study sheds light on our understanding of the structural evolution of the medium-sized gold nanoclusters, the shells and core as well as how the core–shell structures may start to embrace the golden pyramid (bulk-like) fragment.Keywords: core−shell structures; gold anion clusters; gold nanoclusters; photoelectron spectroscopy; structural evolution
Co-reporter:Dao-Ling Huang, Hong-Tao Liu, Chuan-Gang Ning, Guo-Zhu Zhu and Lai-Sheng Wang
Chemical Science 2015 vol. 6(Issue 5) pp:3129-3138
Publication Date(Web):17 Mar 2015
DOI:10.1039/C5SC00704F
Deprotonated thymine can exist in two different forms, depending on which of its two N sites is deprotonated: N1[T–H]− or N3[T–H]−. Here we report a photodetachment study of the N1[T–H]− isomer cooled in a cryogenic ion trap and the observation of an excited dipole-bound state. Eighteen vibrational levels of the dipole-bound state are observed, and its vibrational ground state is found to be 238 ± 5 cm−1 below the detachment threshold of N1[T–H]−. The electron affinity of the deprotonated thymine radical (N1[T–H]˙) is measured accurately to be 26322 ± 5 cm−1 (3.2635 ± 0.0006 eV). By tuning the detachment laser to the sixteen vibrational levels of the dipole-bound state that are above the detachment threshold, highly non-Franck–Condon resonant-enhanced photoelectron spectra are obtained due to state- and mode-selective vibrational autodetachment. Much richer vibrational information is obtained for the deprotonated thymine radical from the photodetachment and resonant-enhanced photoelectron spectroscopy. Eleven fundamental vibrational frequencies in the low-frequency regime are obtained for the N1[T–H]˙ radical, including the two lowest-frequency internal rotational modes of the methyl group at 70 ± 8 cm−1 and 92 ± 5 cm−1.
Co-reporter:Xiao-Gen Xiong, Yi-Lei Wang, Cong-Qiao Xu, Yi-Heng Qiu, Lai-Sheng Wang and Jun Li
Dalton Transactions 2015 vol. 44(Issue 12) pp:5535-5546
Publication Date(Web):03 Feb 2015
DOI:10.1039/C4DT04031G
Gold compounds, clusters, and nanoparticles are widely used as catalysts and therapeutic medicines; the interactions between gold and its ligands in these systems play important roles in their chemical properties and functionalities. In order to elucidate the nature of the chemical interactions between Au(I) and its ligands, herein we use several theoretical methods to study the chemical bonding in a variety of linear [AuX2]− complexes, where X = halogen atoms (F, Cl, Br, I, At and Uus), H, OH, SH, OCH3, SCH3, CN and SCN. It is shown that the most important bonding orbitals in these systems have significant contributions from the Au sd hybridized atomic orbitals. The ubiquitous linear or quasi-linear structures of [AuX2]− are attributed to the well-balanced optimal overlap in both σ and π bonding orbitals and minimal repulsion between the two negatively charged ligands. The stability of these complexes is related to the covalency of the Au–X bond and a periodic trend is found in the evolution of covalency along the halogen group ligands. The special stability of [Au(CN)2]− is a result of strong covalent and ionic interactions. For the superheavy element Uus, the covalency of Au–Uus is enhanced through the spin–orbit interactions.
Co-reporter:Qiang Chen, Wei-Li Li, Ya-Fan Zhao, Su-Yan Zhang, Han-Shi Hu, Hui Bai, Hai-Ru Li, Wen-Juan Tian, Hai-Gang Lu, Hua-Jin Zhai, Si-Dian Li, Jun Li, and Lai-Sheng Wang
ACS Nano 2015 Volume 9(Issue 1) pp:754
Publication Date(Web):December 17, 2014
DOI:10.1021/nn506262c
Chirality plays an important role in chemistry, biology, and materials science. The recent discovery of the B40–/0 borospherenes marks the onset of a class of boron-based nanostructures. Here we report the observation of axially chiral borospherene in the B39– nanocluster on the bases of photoelectron spectroscopy, global minimum searches, and electronic structure calculations. Extensive structural searches in combination with density functional and CCSD(T) calculations show that B39– has a C3 cage global minimum with a close-lying C2 cage isomer. Both the C3 and C2 B39– cages are chiral with degenerate enantiomers. The C3 global minimum consists of three hexagons and three heptagons around the vertical C3 axis. The C2 isomer is built on two hexagons on the top and at the bottom of the cage with four heptagons around the waist. Both the C3 and C2 axially chiral isomers of B39– are present in the experiment and contribute to the observed photoelectron spectrum. The chiral borospherenes also exhibit three-dimensional aromaticity, featuring σ and π double delocalization for all valence electrons. Molecular dynamics simulations reveal that these chiral B39– cages are structurally fluxional above room temperature, compared to the highly robust D2d B40 borospherene. The current findings add chiral members to the borospherene family and indicate the structural diversity of boron-based nanomaterials.Keywords: all-boron fullerene; axial chirality; borospherene; global minimum searches; photoelectron spectroscopy; σ and π double delocalization;
Co-reporter:Hong-Tao Liu; Dao-Ling Huang; Yuan Liu; Ling-Fung Cheung; Phuong Diem Dau; Chuan-Gang Ning
The Journal of Physical Chemistry Letters 2015 Volume 6(Issue 4) pp:637-642
Publication Date(Web):January 30, 2015
DOI:10.1021/acs.jpclett.5b00053
Vibrational state-selective resonant two-photon photoelectron spectra have been obtained via a triplet intermediate state (3Σ–) of AuS– near its detachment threshold using high-resolution photoelectron imaging of cryogenically cooled AuS– anions. Four vibrational levels of the 3Σ– excited state are observed to be below the detachment threshold. Resonant two-photon absorptions through these levels yield vibrational state-selective photoelectron spectra to the 2Σ final state of neutral AuS with broad and drastically different Franck–Condon distributions, reflecting the symmetries of the vibrational wave functions of the 3Σ– intermediate state. The 3Σ– excited state is spin-forbidden from the 1Σ+ ground state of AuS– and is accessed due to strong relativistic effects. The nature of the 3Σ– excited state is confirmed by angular distributions of the photoelectron images and quantum calculations.
Co-reporter:Dao-Ling Huang; Hong-Tao Liu; Chuan-Gang Ning
The Journal of Physical Chemistry Letters 2015 Volume 6(Issue 12) pp:2153-2157
Publication Date(Web):May 26, 2015
DOI:10.1021/acs.jpclett.5b00963
Molecular conformation is important in chemistry and biochemistry. Conformers connected by low energy barriers can only be observed at low temperatures and are difficult to be separated. Here we report a new method to obtain conformation-selective spectroscopic information about dipolar molecular radicals via dipole-bound excited states of the corresponding anions cooled in a cryogenic ion trap. We observed two conformers of cold 3-hydroxyphenoxide anions [m-HO(C6H4)O–] in high-resolution photoelectron spectroscopy and measured different electron affinities, 18 850(8) and 18 917(5) cm–1, for the syn and anti 3-hydroxyphenoxy radicals, respectively. We also observed dipole-bound excited states for m-HO(C6H4)O– with different binding energies for the two conformers due to the different dipole moments of the corresponding 3-hydroxyphenoxy radicals. Excitations to selected vibrational levels of the dipole-bound states result in conformation-selective photoelectron spectra. This method should be applicable to conformation-selective spectroscopic studies of any anions with dipolar neutral cores.
Co-reporter:Alina P. Sergeeva, Ivan A. Popov, Zachary A. Piazza, Wei-Li Li, Constantin Romanescu, Lai-Sheng Wang, and Alexander I. Boldyrev
Accounts of Chemical Research 2014 Volume 47(Issue 4) pp:1349
Publication Date(Web):March 24, 2014
DOI:10.1021/ar400310g
Boron is an interesting element with unusual polymorphism. While three-dimensional (3D) structural motifs are prevalent in bulk boron, atomic boron clusters are found to have planar or quasi-planar structures, stabilized by localized two-center–two-electron (2c–2e) σ bonds on the periphery and delocalized multicenter–two-electron (nc–2e) bonds in both σ and π frameworks. Electron delocalization is a result of boron’s electron deficiency and leads to fluxional behavior, which has been observed in B13+ and B19–. A unique capability of the in-plane rotation of the inner atoms against the periphery of the cluster in a chosen direction by employing circularly polarized infrared radiation has been suggested. Such fluxional behaviors in boron clusters are interesting and have been proposed as molecular Wankel motors. The concepts of aromaticity and antiaromaticity have been extended beyond organic chemistry to planar boron clusters. The validity of these concepts in understanding the electronic structures of boron clusters is evident in the striking similarities of the π-systems of planar boron clusters to those of polycyclic aromatic hydrocarbons, such as benzene, naphthalene, coronene, anthracene, or phenanthrene. Chemical bonding models developed for boron clusters not only allowed the rationalization of the stability of boron clusters but also lead to the design of novel metal-centered boron wheels with a record-setting planar coordination number of 10. The unprecedented highly coordinated borometallic molecular wheels provide insights into the interactions between transition metals and boron and expand the frontier of boron chemistry. Another interesting feature discovered through cluster studies is boron transmutation. Even though it is well-known that B–, formed by adding one electron to boron, is isoelectronic to carbon, cluster studies have considerably expanded the possibilities of new structures and new materials using the B–/C analogy. It is believed that the electronic transmutation concept will be effective and valuable in aiding the design of new boride materials with predictable properties.The study of boron clusters with intermediate properties between those of individual atoms and bulk solids has given rise to a unique opportunity to broaden the frontier of boron chemistry. Understanding boron clusters has spurred experimentalists and theoreticians to find new boron-based nanomaterials, such as boron fullerenes, nanotubes, two-dimensional boron, and new compounds containing boron clusters as building blocks. Here, a brief and timely overview is presented addressing the recent progress made on boron clusters and the approaches used in the authors’ laboratories to determine the structure, stability, and chemical bonding of size-selected boron clusters by joint photoelectron spectroscopy and theoretical studies. Specifically, key findings on all-boron hydrocarbon analogues, metal-centered boron wheels, and electronic transmutation in boron clusters are summarized.
Co-reporter:Wei-Li Li ; Qiang Chen ; Wen-Juan Tian ; Hui Bai ; Ya-Fan Zhao ; Han-Shi Hu ; Jun Li ; Hua-Jin Zhai ; Si-Dian Li
Journal of the American Chemical Society 2014 Volume 136(Issue 35) pp:12257-12260
Publication Date(Web):August 20, 2014
DOI:10.1021/ja507235s
Elemental boron is electron-deficient and cannot form graphene-like structures. Instead, triangular boron lattices with hexagonal vacancies have been predicted to be stable. A recent experimental and computational study showed that the B36 cluster has a planar C6v structure with a central hexagonal hole, providing the first experimental evidence for the viability of atom-thin boron sheets with hexagonal vacancies, dubbed borophene. Here we report a boron cluster with a double-hexagonal vacancy as a new and more flexible structural motif for borophene. Photoelectron spectrum of B35– displays a simple pattern with certain similarity to that of B36–. Global minimum searches find that both B35– and B35 possess planar hexagonal structures, similar to that of B36, except a missing interior B atom that creates a double-hexagonal vacancy. The closed-shell B35– is found to exhibit triple π aromaticity with 11 delocalized π bonds, analogous to benzo(g,h,i)perylene (C22H12). The B35 cluster can be used to build atom-thin boron sheets with various hexagonal hole densities, providing further experimental evidence for the viability of borophene.
Co-reporter:Jing Chen, Qian-Fan Zhang, Paul G. Williard, and Lai-Sheng Wang
Inorganic Chemistry 2014 Volume 53(Issue 8) pp:3932-3934
Publication Date(Web):March 31, 2014
DOI:10.1021/ic500562r
We report the synthesis and structure determination of a new Au20 nanocluster coordinated by four tripodal tetraphosphine (PP3) ligands {PP3 = tris[2-(diphenylphosphino)ethyl]phosphine}. Single-crystal X-ray crystallography and electrospray ionization mass spectrometry show that the cluster assembly can be formulated as [Au20(PP3)4]Cl4. The Au20 cluster consists of an icosahedral Au13 core and a seven-Au-atom partial outer shell arranged in a local C3 symmetry. One PP3 ligand coordinates to four Au atoms in the outer shell, while the other three PP3 ligands coordinate to one Au atom from the outer shell and three Au atoms from the surface of the Au13 core, giving rise to an overall chiral 16-electron Au cluster core with C3 symmetry.
Co-reporter:Bastian Schaefer, Rhitankar Pal, Navneet S. Khetrapal, Maximilian Amsler, Ali Sadeghi, Volker Blum, Xiao Cheng Zeng, Stefan Goedecker, and Lai-Sheng Wang
ACS Nano 2014 Volume 8(Issue 7) pp:7413
Publication Date(Web):June 24, 2014
DOI:10.1021/nn502641q
Using the minima hopping global optimization method at the density functional level, we found low-energy nanostructures for neutral Au26 and its anion. The local-density and a generalized gradient approximation of the exchange–correlation functional predict different nanoscale motifs. We found a vast number of isomers within a small energy range above the respective putative global minima with each method. Photoelectron spectroscopy of Au26– under different experimental conditions revealed definitive evidence of the presence of multiple isomers, consistent with the theoretical predictions. Comparison between the experimental and simulated photoelectron spectra suggests that the photoelectron spectra of Au26– contain a mixture of three isomers, all of which are low-symmetry core–shell-type nanoclusters with a single internal Au atom. We present a disconnectivity graph for Au26– that has been computed completely at the density functional level. The transition states used to build this disconnectivity graph are complete enough to predict Au26– to have a possible fluxional shell, which facilitates the understanding of its catalytic activity.Keywords: BigDFT; density functional theory; gold nanoclusters; minima hopping; photoelectron spectroscopy
Co-reporter:Nan Shao ; Wei Huang ; Wai-Ning Mei ; Lai Sheng Wang ; Qin Wu ;Xiao Cheng Zeng
The Journal of Physical Chemistry C 2014 Volume 118(Issue 13) pp:6887-6892
Publication Date(Web):February 26, 2014
DOI:10.1021/jp500582t
We report a joint experimental and theoretical study of the structural evolution of medium-sized gold clusters. We find that the most stable structures of Au36– to Au38– exhibit core–shell type structures all with a highly robust tetrahedral four-atom core. All three clusters are observed to possess two coexisting isomers in the cluster beam. The appearance of a fragment of the face centered cubic (FCC) bulk gold, that is, the pyramidal Au20–, at the size of Au38– implies that the cluster-to-bulk transformation starts to emerge at the medium size range. It is expected that larger pyramidal-like intermediates may emerge in later medium- to large-sized Au clusters beyond Au38–.
Co-reporter:Yusuf Erdogdu, Tian Jian, Gary V. Lopez, Wei-Li Li, Lai-Sheng Wang
Chemical Physics Letters 2014 s 610–611() pp: 23-28
Publication Date(Web):
DOI:10.1016/j.cplett.2014.07.018
Co-reporter:Gary V. Lopez, Tian Jian, Wei-Li Li, and Lai-Sheng Wang
The Journal of Physical Chemistry A 2014 Volume 118(Issue 28) pp:5204-5211
Publication Date(Web):June 25, 2014
DOI:10.1021/jp504236s
We have produced an auro–aluminum oxide cluster, Au2(AlO)2–, as a possible model for an Au–alumina interface and investigated its electronic and structural properties using photoelectron spectroscopy and density functional theory. An extremely large energy gap (3.44 eV) is observed between the lowest unoccupied and the highest occupied molecular orbitals of Au2(AlO)2, suggesting its high electronic stability. The global minima of both Au2(AlO)2– and Au2(AlO)2 are found to have D2h symmetry with the two Au atoms bonded to the Al atoms of a nearly square-planar (AlO)2 unit. Chemical bonding analyses reveal a strong σ bond between Au and Al, as well as a completely delocalized π bond over the (AlO)2 unit, rendering aromatic character to the Au2(AlO)2 cluster. The high electronic stability and novel chemical bonding uncovered for Au2(AlO)2 suggest that it may be susceptible to chemical syntheses as a stable compound if appropriate ligands can be found.
Co-reporter:Ivan A. Popov, Wei-Li Li, Zachary A. Piazza, Alexander I. Boldyrev, and Lai-Sheng Wang
The Journal of Physical Chemistry A 2014 Volume 118(Issue 37) pp:8098-8105
Publication Date(Web):January 15, 2014
DOI:10.1021/jp411867q
Small boron clusters are known to be planar, and may be used as ligands to form novel coordination complexes with transition metals. Here we report a combined photoelectron spectroscopy and ab initio study of CoB12– and RhB12–. Photoelectron spectra of the two doped-B12 clusters show similar spectral patterns, suggesting they have similar structures. Global minimum searches reveal that both CoB12– and RhB12– possess half-sandwich-type structures with the quasi-planar B12 moiety coordinating to the metal atom. The B12 ligand is found to have similar structure as the bare B12 cluster with C3v symmetry. Structures with Co or Rh inserted into the quasi-planar boron framework are found to be much higher in energy. Chemical bonding analyses of the two B12 half sandwiches reveal two sets of σ bonds on the boron unit: nine classical two-center–two-electron (2c–2e) σ bonds on the periphery of the B12 unit and four 3c–2e σ bonds within the boron unit. Both σ and π bonds are found between the metal and the B12 ligand: three M–B single σ bonds and one delocalized 4c–2e π bond. The exposed metal sites in these complexes can be further coordinated by other ligands or become reaction centers as model catalysts.
Co-reporter:Dr. Hong-Tao Liu;Dr. Chuan-Gang Ning;Dao-Ling Huang;Dr. Lai-Sheng Wang
Angewandte Chemie 2014 Volume 126( Issue 9) pp:2496-2500
Publication Date(Web):
DOI:10.1002/ange.201310323
Abstract
Molecules with large enough dipole moments can bind an electron by the dipole field, which has little effect on the molecular core. A molecular anion can be excited to a dipole-bound state, which can autodetach by vibronic coupling. Autodetachment spectroscopy of a complex anion cooled in a cryogenic ion trap is reported. Vibrational spectroscopy of the dehydrogenated uracil radical is obtained by a dipole-bound state with partial rotational resolution. Fundamental frequencies for 21 vibrational modes of the uracil radical are reported. The electron affinity of the uracil radical is measured accurately to be 3.4810±0.0006 eV and the binding energy of the dipole-bound state is measured to be 146±5 cm−1. The rotational temperature of the trapped uracil anion is evaluated to be 35 K.
Co-reporter:Wei-Li Li;Dr. Ya-Fan Zhao;Dr. Han-Shi Hu;Dr. Jun Li;Dr. Lai-Sheng Wang
Angewandte Chemie International Edition 2014 Volume 53( Issue 22) pp:
Publication Date(Web):
DOI:10.1002/anie.201482271
Co-reporter:Wei-Li Li;Dr. Ya-Fan Zhao;Dr. Han-Shi Hu;Dr. Jun Li;Dr. Lai-Sheng Wang
Angewandte Chemie International Edition 2014 Volume 53( Issue 22) pp:5540-5545
Publication Date(Web):
DOI:10.1002/anie.201402488
Abstract
Chirality is vital in chemistry. Its importance in atomic clusters has been recognized since the discovery of the first chiral fullerene, the D2 symmetric C76.1 A number of gold clusters have been found to be chiral,2 raising the possibility to use them as asymmetric catalysts. The discovery of clusters with enantiomeric structures is essential to design new chiral materials with tailored chemical and physical properties.3 Herein we report the first inherently chiral boron cluster of [B30]− in a joint photoelectron spectroscopy and theoretical study. The most stable structure of [B30]− is found to be quasiplanar with a hexagonal hole. Interestingly, a pair of enantiomers arising from different positions of the hexagonal hole are found to be degenerate in our global minimum searches and both should co-exist experimentally because they have identical electronic structures and give rise to identical simulated photoelectron spectra.
Co-reporter:Dr. Hong-Tao Liu;Dr. Chuan-Gang Ning;Dao-Ling Huang;Dr. Lai-Sheng Wang
Angewandte Chemie International Edition 2014 Volume 53( Issue 9) pp:2464-2468
Publication Date(Web):
DOI:10.1002/anie.201310323
Abstract
Molecules with large enough dipole moments can bind an electron by the dipole field, which has little effect on the molecular core. A molecular anion can be excited to a dipole-bound state, which can autodetach by vibronic coupling. Autodetachment spectroscopy of a complex anion cooled in a cryogenic ion trap is reported. Vibrational spectroscopy of the dehydrogenated uracil radical is obtained by a dipole-bound state with partial rotational resolution. Fundamental frequencies for 21 vibrational modes of the uracil radical are reported. The electron affinity of the uracil radical is measured accurately to be 3.4810±0.0006 eV and the binding energy of the dipole-bound state is measured to be 146±5 cm−1. The rotational temperature of the trapped uracil anion is evaluated to be 35 K.
Co-reporter:Wei-Li Li;Lu Xie;Tian Jian;Dr. Constantin Romanescu;Dr. Xin Huang;Dr. Lai-Sheng Wang
Angewandte Chemie International Edition 2014 Volume 53( Issue 5) pp:1288-1292
Publication Date(Web):
DOI:10.1002/anie.201309469
Abstract
It has been a long-sought goal in cluster science to discover stable atomic clusters as building blocks for cluster-assembled nanomaterials, as exemplified by the fullerenes and their subsequent bulk syntheses.1, 2 Clusters have also been considered as models to understand bulk properties, providing a bridge between molecular and solid-state chemistry.3 Because of its electron deficiency, boron is an interesting element with unusual polymorphism. While bulk boron is known to be dominated by the three-dimensional (3D) B12 icosahedral motifs,4 new forms of elemental boron are continuing to be discovered.5 In contrast to the 3D cages commonly found in bulk boron, in the gas phase two-dimensional (2D) boron clusters are prevalent.6–8 The unusual planar boron clusters have been suggested as potential new bulking blocks or ligands in chemistry.6a Herein we report a joint experimental and theoretical study on the [Ta2B6]− and [Ta2B6] clusters. We found that the most stable structures of both the neutral and anion are D6h bipyramidal, similar to the recently discovered MB6M structural motif in the Ti7Rh4Ir2B8 solid compound.9
Co-reporter:Constantin Romanescu, Timur R. Galeev, Wei-Li Li, Alexander I. Boldyrev, and Lai-Sheng Wang
Accounts of Chemical Research 2013 Volume 46(Issue 2) pp:350
Publication Date(Web):December 5, 2012
DOI:10.1021/ar300149a
Atomic clusters have intermediate properties between that of individual atoms and bulk solids, which provide fertile ground for the discovery of new molecules and novel chemical bonding. In addition, the study of small clusters can help researchers design better nanosystems with specific physical and chemical properties. From recent experimental and computational studies, we know that small boron clusters possess planar structures stabilized by electron delocalization both in the σ and π frameworks. An interesting boron cluster is B9–, which has a D8h molecular wheel structure with a single boron atom in the center of a B8 ring. This ring in the D8h-B9– cluster is connected by eight classical two-center, two-electron bonds. In contrast, the cluster’s central boron atom is bonded to the peripheral ring through three delocalized σ and three delocalized π bonds. This bonding structure gives the molecular wheel double aromaticity and high electronic stability. The unprecedented structure and bonding pattern in B9– and other planar boron clusters have inspired the designs of similar molecular wheel-type structures. But these mimics instead substitute a heteroatom for the central boron.Through recent experiments in cluster beams, chemists have demonstrated that transition metals can be doped into the center of the planar boron clusters. These new metal-centered monocyclic boron rings have variable ring sizes, M©Bn and M©Bn– with n = 8–10. Using size-selected anion photoelectron spectroscopy and ab initio calculations, researchers have characterized these novel borometallic molecules. Chemists have proposed a design principle based on σ and π double aromaticity for electronically stable borometallic cluster compounds, featuring a highly coordinated transition metal atom centered inside monocyclic boron rings. The central metal atom is coordinatively unsaturated in the direction perpendicular to the molecular plane. Thus, chemists may design appropriate ligands to synthesize the molecular wheels in the bulk. In this Account, we discuss these recent experimental and theoretical advances of this new class of aromatic borometallic compounds, which contain a highly coordinated central transition metal atom inside a monocyclic boron ring. Through these examples, we show that atomic clusters can facilitate the discovery of new structures, new chemical bonding, and possibly new nanostructures with specific, advantageous properties.
Co-reporter:Jing Chen ; Qian-Fan Zhang ; Timary A. Bonaccorso ; Paul G. Williard
Journal of the American Chemical Society 2013 Volume 136(Issue 1) pp:92-95
Publication Date(Web):December 16, 2013
DOI:10.1021/ja411061e
We report the synthesis and structure determination of a new Au22 nanocluster coordinated by six bidentate diphosphine ligands: 1,8-bis(diphenylphosphino) octane (L8 for short). Single crystal X-ray crystallography and electrospray ionization mass spectrometry show that the cluster assembly is neutral and can be formulated as Au22(L8)6. The Au22 core consists of two Au11 units clipped together by four L8 ligands, while the additional two ligands coordinate to each Au11 unit in a bidentate fashion. Eight gold atoms at the interface of the two Au11 units are not coordinated by any ligands. Four short gold–gold distances (2.64–2.65 Å) are observed at the interface of the two Au11 clusters as a result of the clamping force of the four clipping ligands and strong electronic interactions. The eight uncoordinated surface gold atoms in the Au22(L8)6 nanocluster are unprecedented in atom-precise gold nanoparticles and can be considered as potential in situ active sites for catalysis.
Co-reporter:Jing Su, Phuong Diem Dau, Yi-Heng Qiu, Hong-Tao Liu, Chao-Fei Xu, Dao-Ling Huang, Lai-Sheng Wang, and Jun Li
Inorganic Chemistry 2013 Volume 52(Issue 11) pp:6617-6626
Publication Date(Web):May 10, 2013
DOI:10.1021/ic4006482
While uranyl halide complexes [UO2(halogen)n]2–n (n = 1, 2, 4) are ubiquitous, the tricoordinate species have been relatively unknown until very recently. Here photoelectron spectroscopy and relativistic quantum chemistry are used to investigate the bonding and stability of a series of gaseous tricoordinate uranyl complexes, UO2X3– (X = F, Cl, Br, I). Isolated UO2X3– ions are produced by electrospray ionization and observed to be highly stable with very large adiabatic electron detachment energies: 6.25, 6.64, 6.27, and 5.60 eV for X = F, Cl, Br, and I, respectively. Theoretical calculations reveal that the frontier molecular orbitals are mainly of uranyl U–O bonding character in UO2F3–, but they are from the ligand valence np lone pairs in the heavier halogen complexes. Extensive bonding analyses are carried out for UO2X3– as well as for the doubly charged tetracoordinate complexes (UO2X42–), showing that the U–X bonds are dominated by ionic interactions with weak covalency. The U–X bond strength decreases down the periodic table from F to I. Coulomb barriers and dissociation energies of UO2X42– → UO2X3– + X– are calculated, revealing that all gaseous dianions are in fact metastable. The dielectric constant of the environment is shown to be the key in controlling the thermodynamic and kinetic stabilities of the tetracoordinate uranyl complexes via modulation of the ligand–ligand Coulomb repulsions.
Co-reporter:Marc-Oliver Winghart, Ji-Ping Yang, Michael Kühn, Andreas-Neil Unterreiner, Thomas J. A. Wolf, Phuong D. Dau, Hong-Tao Liu, Dao-Ling Huang, Wim Klopper, Lai-Sheng Wang and Manfred M. Kappes
Physical Chemistry Chemical Physics 2013 vol. 15(Issue 18) pp:6726-6736
Publication Date(Web):18 Mar 2013
DOI:10.1039/C3CP50497B
Photoelectron spectra of isolated [M–BDSZ]3− (BDSZ = bisdisulizole, M = H, Li, Na, K, Cs) triply charged anions exhibit a dominant constant electron kinetic energy (KE) detachment feature, independent of detachment wavelengths over a wide UV range. Photoelectron imaging spectroscopy shows that this constant KE feature displays an angular distribution consistent with delayed rather than direct electron emission. Time-resolved pump–probe (388 nm/775 nm) two-colour photoelectron spectroscopy reveals that the constant KE feature results from two simultaneously populated excited states, which decay at different rates. The faster of the two rates is essentially the same for all the [M–BDSZ]3− species, regardless of M. The slower process is associated with lifetimes ranging from several picoseconds to tens of picoseconds. The lighter the alkali cation is, the longer the lifetime of this state. Quantum chemical calculations indicate that the two decaying states are in fact the two lowest singlet excited states of the trianions. Each of the two corresponding photoexcitations is associated with significant charge transfer. However, electron density is transferred from different ends of the roughly chain-like molecule to its aromatic center. The energy (and therefore the decay rate) of the longer-lived excited state is found to be influenced by polarization effects due to the proximal alkali cation complexed to that end of the molecule. Systematic M-dependent geometry changes, mainly due to the size of the alkali cation, lead to M-dependent shifts in transition energies. At the constant pump wavelength this leads to different amounts of vibrational energy in the respective excited state, contributing to the variations in decay rates. The current experiments and calculations confirm excited state electron tunneling detachment (ESETD) to be the mechanism responsible for the observed constant KE feature. The ESETD phenomenon may be quite common for isolated multiply charged anions, which are strong fluorophores in the condensed phase – making ESETD useful for studies of the transient response of such species after electronic excitation.
Co-reporter:Hui Bai, Hua-Jin Zhai, Si-Dian Li and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2013 vol. 15(Issue 24) pp:9646-9653
Publication Date(Web):17 Apr 2013
DOI:10.1039/C3CP50167A
We report a photoelectron spectroscopy and density-functional theory study of the B12Au− and B13O− clusters and their neutrals, which are shown to be six π electron aromatic compounds between the quasi-planar all-boron B12 benzene-analogue and a monovalent Au or BO ligand. Electron affinities of B12Au and B13O are measured to be 3.48 ± 0.04 and 3.90 ± 0.04 eV, respectively. Structural searches are performed for B12Au− and B13O−, which are compared with the isovalent B12H− cluster. The global minima of B12Au− and B13O− both feature an almost intact B12 cluster with the Au and BO ligands bonded to its periphery, respectively. For B12Au−, a low-lying isomer is also identified, which is only 0.4 kcal mol−1 above the global minimum, in agreement with the experimental observation of a weakly populated isomer in the cluster beam of B12Au−. These aromatic compound clusters provide new examples for the Au/H isolobal analogy and the boronyl (BO) chemistry.
Co-reporter:Dr. Hong-Tao Liu;Dr. Chuan-Gang Ning;Dao-Ling Huang;Phuong Diem Dau;Dr. Lai-Sheng Wang
Angewandte Chemie 2013 Volume 125( Issue 34) pp:9146-9149
Publication Date(Web):
DOI:10.1002/ange.201304695
Co-reporter:Dr. Jing Su;Phuong Diem Dau;Chao-Fei Xu;Dao-Ling Huang;Dr. Hong-Tao Liu;Dr. Fan Wei;Dr. Lai-Sheng Wang;Dr. Jun Li
Chemistry – An Asian Journal 2013 Volume 8( Issue 10) pp:
Publication Date(Web):
DOI:10.1002/asia.201390035
Co-reporter:Dr. Jing Su;Phuong Diem Dau;Chao-Fei Xu;Dao-Ling Huang;Dr. Hong-Tao Liu;Dr. Fan Wei;Dr. Lai-Sheng Wang;Dr. Jun Li
Chemistry – An Asian Journal 2013 Volume 8( Issue 10) pp:2489-2496
Publication Date(Web):
DOI:10.1002/asia.201300627
Abstract
We report a combined photoelectron spectroscopic and relativistic quantum chemistry study on gaseous UCl5− and UCl5. The UCl5− anion is produced using electrospray ionization and found to be highly electronically stable with an adiabatic electron binding energy of 4.76±0.03 eV, which also represents the electron affinity of the neutral UCl5 molecule. Theoretical investigations reveal that the ground state of UCl5− has an open shell with two unpaired electrons occupying two primarily U 5f and 5fxyz based molecular orbitals. The structures of both UCl5− and UCl5 are theoretically optimized and confirmed to have C4v symmetry. The computational results are in good agreement with the photoelectron spectra, providing insights into the electronic structures and valence molecular orbitals of UCl5− and UCl5. We also performed systematic theoretical studies on all the uranium pentahalide complexes UX5− (X=F, Cl, Br, I). Chemical bonding analyses indicate that the UX interactions in UX5− are dominated by ionic bonding, with increasing covalent contributions for the heavier halogen complexes.
Co-reporter:Hua-Jin Zhai, Wen-Jie Chen, Shu-Juan Lin, Xin Huang, and Lai-Sheng Wang
The Journal of Physical Chemistry A 2013 Volume 117(Issue 6) pp:1042-1052
Publication Date(Web):June 6, 2012
DOI:10.1021/jp302822p
The electronic and structural properties of monohafnium oxide clusters, HfOn– and HfOn (n = 1–6), are investigated using anion photoelectron spectroscopy and density-functional theory at the B3LYP level. The observed ground-state adiabatic detachment energy is low for HfO– (0.5 ± 0.1 eV) and HfO2– (2.125 ± 0.010 eV), roughly constant for HfO3– (3.6 ± 0.1 eV), HfO4– (3.67 ± 0.05 eV), and HfO5– (3.9 ± 0.1 eV), and substantially higher for HfO6– (4.9 ± 0.1 eV). Activated oxygen species, such as radical, superoxide, peroxide, diradical, and triradical, are identified in the HfOn– and HfOn clusters. The Hf center is shown to be flexible to accommodate the oxygen species. The sum of formal Hf–O bond orders around the Hf center is equal to four for all of the neutral clusters studied, and five for all of the anions. The O-rich HfOn– and HfOn (n = 3–6) clusters provide well-defined molecular models to understand O2 adsorption and activation on an Hf center.
Co-reporter:Dr. Hong-Tao Liu;Dr. Chuan-Gang Ning;Dao-Ling Huang;Phuong Diem Dau;Dr. Lai-Sheng Wang
Angewandte Chemie International Edition 2013 Volume 52( Issue 34) pp:8976-8979
Publication Date(Web):
DOI:10.1002/anie.201304695
Co-reporter:Alina P. Sergeeva ; Zachary A. Piazza ; Constantin Romanescu ; Wei-Li Li ; Alexander I. Boldyrev
Journal of the American Chemical Society 2012 Volume 134(Issue 43) pp:18065-18073
Publication Date(Web):October 3, 2012
DOI:10.1021/ja307605t
Clusters of boron atoms exhibit intriguing size-dependent structures and chemical bonding that are different from bulk boron and may lead to new boron-based nanostructures. We report a combined photoelectron spectroscopic and ab initio study of the 22- and 23-atom boron clusters. The joint experimental and theoretical investigation shows that B22– and B23– possess quasi-planar and planar structures, respectively. The quasi-planar B22– consists of fourteen peripheral atoms and eight interior atoms in a slightly buckled triangular lattice. Chemical bonding analyses of the closed-shell B222– species reveal seven delocalized π orbitals, which are similar to those in anthracene. B23– is a perfectly planar and heart-shaped cluster with a pentagonal cavity and a π-bonding pattern similar to that in phenanthrene. Thus, B22– and B23–, the largest negatively charged boron clusters that have been characterized experimentally to date, can be viewed as all-boron analogues of anthracene and phenanthrene, respectively. The current work shows not only that boron clusters are planar at very large sizes but also that they continue to yield surprises and novel chemical bonding analogous to specific polycyclic aromatic hydrocarbons.
Co-reporter:Rhitankar Pal ; Lei-Ming Wang ; Yong Pei ; Lai-Sheng Wang ;Xiao Cheng Zeng
Journal of the American Chemical Society 2012 Volume 134(Issue 22) pp:9438-9445
Publication Date(Web):May 9, 2012
DOI:10.1021/ja302902p
The activation of dioxygen is a key step in CO oxidation catalyzed by gold nanoparticles. It is known that small gold cluster anions with even-numbered atoms can molecularly chemisorb O2 via one-electron transfer from Aun– to O2, whereas clusters with odd-numbered atoms are inert toward O2. Here we report spectroscopic evidence of two modes of O2 activation by the small even-sized Aun– clusters: superoxo and peroxo chemisorption. Photoelectron spectroscopy of O2Au8– revealed two distinct isomers, which can be converted from one to the other depending on the reaction time. Ab initio calculations show that there are two close-lying molecular O2-chemisorbed isomers for O2Au8–: the lower energy isomer involves a peroxo-type binding of O2 onto Au8–, while the superoxo chemisorption is a slightly higher energy isomer. The computed detachment transitions of the superoxo and peroxo species are in good agreement with the experimental observation. The current work shows that there is a superoxo to peroxo chemisorption transition of O2 on gold clusters at Au8–: O2Aun– (n = 2, 4, 6) involves superoxo binding and n = 10, 12, 14, 18 involves peroxo binding, whereas the superoxo binding re-emerges at n = 20 due to the high symmetry tetrahedral structure of Au20, which has a very low electron affinity. Hence, the two-dimensional (2D) Au8– is the smallest anionic gold nanoparticle that prefers peroxo binding with O2. At Au12–, although both 2D and 3D isomers coexist in the cluster beam, the 3D isomer prefers the peroxo binding with O2.
Co-reporter:Wei-Li Li ; Constantin Romanescu ; Tian Jian
Journal of the American Chemical Society 2012 Volume 134(Issue 32) pp:13228-13231
Publication Date(Web):July 31, 2012
DOI:10.1021/ja305744a
Dihydrogenated boron clusters, H2Bn– (n = 7–12), were produced and characterized using photoelectron spectroscopy and computational chemistry to have ladderlike structures terminated by a hydrogen atom on each end. The two rows of boron atoms in the dihydrides are bonded by delocalized three-, four-, or five-center σ and π bonds. The π bonding patterns in these boron nanoladders bear similarities to those in conjugated alkenes: H2B7–, H2B8, and H2B9–, each with two π bonds, are similar to butadiene, while H2B102–, H2B11–, and H2B12, each with three π bonds, are analogous to 1,3,5-hexatriene. The boron cluster dihydrides can thus be considered as polyene analogues, or “polyboroenes”. Long polyboroenes with conjugated π bonds (analogous to polyacetylenes), which may form a new class of molecular wires, should exist.
Co-reporter:Hong-Tao Liu, Yi-Lei Wang, Xiao-Gen Xiong, Phuong Diem Dau, Zachary A. Piazza, Dao-Ling Huang, Cong-Qiao Xu, Jun Li and Lai-Sheng Wang
Chemical Science 2012 vol. 3(Issue 11) pp:3286-3295
Publication Date(Web):15 Aug 2012
DOI:10.1039/C2SC20984E
We report an investigation of the electronic structure and chemical bonding of AuH2− using photoelectron spectroscopy and ab initio calculations. We obtained vibrationally resolved photoelectron spectra of AuH2− at several photon energies. Six electronic states of AuH2 were observed and assigned according to the theoretical calculations. The ground state of AuH2− is known to be linear, while that of neutral AuH2 is bent with a ∠H–Au–H equilibrium bond angle of 129°. This large geometry change results in a very broad bending vibrational progression in the photoelectron spectra for the ground-state transition. The electron affinity of AuH2 is measured to be 3.030 ± 0.020 eV. A short bending vibrational progression is also observed in the second photodetachment band, suggesting a slightly bent structure for the first excited state of AuH2. The linear geometry is a saddle point for the ground and first excited states of AuH2, resulting in double-well potentials for these states along the bending coordinate. Spectroscopic evidence is observed for the detachment transitions to the double-well potentials of the ground and first excited states of AuH2. Higher excited states of AuH2 due to detachment from the nonbonding Au 5d electrons are all linear, similar to the anion ground state. Kohn–Sham molecular orbital analyses reveal surprising participation of H 2p orbitals in the Au–H chemical bonding and an unprecedented weak Au 5dπ to H 2pπ back donation. The simplicity of the linear AuH2− anion and its novel spectroscopic features make it a textbook example for understanding the covalent bonding properties and relativistic effects of Au.
Co-reporter:Phuong Diem Dau, Jing Su, Hong-Tao Liu, Jian-Biao Liu, Dao-Ling Huang, Jun Li and Lai-Sheng Wang
Chemical Science 2012 vol. 3(Issue 4) pp:1137-1146
Publication Date(Web):04 Jan 2012
DOI:10.1039/C2SC01052F
Bare uranyl tetrafluoride (UO2F42−) and its solvation complexes by one and two water or acetonitrile molecules have been observed in the gas phase using electrospray ionization and investigated by photoelectron spectroscopy and ab initio calculations. The isolated UO2F42− dianion is found to be electronically stable with an adiabatic electron binding energy of 1.10 ± 0.05 eV and a repulsive Coulomb barrier of ∼2 eV. Photoelectron spectra of UO2F42− display congested features due to detachment from U–O bonding orbitals and F 2p lone pairs. Solvated complexes by H2O and CH3CN, UO2F4(H2O)n2− and UO2F4(CH3CN)n2− (n = 1, 2), are also observed and their photoelectron spectra are similar to those of the bare UO2F42− dianion, suggesting that the solvent molecules are coordinated to the outer sphere of UO2F42− with relatively weak interactions between the solvent molecules and the dianion core. Both DFT and CCSD(T) calculations are performed on UO2F42− and its solvated species to understand the electronic structure of the dianion core and solute–solvent interactions. The strong U–F interactions with partial (d–p)π bonding are shown to weaken the UO bonds in the [OUO]2+ unit. Each H atom in the water molecules forms a H-bond to a F atom in the equatorial plane of UO2F42−, while each CH3CN molecule forms three H-bonds to two F ligands and one axial oxygen.
Co-reporter:Lei-Ming Wang and Lai-Sheng Wang
Nanoscale 2012 vol. 4(Issue 14) pp:4038-4053
Publication Date(Web):16 Mar 2012
DOI:10.1039/C2NR30186E
Gold nanoparticles have been discovered to exhibit remarkable catalytic properties in contrast to the chemical inertness of bulk gold. A prerequisite to elucidate the molecular mechanisms of the catalytic effect of nanogold is a detailed understanding of the structural and electronic properties of gold clusters as a function of size. In this review, we describe joint experimental studies (mainly photoelectron spectroscopy) and theoretical calculations to probe the structural properties of anionic gold clusters. Electronic properties and structural evolutions of all known Aun− clusters as experimentally confirmed to date are summarized, covering the size ranges of n = 3–35 and 55–64. Recent experimental efforts in resolving the isomeric issues of small gold clusters using Ar-tagging, O2-titration and isoelectronic substitution are also discussed.
Co-reporter:Wei-Li Li, Constantin Romanescu, Zachary A. Piazza and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2012 vol. 14(Issue 39) pp:13663-13669
Publication Date(Web):20 Aug 2012
DOI:10.1039/C2CP42218B
A class of transition-metal-centered aromatic boron wheels (Dnh-M©Bnq−) have been recently produced and characterized according to an electronic design principle. Here we investigate the interplay between electronic and geometric requirements for the molecular wheels using the case of VB10−, which is isoelectronic to the decacoordinated molecular wheels, Ta©B10− and Nb©B10−. Photoelectron spectra of VB10− are observed to be broad and complicated with relatively low electron binding energies, in contrast to the simple and high electron binding energies observed for the molecular wheels of its heavier congeners. An unbiased global minimum search found the most stable isomer of VB10− to be a singlet “boat”-like structure (C2), in which the V atom is coordinated to a quasi-planar B10 unit. A similar triplet C2v boat-like isomer is found to be almost degenerate to the C2 structure, whereas the beautiful molecular wheel structure, D10h-V©B10−, is significantly higher in energy on the potential energy surface. Therefore, even though the VB10− system fulfills the electronic requirement to form a D10h-M©B10− aromatic molecular wheel, the V atom is too small to stabilize the ten-membered boron ring.
Co-reporter:Chuan-Gang Ning, Xiao-Gen Xiong, Yi-Lei Wang, Jun Li and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2012 vol. 14(Issue 26) pp:9323-9329
Publication Date(Web):12 Dec 2011
DOI:10.1039/C2CP23490D
Thiolate-protected gold nanoparticles have been found recently to be coordinated by the so-called “staple” bonding motifs, consisting of quasi-linear [RS–Au–SR] and V-shaped [RS–Au–(SR)–Au–SR] units, which carry a negative charge formally. Using photoelectron spectroscopy (PES) in conjunction with ab initio calculations, we have investigated the electronic structure and chemical bonding of the simplest staples with R = CH3: Au(SCH3)2− and Au2(SCH3)3−, which were produced by electrospray ionization. PES data of the two Au–thiolate complexes are obtained both at room temperature (RT) and 20 K. The temperature-dependent study reveals significant spectral broadening at RT, in agreement with theoretical predictions of multiple conformations due to the different orientations of the –SCH3 groups. The Au–S bonds in Aun(SCH3)n+1− (n = 1, 2) are shown to be covalent via a variety of chemical bonding analyses. The strong Au–thiolate bonding and the stability of the Au–thiolate complexes are consistent with their ubiquity as staples for gold nanoparticles and on gold surfaces.
Co-reporter:Hua-Jin Zhai, Wen-Jie Chen, Xin Huang and Lai-Sheng Wang
RSC Advances 2012 vol. 2(Issue 7) pp:2707-2712
Publication Date(Web):22 Feb 2012
DOI:10.1039/C2RA00753C
The structure and chemical bonding in the Re3O3− cluster are investigated using photoelectron spectroscopy and density-functional theory calculations. Vibrationally-resolved photoelectron spectra were obtained, yielding an accurate electron affinity (2.54 ± 0.02 eV) and a ground-state ReO stretching frequency (960 ± 30 cm−1) for the Re3O3 neutral cluster. It is shown that the Re3O3− cluster possesses a C2v (1A1) ground-state structure consisting of a Re3 triangle with one bridging and two terminal oxygens. Molecular orbital analysis reveals that the Re3 core in Re3O3− possesses conflicting d-orbital aromaticity (π-antiaromatic and σ-aromatic), consistent with its C2v symmetry. Well-resolved photodetachment transitions from the Re 5dz2 δ orbitals allow the bond strength and resonance energy of a delocalized δ-bond to be estimated.
Co-reporter:Shenggang Li, Hua-Jin Zhai, Lai-Sheng Wang, and David A. Dixon
The Journal of Physical Chemistry A 2012 Volume 116(Issue 21) pp:5256-5271
Publication Date(Web):May 2, 2012
DOI:10.1021/jp303604k
Anion photoelectron spectroscopy and quantum chemical calculations at the density functional theory (DFT), coupled cluster theory (CCSD(T)), and complete active space self-consistent field (CASSCF) theory levels are employed to study the reduced transition metal oxide clusters M4O10– (M = Cr, W) and their neutrals. Photoelectron spectra are obtained at 193 and 157 nm photon energies, revealing very different electronic structures for the Cr versus W oxide clusters. The electron affinity and HOMO–LUMO gap are measured to be 3.68 ± 0.05 and 0.7 eV, respectively, for the Cr4O10 neutral cluster, as compared to 4.41 ± 0.04 and 1.3 eV for W4O10. A comprehensive search is performed to determine the ground-state structures for M4O10 and M4O10–, in terms of geometry and electronic states by carefully examining the calculated relative energies at the DFT, CCSD(T), and CASSCF levels. The ground states of Cr4O10 and Cr4O10– have tetrahedral structures similar to that of P4O10 with the anion having a lower symmetry due to a Jahn–Teller distortion. The ground states of W4O10 and W4O10– have butterfly shape structures, featuring two fused five-member rings with a metal–metal multiple bond between the central metal atoms. The much stronger WW bonding than the CrCr bonding is found to be the primary cause for the different ground state structures of the reduced Cr4O100/– versus W4O100/– oxide clusters. The photoelectron spectra are assigned by comparing the experimental and theoretical adiabatic and vertical electron detachment energies, further confirming the determination of the ground electronic states of M4O10 and M4O10–. The time-dependent DFT method is used to calculate the excitation energies of M4O10. The TD-DFT results in combination with the self-consistently calculated vertical detachment energies for some of the excited states at the DFT and CCSD(T) levels are used to assign the higher energy bands. Accurate clustering energies and heats of formation of M4O10 are calculated and used to calculate accurate reaction energies for the reduction of M4O12 to M4O10 by CH3OH, as well as for the oxidation of M4O10 to M4O12 by O2. The performance of the DFT method with the B3LYP and BP86 functionals in the calculations of the relative energies, electron detachment energies, and excitation energies are evaluated, and the BP86 functional is found to give superior results for most of these energetic properties.
Co-reporter:Constantin Romanescu, Timur R. Galeev, Alina P. Sergeeva, Wei-Li Li, Lai-Sheng Wang, Alexander I. Boldyrev
Journal of Organometallic Chemistry 2012 s 721–722() pp: 148-154
Publication Date(Web):
DOI:10.1016/j.jorganchem.2012.07.050
Co-reporter:Timur R. Galeev;Dr. Constantin Romanescu;Wei-Li Li;Dr. Lai-Sheng Wang;Dr. Alexer I. Boldyrev
Angewandte Chemie International Edition 2012 Volume 51( Issue 9) pp:2101-2105
Publication Date(Web):
DOI:10.1002/anie.201107880
Co-reporter:Timur R. Galeev;Dr. Constantin Romanescu;Wei-Li Li;Dr. Lai-Sheng Wang;Dr. Alexer I. Boldyrev
Angewandte Chemie 2012 Volume 124( Issue 9) pp:2143-2147
Publication Date(Web):
DOI:10.1002/ange.201107880
Co-reporter:Phuong Diem Dau, Damian P. Hruszkewycz, Dao-Ling Huang, Matthew J. Chalkley, Hong-Tao Liu, Jennifer C. Green, Nilay Hazari, and Lai-Sheng Wang
Organometallics 2012 Volume 31(Issue 24) pp:8571-8576
Publication Date(Web):December 12, 2012
DOI:10.1021/om300956g
The dianionic PdI dimers [TBA]2[(TPPMS)2Pd2(μ-C3H5)2] (1) [TBA = tetrabutylammonium, TPPMS = PPh2(3-C6H4SO3)−] and [TBA]2[(TPPMS)2Pd2(μ-C3H5)(μ-Cl)] (2), containing two bridging allyl ligands and one bridging allyl ligand and one bridging chloride ligand, respectively, were synthesized. The electronic structures of these complexes were investigated by combining electrospray mass spectrometry with gas phase photodetachment photoelectron spectroscopy. The major difference between the photoelectron spectra of the anions of 1 and 2 is the presence of a low-energy detachment band with an adiabatic electron detachment energy of 2.44(6) eV in 1, which is not present in 2. The latter has a much higher adiabatic electron detachment energy of 3.24(6) eV. Density functional theory calculations suggest that this band is present in 1 due to electron detachment from the out-of-phase combination of the π2 orbitals, which are localized on the terminal carbon atoms of the bridging allyl ligands. In 2, the Pd centers stabilize the single π2 orbital of the bridging allyl ligand, and it is lowered in energy. The presence of the high-energy out-of-phase combination of the π2 allyl orbitals makes 1 a better nucleophile, which explains why species with two bridging allyl ligands react with CO2 in an analogous fashion to momoneric Pd η1-allyls, whereas species with one bridging allyl and one bridging chloride ligand are unreactive.
Co-reporter:Hua-Jin Zhai ; Xian-Hui Zhang ; Wen-Jie Chen ; Xin Huang
Journal of the American Chemical Society 2011 Volume 133(Issue 9) pp:3085-3094
Publication Date(Web):February 9, 2011
DOI:10.1021/ja110061v
We investigated the structures and bonding of two series of early transition-metal oxide clusters, M2On− and M2On (M = Nb, Ta; n = 5−7) using photoelectron spectroscopy (PES) and density-functional theory (DFT). The stoichiometric M2O5 clusters are found to be closed shell with large HOMO−LUMO gaps, and their electron affinities (EAs) are measured to be 3.33 and 3.71 eV for M = Nb and Ta, respectively; whereas EAs for the oxygen-rich clusters are found to be much higher: 5.35, 5.25, 5.28, and 5.15 eV for Nb2O6, Nb2O7, Ta2O6, and Ta2O7, respectively. Structural searches at the B3LYP level yield triplet and doublet ground states for the oxygen-rich neutral and anionic clusters, respectively. Spin density analyses reveal oxygen radical, diradical, and superoxide characters in the oxygen-rich clusters. The M2O7− and M2O7 clusters, which can be viewed to be formed by M2O5−/0 + O2, are utilized as molecular models to understand dioxygen activation on M2O5− and M2O5 clusters. The O2 adsorption energies on the stoichiometric M2O5 neutrals are shown to be surprisingly high (1.3−1.9 eV), suggesting strong capabilities to activate O2 by structural defects in Nb and Ta oxides. The PES data also provides valuable benchmarks for various density functionals (B3LYP, BP86, and PW91) for the Nb and Ta oxides.
Co-reporter:Wei-Li Li ; Constantin Romanescu ; Timur R. Galeev ; Zachary A. Piazza ; Alexander I. Boldyrev
Journal of the American Chemical Society 2011 Volume 134(Issue 1) pp:165-168
Publication Date(Web):December 13, 2011
DOI:10.1021/ja209808k
We report the observation of two transition-metal-centered nine-atom boron rings, RhⓒB9– and IrⓒB9–. These two doped-boron clusters are produced in a laser-vaporization supersonic molecular beam and characterized by photoelectron spectroscopy and ab initio calculations. Large HOMO–LUMO gaps are observed in the anion photoelectron spectra, suggesting that neutral RhⓒB9 and IrⓒB9 are highly stable, closed shell species. Theoretical calculations show that RhⓒB9 and IrⓒB9 are of D9h symmetry. Chemical bonding analyses reveal that these complexes are doubly aromatic, each with six completely delocalized π and σ electrons, which describe the bonding between the central metal atom and the boron ring. This work establishes firmly the metal-doped B rings as a new class of novel aromatic molecular wheels.
Co-reporter:Hong-Tao Liu, Xiao-Gen Xiong, Phuong Diem Dau, Yi-Lei Wang, Jun Li and Lai-Sheng Wang
Chemical Science 2011 vol. 2(Issue 11) pp:2101-2108
Publication Date(Web):06 Sep 2011
DOI:10.1039/C1SC00487E
We report a combined experimental and theoretical investigation of [XAuCN]− (X = F, Cl, Br, I) to examine the chemical bonding in the mixed cyanide halide Au(I) complexes. Photoelectron spectra are obtained for [XAuCN]−, yielding electron affinities of 5.38 ± 0.05, 5.14 ± 0.05, and 4.75 ± 0.05 eV for XAuCN (X = Cl, Br, I), respectively. Relativistic quantum chemical calculations based on wavefunction theory and density functional theory are carried out to help interpret the photoelectron spectra and elucidate the electronic structures and chemical bonding in the [XAuCN]− complexes. Spin–orbit coupling is found to be important in all the complexes, quenching the Renner–Teller distortion in the neutral molecules. Ab initio calculations including spin–orbit effects allow quantitative assignments of the observed photoelectron spectra. A variety of chemical bonding analyses based on the charge population, bond orders, and electron localization functions have been carried out, revealing a gradual transition from ionic behavior between F–Au in [FAuCN]− to relatively strong covalent bonding between I–Au in [IAuCN]−. Both relativistic effects and electron correlations are shown to enhance the covalency in the gold iodide complex.
Co-reporter:Timur R. Galeev, Alexander S. Ivanov, Constantin Romanescu, Wei-Li Li, Konstantin V. Bozhenko, Lai-Sheng Wang and Alexander I. Boldyrev
Physical Chemistry Chemical Physics 2011 vol. 13(Issue 19) pp:8805-8810
Publication Date(Web):12 Apr 2011
DOI:10.1039/C1CP20359B
In this joint experimental and theoretical work we present a novel type of structural transition occurring in the series of CxB8−x− (x = 1–8) mixed clusters upon increase of the carbon content from x = 2 to x = 3. The wheel to ring transition is surprising because it is rather planar-to-linear type of transition to be expected in the series since B8, B8−, B82− and CB7− are known to possess wheel-type global minimum structures while C8 is linear.
Co-reporter:Wen-Jie Chen, Hua-Jin Zhai, Xin Huang, Lai-Sheng Wang
Chemical Physics Letters 2011 Volume 512(1–3) pp:49-53
Publication Date(Web):16 August 2011
DOI:10.1016/j.cplett.2011.07.018
Co-reporter:Wei-Li Li, Constantin Romanescu, Timur R. Galeev, Lai-Sheng Wang, and Alexander I. Boldyrev
The Journal of Physical Chemistry A 2011 Volume 115(Issue 38) pp:10391-10397
Publication Date(Web):August 1, 2011
DOI:10.1021/jp205873g
The structures and the electronic properties of two Al-doped boron clusters, AlB9– and AlB10–, were investigated via joint photoelectron spectroscopy and high-level ab initio study. The photoelectron spectra of both anions are relatively broad and have no vibrational structure. The geometrical structures were established by unbiased global minimum searches using the Coalescence Kick method and comparison between the experimental and calculated vertical electron detachment energies. The results show that both clusters have quasi-planar structures and that the Al atom is located at the periphery. Chemical bonding analysis revealed that the global minimum structures of both anions can be described as doubly (σ- and π-) aromatic systems. The nona-coordinated wheel-type structure of AlB9– was found to be a relatively high-lying isomer, while a similar structure for the neutral AlB9 cluster was previously shown to be either a global minimum or a low-lying isomer.
Co-reporter:Dr. Constantin Romanescu;Timur R. Galeev;Wei-Li Li;Dr. Alexer I. Boldyrev;Dr. Lai-Sheng Wang
Angewandte Chemie International Edition 2011 Volume 50( Issue 40) pp:9334-9337
Publication Date(Web):
DOI:10.1002/anie.201104166
Co-reporter:Dr. Hua-Jin Zhai;Dr. Jin-Chang Guo; Dr. Si-Dian Li; Dr. Lai-Sheng Wang
ChemPhysChem 2011 Volume 12( Issue 14) pp:2549-2553
Publication Date(Web):
DOI:10.1002/cphc.201100553
Abstract
Anion photoelectron spectroscopy and theoretical calculations are combined to probe the structures and chemical bonding of two boron-rich oxide clusters, B5O3− and B6O3−, which are shown to be appropriately formulated as B2(BO)3− and B3(BO)3−, respectively. The anion clusters are found to each possess a bridging η2-BO group, as well as two terminal BO groups and are analogs of B2H3− and B3H3−. This finding advances the boronyl chemistry and helps establish the isolobal analogy between boron-rich oxide clusters and boranes.
Co-reporter:Rhitankar Pal, Wei Huang, Yi-Lei Wang, Han-Shi Hu, Satya Bulusu, Xiao-Gen Xiong, Jun Li, Lai-Sheng Wang, and Xiao Cheng Zeng
The Journal of Physical Chemistry Letters 2011 Volume 2(Issue 18) pp:2288-2293
Publication Date(Web):August 22, 2011
DOI:10.1021/jz201023q
CO chemisorption onto the Au7– cluster is investigated using photoelectron spectroscopy (PES) and ab initio calculations. It is found that CO binding can induce previously unreported 2D–3D–2D structural changes. The gold motif in the most stable structure of COAu7– is an intermediate between the two known stable 2D isomers of Au7–. Two minor isomers are observed in the PES of (CO)2Au7–; one is due to an unprecedented 3D Au7– species with Cs symmetry. This 3D Cs Au7 motif becomes a major isomer in (CO)3Au7–. The most stable isomers of COAu7– and (CO)2Au7– are planar with identical Au7 motifs; the stable planar isomers of (CO)3Au7– include not only the global-minimum structure of Au7– but also a planar hexagonal Au7 motif. The PES spectrum of (CO)4Au7– is markedly different, and its most stable structure consists of the global-minimum structure of Au7–, three terminal CO, and one bridging CO.Keywords: PES (photoelectron spectroscopy); SO (spin−orbit); VDE (vertical detachment energy);
Co-reporter:Nan Shao ; Wei Huang ; Yi Gao ; Lei-Ming Wang ; Xi Li ; Lai-Sheng Wang ;Xiao Cheng Zeng
Journal of the American Chemical Society 2010 Volume 132(Issue 18) pp:6596-6605
Publication Date(Web):April 20, 2010
DOI:10.1021/ja102145g
The structural evolution of negatively charged gold clusters (Aun−) in the medium size range for n = 27−35 has been investigated using photoelectron spectroscopy (PES) and theoretical calculations. New PES data are obtained using Ar-seeded He supersonic beams to achieve better cluster cooling, resulting in well-resolved spectra and revealing the presence of low-lying isomers in a number of systems. Density-functional theory calculations are used for global minimum searches. For each cluster anion, more than 200 low-lying isomers are generated using the basin-hopping global minimum search algorithm. The most viable structures and low-lying isomers are obtained using both the relative energies and comparisons between the simulated spectra and experimental PES data. The global minimum structures of Aun− (n = 27, 28, 30, and 32−35) are found to exhibit low-symmetry core−shell structures with the number of core atoms increasing with cluster size: Au27−, Au28−, and Au30− possess a one-atom core; Au32− features a three-atom triangular core; and Au33− to Au35− all contain a four-atom tetrahedral core. The global searches reveal that the tetrahedral core is a popular motif for low-lying structures of Au33− to Au35−. The structural information forms the basis for future chemisorption studies to unravel the catalytic effects of gold nanoparticles.
Co-reporter:Wei Huang ; Hua-Jin Zhai
Journal of the American Chemical Society 2010 Volume 132(Issue 12) pp:4344-4351
Publication Date(Web):March 10, 2010
DOI:10.1021/ja910401x
Activation of O2 is the most critical step in catalytic oxidation reactions involving gold and remains poorly understood. Here we report a systematic investigation of the interactions between O2 and small gold cluster anions Aun− (n = 1−7) using photoelectron spectroscopy. Higher resolution photoelectron spectra are obtained for the molecularly chemisorbed even-sized AunO2− (n = 2, 4, 6) complexes. Well-resolved vibrational structures due to O−O stretching are observed and can be readily distinguished from the Au-derived PES bands. The adiabatic detachment energies and O−O vibrational frequencies are measured to be 3.03 ± 0.04, 3.53 ± 0.05, and 3.17 ± 0.05 eV, and 1360 ± 80, 1360 ± 80, and 1330 ± 80 cm−1 for n = 2, 4, 6, respectively. Physisorbed Aun−(O2) complexes for n = 1, 3, 5, 7 are observed for the first time, providing direct evidence for the inertness of the closed-shell odd-sized Aun− clusters toward O2. Neutral even-sized Aun clusters are closed-shell and are expected to be inert toward O2, which is not consistent with the reduced O−O vibrational frequencies observed in the photoelectron spectra relative to free O2. It is suggested that the photodetachment transitions can only access excited states of the neutral even-sized AunO2 complexes; a double-well potential is proposed consisting of the ground-state van der Walls well at long Aun−O2 distances and a higher energy deeper well at short Aun−O2 distances derived from singlet O2 (1Δg). The current study provides further insight into O2 interactions with small gold clusters, as well as accurate experimental data to benchmark theoretical investigations.
Co-reporter:Lei-Ming Wang ; Boris B. Averkiev ; Jordan A. Ramilowski ; Wei Huang ; Lai-Sheng Wang ;Alexander I. Boldyrev
Journal of the American Chemical Society 2010 Volume 132(Issue 40) pp:14104-14112
Publication Date(Web):September 21, 2010
DOI:10.1021/ja103846q
Bulk carbon and boron form very different materials, which are also reflected in their clusters. Small carbon clusters form linear structures, whereas boron clusters are planar. For example, it is known that the B5− cluster possesses a C2v planar structure and C5− is a linear chain. Here we study B/C mixed clusters containing five atoms, CxB5−x− (x = 1−5), which are expected to exhibit a planar to linear structural transition as a function of the C content. The CxB5−x− (x = 1−5) clusters were produced and studied by photoelectron spectroscopy; their geometric and electronic structures were investigated using a variety of theoretical methods. We found that the planar-to-linear transition occurs between x = 2 and 3: the global minimum structures of the B-rich clusters, CB4− and C2B3−, are planar, similar to B5−, and those of the C-rich clusters, C3B2− and C4B−, are linear, similar to C5−.
Co-reporter:Xiao-Peng Xing, Xue-Bin Wang and Lai-Sheng Wang
The Journal of Physical Chemistry A 2010 Volume 114(Issue 13) pp:4524-4530
Publication Date(Web):March 17, 2010
DOI:10.1021/jp1011523
The hallmark of multiply charged anions is the repulsive Coulomb barrier (RCB), which prevents low-energy electrons from being emitted in photodetachment experiments. However, using photoelectron imaging, we have observed persistent near 0 eV electrons during photodetachment of doubly charged dicarboxylate anions, −O2C(CH2)nCO2− (Dn2−, n = 2−8). Here we show that these low-energy electron signals are well structured and are independent of the detachment photon fluxes or energies. The relative intensities of these signals are dependent on n, with maxima at n = 2, 4, and 6. These near 0 eV electrons cannot come from direct photodetachment of the dianions and are proposed to come from decarboxylation of the product radical anions upon photodetachment of the parent dianions [•O2C(CH2)nCO2− → CO2 + •(CH2)nCO2−], followed by dissociative autodetachment [•(CH2)nCO2− → (CH2)n + CO2 + e] or hydrogen-transfer-induced electron detachment [•(CH2)nCO2− → CH2═CH(CH2)n−2CO2H + e]. Energetic considerations suggest that these processes are exothermic. It is further observed that solvation by one water molecule quenches the low-energy electron signals in the spectra of Dn2−(H2O), consistent with the proposed mechanisms. These indirect dissociative autodetachment processes are expected to involve cyclic transition states for n > 2, which is in agreement with the dependence on the chain length due to the anticipated strains in the intermediate steps. The quenching of the low-energy electron signals by one water molecule demonstrates the importance of solvation on chemical reactions.
Co-reporter:Hua-Jin Zhai, Chang-Qing Miao, Si-Dian Li, and Lai-Sheng Wang
The Journal of Physical Chemistry A 2010 Volume 114(Issue 46) pp:12155-12161
Publication Date(Web):October 29, 2010
DOI:10.1021/jp108668t
During photoelectron spectroscopy experiments, the spectra of B11O− and B10Au− clusters are found to exhibit similar patterns except for a systematic spectral shift of ∼0.5 eV, hinting that they possess similar geometric structures. The electron affinities are measured to be 4.02 ± 0.04 eV for B11O and 3.55 ± 0.02 eV for B10Au. DFT calculations at the B3LYP level show that B11O− and B10Au− adopt similar C1 (1A) ground states, which are based on the quasiplanar B10 cluster interacting with a BO unit and Au, respectively. The B11O− and B10Au− clusters are thus valent isoelectronic because both BO and Au can be viewed as monovalent units, forming highly covalent B−BO and B−Au bonds analogous to the B−H bond in B10H−. For B10Au−, we also find a highly symmetric D10h (1A1g) planar molecular wheel as a minimum on the potential energy surface. However, it is 45 kcal/mol above the ground state at the B3LYP level and not viable for experimental observation. Natural bond orbital analyses reveal interesting covalent versus ionic B−Au bonding in the C1 B10Au− and D10h B10Au− structures, respectively, providing insight for the design of Dnh MBn molecular wheels.
Co-reporter:Hua-Jin Zhai, Lai-Sheng Wang
Chemical Physics Letters 2010 500(4–6) pp: 185-195
Publication Date(Web):
DOI:10.1016/j.cplett.2010.10.001
Co-reporter:Wen-Jie Chen, Hua-Jin Zhai, Yong-Fan Zhang, Xin Huang and Lai-Sheng Wang
The Journal of Physical Chemistry A 2010 Volume 114(Issue 19) pp:5958-5966
Publication Date(Web):April 29, 2010
DOI:10.1021/jp102439v
The electronic and structural properties of a series of triniobium oxide clusters, Nb3On− and Nb3On (n = 3−8), are investigated using photoelectron spectroscopy (PES) and density functional theory (DFT) calculations. PES spectra are obtained for Nb3On− (n = 3−8) at various photon energies and are used to compare with the DFT calculations. A trend of sequential oxidation is observed as a function of O content until Nb3O8−, reaching the highest oxidation state of Nb. DFT calculations are performed to search for the lowest energy structures for both the anionic and neutral clusters. For Nb3O3−, the three O atoms are shown to prefer the bridging sites of a triangular Nb3, leading to two nearly degenerate cyclic structures of Cs symmetry. The next three O atoms from n = 4−6 each occupy a terminal site directly bonded to Nb, resulting in a symmetric Nb3O6− with C3v symmetry and a low-lying isomer of Cs symmetry. The seventh O atom is bonded to two Nb atoms forming a double bridge, whereas the eighth O atom is bonded to a terminal site so that in Nb3O8− each Nb atom reaches its maximum oxidation state of +5. The structures and electronic states for the triniobium oxide clusters are significantly different from the corresponding tritantalum oxide clusters, in particular, for Nb3O3−, Nb3O5−, and Nb3O7−. Molecular orbital analyses are performed to elucidate the chemical bonding and the electronic and structural evolution in these triniobium oxide clusters.
Co-reporter:Xue-Bin Wang, Chaoxian Chi, Mingfei Zhou, Igor V. Kuvychko, Konrad Seppelt, Alexey A. Popov, Steven H. Strauss, Olga V. Boltalina and Lai-Sheng Wang
The Journal of Physical Chemistry A 2010 Volume 114(Issue 4) pp:1756-1765
Publication Date(Web):January 8, 2010
DOI:10.1021/jp9097364
A photoelectron spectroscopy investigation of the fluorofullerene anions C60Fn− (n = 17, 33, 35, 43, 45, 47) and the doubly charged anions C60F342− and C60F462− is reported. The first electron affinities for the corresponding neutral molecules, C60Fn, were directly measured and were found to increase as n increased, reaching the extremely high value of 5.66 ± 0.10 eV for C60F47. Density functional calculations suggest that the experimentally observed species C60F17−, C60F35−, and C60F47− were each formed by reductive defluorination of the parent fluorofullerene, C3v-C60F18, C60F36 (a mixture of isomers), and D3-C60F48, respectively, without rearrangement of the remaining fluorine atoms. The DFT-predicted stability of C60F47− was verified by its generation by chemical reduction from D3-C60F48 in chloroform solution at 25 °C and its characterization by mass spectrometry and 19F NMR spectroscopy. Further reductive defluorination of C60F47− in solution resulted in the selective generation of a new fluorofullerene, D2-C60F44, which was also characterized by mass spectrometry and 19F NMR spectroscopy.
Co-reporter:Yi-Lei Wang, Xue-Bin Wang, Xiao-Peng Xing, Fan Wei, Jun Li, and Lai-Sheng Wang
The Journal of Physical Chemistry A 2010 Volume 114(Issue 42) pp:11244-11251
Publication Date(Web):May 12, 2010
DOI:10.1021/jp103173d
We report a combined experimental and theoretical investigation of MI2− (M = Cs, Cu, Ag, Au) to explore the chemical bonding in the group IA and IB diiodide complexes. Both photoelectron imaging and low-temperature photoelectron spectroscopy are applied to MI2− (M = Cs, Cu, Au), yielding vibrationally resolved spectra for CuI2− and AuI2− and accurate electron affinities, 4.52 ± 0.02, 4.256 ± 0.010, and 4.226 ± 0.010 eV for CsI2, CuI2, and AuI2, respectively. Spin−orbit coupling is found to be important in all the diiodide complexes and ab initio calculations including spin−orbit effects allow quantitative assignments of the observed photoelectron spectra. A variety of chemical bonding analyses (charge population, bond order, and electron localization functions) have been carried out, revealing a gradual transition from the expected ionic behavior in CsI2− to relatively strong covalent bonding in AuI2−. Both relativistic effects and electron correlation are shown to enhance the covalency in the gold diiodide complex.
Co-reporter:Matthew M. Meyer ; Xue-Bin Wang ; Christopher A. Reed ; Lai-Sheng Wang ;Steven R. Kass
Journal of the American Chemical Society 2009 Volume 131(Issue 50) pp:18050-18051
Publication Date(Web):December 1, 2009
DOI:10.1021/ja908964h
Five CHB11X6Y5− carborane anions from the series X = Br, Cl, I and Y = H, Cl, CH3 were generated by electrospray ionization, and their reactivity with a series of Brønsted acids and electron transfer reagents were examined in the gas phase. The undecachlorocarborane acid, H(CHB11Cl11), was found to be far more acidic than the former record holder, (1-C4F9SO2)2NH (i.e., ΔH°acid = 241 ± 29 vs 291.1 ± 2.2 kcal mol−1) and bridges the gas-phase acidity and basicity scales for the first time. Its conjugate base, CHB11Cl11−, was found by photoelectron spectroscopy to have a remarkably large electron binding energy (6.35 ± 0.02 eV) but the value for the (1-C4F9SO2)2N− anion is even larger (6.5 ± 0.1 eV). Consequently, it is the weak H-(CHB11Cl11) BDE (70.0 kcal mol−1, G3(MP2)) compared to the strong BDE of (1-C4F9SO2)2N−H (127.4 ± 3.2 kcal mol−1) that accounts for the greater acidity of carborane acids.
Co-reporter:Xue-Bin Wang ; Yi-Lei Wang ; Jie Yang ; Xiao-Peng Xing ; Jun Li
Journal of the American Chemical Society 2009 Volume 131(Issue 45) pp:16368-16370
Publication Date(Web):October 27, 2009
DOI:10.1021/ja908106e
The Au(CN)2− ion is the most stable Au compound known for centuries, yet a detailed understanding of its chemical bonding is still lacking. Here we report direct experimental evidence of significant covalent bonding character in the Au−C bonds in Au(CN)2− using photoelectron spectroscopy and comparisons with its lighter congeners, Ag(CN)2− and Cu(CN)2−. Vibrational progressions in the Au−C stretching mode were observed for all detachment transitions for Au(CN)2−, in contrast to the atomic-like transitions for Cu(CN)2−, revealing the Au−C covalent bonding character. In addition, rich electronic structural information was obtained for Au(CN)2− by employing 118 nm detachment photons. Density functional theory and high-level ab initio calculations were carried out to understand the photoelectron spectra and obtain insight into the nature of the chemical bonding in the M(CN)2− complexes. Significant covalent character in the Au−C bonding due to the strong relativistic effects was revealed in Au(CN)2−, consistent with its high stability.
Co-reporter:Dao-Ling Huang, Guo-Zhu Zhu, Yuan Liu, Lai-Sheng Wang
Journal of Molecular Spectroscopy (February 2017) Volume 332() pp:
Publication Date(Web):February 2017
DOI:10.1016/j.jms.2016.10.021
•Observation of dipole-bound excited state in deprotonated 2-hydroxypyrimidine.•A photodetachment spectroscopy of deprotonated 2-hydroxypyrimidine anion.•Resonant high-resolution photoelectron imaging.•Twenty vibrational levels of the dipole-bound state are observed.•Observation of nine fundamental vibrational frequencies.We report a photodetachment and high-resolution photoelectron imaging study of cold deprotonated 2-hydroxypyrimidine anions, C4H3N2O−. Photodetachment spectroscopy reveals an excited dipole-bound state (DBS) of C4H3N2O− with a binding energy of 598 ± 5 cm−1 below the detachment threshold of 26,010 ± 5 cm−1. Twenty vibrational levels of the DBS are observed as resonances in the photodetachment spectrum, with three below the detachment threshold and seventeen above the threshold. By tuning the detachment laser to the above-threshold vibrational resonances, highly non-Franck-Condon photoelectron spectra are obtained. Nine fundamental vibrational frequencies are resolved, including six symmetry-forbidden modes. The 598 cm−1 binding energy for the DBS is quite high due to the large dipole moment of the C4H3N2OC4H3N2O radical (>6 D). However, no evidence of a second DBS is observed below the detachment threshold.
Co-reporter:Dao-Ling Huang, Hong-Tao Liu, Chuan-Gang Ning, Phuong Diem Dau, Lai-Sheng Wang
Chemical Physics (12 January 2017) Volume 482() pp:
Publication Date(Web):12 January 2017
DOI:10.1016/j.chemphys.2016.06.003
•Forty-four resonant photoelectron imaging and spectra of N1[U-H]− are reported.•The autodetachment is largely governed by the Δv = −1 vibrational propensity rule.•The breakdown of the propensity rule is observed due to electron rescattering.•The breakdown of the propensity rule is observed due to the anharmonic effect.We report both non-resonant and resonant high-resolution photoelectron imaging of cryogenically-cooled deprotonated uracil anions, N1[U-H]−, via vibrational levels of a dipole-bound excited state. Photodetachment spectroscopy of N1[U-H]− was reported previously (Liu et al., 2014), in which forty-six vibrational autodetachment resonances due to the excited dipole-bound state were observed. By tuning the detachment laser to the vibrational levels of the dipole-bound state, we obtained high-resolution resonant photoelectron spectra, which are highly non-Franck–Condon. The resonant photoelectron spectra reveal many Franck–Condon inactive vibrational modes, significantly expanding the capability of photoelectron spectroscopy. A total of twenty one fundamental vibrational frequencies for the N1[U-H] radical are obtained, including all eight low-frequency out-of-plane modes, which are forbidden in non-resonant photoelectron spectroscopy. Furthermore, the breakdown of the Δv = −1 propensity rule is observed for autodetachment from many vibrational levels of the dipole-bound state, due to anharmonic effects. In particular, we have observed intramolecular electron rescattering in a number of resonant photoelectron spectra, leading to excitations of low-frequency vibrational modes. Further theoretical study may be warranted, in light of the extensive experimental data and new observations, to provide further insight into the autodetachment dynamics and vibronic coupling in dipole-bound states, as well as electron molecule interactions.
Co-reporter:Hua-Jin Zhai ; Qiang Chen ; Hui Bai ; Si-Dian Li
Accounts of Chemical Research () pp:
Publication Date(Web):June 10, 2014
DOI:10.1021/ar500136j
The BO groups also dominate the structures and bonding of boron oxide clusters and boron boronyl complexes, in which BO groups occupy terminal, bridging, or face-capping positions. The bridging η2-BO groups feature three-center two-electron bonds, akin to the BHB τ bonds in boranes. A close isolobal analogy is thus established between boron oxide clusters and boranes, offering vast opportunities for the rational design of novel boron oxide clusters and compounds. Boron boronyl clusters may also serve as molecular models for mechanistic understanding of the combustion of boron and boranes. An effort to tune the B versus O composition in boron oxide clusters leads to the discovery of boronyl boroxine, D3h B3O3(BO)3, an analogue of boroxine and borazine and a new member of the “inorganic benzene” family. Furthermore, a unique concept of π and σ double conjugation is proposed for the first time to elucidate the structures and bonding in the double-chain nanoribbon boron diboronyl clusters, which appear to be inorganic analogues of polyenes, cumulenes, and polyynes. This Account concludes with a brief outlook for the future directions in this emerging and expanding research field.
Co-reporter:Wan-Lu Li, Tian Jian, Xin Chen, Hai-Ru Li, Teng-Teng Chen, Xue-Mei Luo, Si-Dian Li, Jun Li and Lai-Sheng Wang
Chemical Communications 2017 - vol. 53(Issue 10) pp:NaN1590-1590
Publication Date(Web):2016/12/20
DOI:10.1039/C6CC09570D
A tubular molecular rotor B2-Ta@B18− (1) and boron drum Ta@B20− (2) with the highest coordination number of twenty in chemistry are observed via a joint photoelectron spectroscopy and first-principles theory investigation.
Co-reporter:Wan-Lu Li, Hong-Tao Liu, Tian Jian, Gary V. Lopez, Zachary A. Piazza, Dao-Ling Huang, Teng-Teng Chen, Jing Su, Ping Yang, Xin Chen, Lai-Sheng Wang and Jun Li
Chemical Science (2010-Present) 2016 - vol. 7(Issue 1) pp:NaN481-481
Publication Date(Web):2015/10/13
DOI:10.1039/C5SC03568F
We report a joint photoelectron spectroscopy and theoretical investigation of the gaseous Au2I3− cluster, which is found to exhibit two types of isomers due to competition between Au–I covalent bonding and Au–Au aurophilic interactions. The covalent bonding favors a bent IAuIAuI− structure with an obtuse Au–I–Au angle (100.7°), while aurophilic interactions pull the two Au atoms much closer, leading to an acutely bent structure (72.0°) with an Au–Au distance of 3.08 Å. The two isomers are separated by a small barrier and are nearly degenerate with the obtuse isomer being slightly more stable. At low temperature, only the obtuse isomer is observed; distinct experimental evidence is observed for the co-existence of a combination of isomers with both acute and obtuse bending angles at room temperature. The two bond-bending isomers of Au2I3− reveal a unique example of one molecule being able to oscillate between different structures as a result of two competing chemical forces.
Co-reporter:Phuong Diem Dau, Jing Su, Hong-Tao Liu, Jian-Biao Liu, Dao-Ling Huang, Jun Li and Lai-Sheng Wang
Chemical Science (2010-Present) 2012 - vol. 3(Issue 4) pp:NaN1146-1146
Publication Date(Web):2012/01/04
DOI:10.1039/C2SC01052F
Bare uranyl tetrafluoride (UO2F42−) and its solvation complexes by one and two water or acetonitrile molecules have been observed in the gas phase using electrospray ionization and investigated by photoelectron spectroscopy and ab initio calculations. The isolated UO2F42− dianion is found to be electronically stable with an adiabatic electron binding energy of 1.10 ± 0.05 eV and a repulsive Coulomb barrier of ∼2 eV. Photoelectron spectra of UO2F42− display congested features due to detachment from U–O bonding orbitals and F 2p lone pairs. Solvated complexes by H2O and CH3CN, UO2F4(H2O)n2− and UO2F4(CH3CN)n2− (n = 1, 2), are also observed and their photoelectron spectra are similar to those of the bare UO2F42− dianion, suggesting that the solvent molecules are coordinated to the outer sphere of UO2F42− with relatively weak interactions between the solvent molecules and the dianion core. Both DFT and CCSD(T) calculations are performed on UO2F42− and its solvated species to understand the electronic structure of the dianion core and solute–solvent interactions. The strong U–F interactions with partial (d–p)π bonding are shown to weaken the UO bonds in the [OUO]2+ unit. Each H atom in the water molecules forms a H-bond to a F atom in the equatorial plane of UO2F42−, while each CH3CN molecule forms three H-bonds to two F ligands and one axial oxygen.
Co-reporter:Hong-Tao Liu, Yi-Lei Wang, Xiao-Gen Xiong, Phuong Diem Dau, Zachary A. Piazza, Dao-Ling Huang, Cong-Qiao Xu, Jun Li and Lai-Sheng Wang
Chemical Science (2010-Present) 2012 - vol. 3(Issue 11) pp:NaN3295-3295
Publication Date(Web):2012/08/15
DOI:10.1039/C2SC20984E
We report an investigation of the electronic structure and chemical bonding of AuH2− using photoelectron spectroscopy and ab initio calculations. We obtained vibrationally resolved photoelectron spectra of AuH2− at several photon energies. Six electronic states of AuH2 were observed and assigned according to the theoretical calculations. The ground state of AuH2− is known to be linear, while that of neutral AuH2 is bent with a ∠H–Au–H equilibrium bond angle of 129°. This large geometry change results in a very broad bending vibrational progression in the photoelectron spectra for the ground-state transition. The electron affinity of AuH2 is measured to be 3.030 ± 0.020 eV. A short bending vibrational progression is also observed in the second photodetachment band, suggesting a slightly bent structure for the first excited state of AuH2. The linear geometry is a saddle point for the ground and first excited states of AuH2, resulting in double-well potentials for these states along the bending coordinate. Spectroscopic evidence is observed for the detachment transitions to the double-well potentials of the ground and first excited states of AuH2. Higher excited states of AuH2 due to detachment from the nonbonding Au 5d electrons are all linear, similar to the anion ground state. Kohn–Sham molecular orbital analyses reveal surprising participation of H 2p orbitals in the Au–H chemical bonding and an unprecedented weak Au 5dπ to H 2pπ back donation. The simplicity of the linear AuH2− anion and its novel spectroscopic features make it a textbook example for understanding the covalent bonding properties and relativistic effects of Au.
Co-reporter:Hong-Tao Liu, Xiao-Gen Xiong, Phuong Diem Dau, Yi-Lei Wang, Jun Li and Lai-Sheng Wang
Chemical Science (2010-Present) 2011 - vol. 2(Issue 11) pp:NaN2108-2108
Publication Date(Web):2011/09/06
DOI:10.1039/C1SC00487E
We report a combined experimental and theoretical investigation of [XAuCN]− (X = F, Cl, Br, I) to examine the chemical bonding in the mixed cyanide halide Au(I) complexes. Photoelectron spectra are obtained for [XAuCN]−, yielding electron affinities of 5.38 ± 0.05, 5.14 ± 0.05, and 4.75 ± 0.05 eV for XAuCN (X = Cl, Br, I), respectively. Relativistic quantum chemical calculations based on wavefunction theory and density functional theory are carried out to help interpret the photoelectron spectra and elucidate the electronic structures and chemical bonding in the [XAuCN]− complexes. Spin–orbit coupling is found to be important in all the complexes, quenching the Renner–Teller distortion in the neutral molecules. Ab initio calculations including spin–orbit effects allow quantitative assignments of the observed photoelectron spectra. A variety of chemical bonding analyses based on the charge population, bond orders, and electron localization functions have been carried out, revealing a gradual transition from ionic behavior between F–Au in [FAuCN]− to relatively strong covalent bonding between I–Au in [IAuCN]−. Both relativistic effects and electron correlations are shown to enhance the covalency in the gold iodide complex.
Co-reporter:Xiao-Gen Xiong, Yi-Lei Wang, Cong-Qiao Xu, Yi-Heng Qiu, Lai-Sheng Wang and Jun Li
Dalton Transactions 2015 - vol. 44(Issue 12) pp:NaN5546-5546
Publication Date(Web):2015/02/03
DOI:10.1039/C4DT04031G
Gold compounds, clusters, and nanoparticles are widely used as catalysts and therapeutic medicines; the interactions between gold and its ligands in these systems play important roles in their chemical properties and functionalities. In order to elucidate the nature of the chemical interactions between Au(I) and its ligands, herein we use several theoretical methods to study the chemical bonding in a variety of linear [AuX2]− complexes, where X = halogen atoms (F, Cl, Br, I, At and Uus), H, OH, SH, OCH3, SCH3, CN and SCN. It is shown that the most important bonding orbitals in these systems have significant contributions from the Au sd hybridized atomic orbitals. The ubiquitous linear or quasi-linear structures of [AuX2]− are attributed to the well-balanced optimal overlap in both σ and π bonding orbitals and minimal repulsion between the two negatively charged ligands. The stability of these complexes is related to the covalency of the Au–X bond and a periodic trend is found in the evolution of covalency along the halogen group ligands. The special stability of [Au(CN)2]− is a result of strong covalent and ionic interactions. For the superheavy element Uus, the covalency of Au–Uus is enhanced through the spin–orbit interactions.
Co-reporter:Alexander I. Boldyrev and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2016 - vol. 18(Issue 17) pp:NaN11605-11605
Publication Date(Web):2016/01/28
DOI:10.1039/C5CP07465G
We describe joint experimental and theoretical studies carried out collaboratively in the authors' labs for understanding the structures and chemical bonding of novel atomic clusters, which exhibit aromaticity. The concept of aromaticity was first discovered to be useful in understanding the square-planar unit of Al4 in a series of MAl4− bimetallic clusters that led to discoveries of aromaticity in many metal cluster systems, including transition metals and similar cluster motifs in solid compounds. The concept of aromaticity has been found to be particularly powerful in understanding the stability and bonding in planar boron clusters, many of which have been shown to be analogous to polycyclic aromatic hydrocarbons in their π bonding. Stimulated by the multiple aromaticity in planar boron clusters, a design principle has been proposed for stable metal-cerntered aromatic molecular wheels of the general formula, M@Bnk−. A series of such borometallic aromatic wheel complexes have been produced in supersonic cluster beams and characterized experimentally and theoretically, including Ta@B10− and Nb@B10−, which exhibit the highest coordination number in two dimensions.
Co-reporter:Marc-Oliver Winghart, Ji-Ping Yang, Michael Kühn, Andreas-Neil Unterreiner, Thomas J. A. Wolf, Phuong D. Dau, Hong-Tao Liu, Dao-Ling Huang, Wim Klopper, Lai-Sheng Wang and Manfred M. Kappes
Physical Chemistry Chemical Physics 2013 - vol. 15(Issue 18) pp:NaN6736-6736
Publication Date(Web):2013/03/18
DOI:10.1039/C3CP50497B
Photoelectron spectra of isolated [M–BDSZ]3− (BDSZ = bisdisulizole, M = H, Li, Na, K, Cs) triply charged anions exhibit a dominant constant electron kinetic energy (KE) detachment feature, independent of detachment wavelengths over a wide UV range. Photoelectron imaging spectroscopy shows that this constant KE feature displays an angular distribution consistent with delayed rather than direct electron emission. Time-resolved pump–probe (388 nm/775 nm) two-colour photoelectron spectroscopy reveals that the constant KE feature results from two simultaneously populated excited states, which decay at different rates. The faster of the two rates is essentially the same for all the [M–BDSZ]3− species, regardless of M. The slower process is associated with lifetimes ranging from several picoseconds to tens of picoseconds. The lighter the alkali cation is, the longer the lifetime of this state. Quantum chemical calculations indicate that the two decaying states are in fact the two lowest singlet excited states of the trianions. Each of the two corresponding photoexcitations is associated with significant charge transfer. However, electron density is transferred from different ends of the roughly chain-like molecule to its aromatic center. The energy (and therefore the decay rate) of the longer-lived excited state is found to be influenced by polarization effects due to the proximal alkali cation complexed to that end of the molecule. Systematic M-dependent geometry changes, mainly due to the size of the alkali cation, lead to M-dependent shifts in transition energies. At the constant pump wavelength this leads to different amounts of vibrational energy in the respective excited state, contributing to the variations in decay rates. The current experiments and calculations confirm excited state electron tunneling detachment (ESETD) to be the mechanism responsible for the observed constant KE feature. The ESETD phenomenon may be quite common for isolated multiply charged anions, which are strong fluorophores in the condensed phase – making ESETD useful for studies of the transient response of such species after electronic excitation.
Co-reporter:Chuan-Gang Ning, Xiao-Gen Xiong, Yi-Lei Wang, Jun Li and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2012 - vol. 14(Issue 26) pp:NaN9329-9329
Publication Date(Web):2011/12/12
DOI:10.1039/C2CP23490D
Thiolate-protected gold nanoparticles have been found recently to be coordinated by the so-called “staple” bonding motifs, consisting of quasi-linear [RS–Au–SR] and V-shaped [RS–Au–(SR)–Au–SR] units, which carry a negative charge formally. Using photoelectron spectroscopy (PES) in conjunction with ab initio calculations, we have investigated the electronic structure and chemical bonding of the simplest staples with R = CH3: Au(SCH3)2− and Au2(SCH3)3−, which were produced by electrospray ionization. PES data of the two Au–thiolate complexes are obtained both at room temperature (RT) and 20 K. The temperature-dependent study reveals significant spectral broadening at RT, in agreement with theoretical predictions of multiple conformations due to the different orientations of the –SCH3 groups. The Au–S bonds in Aun(SCH3)n+1− (n = 1, 2) are shown to be covalent via a variety of chemical bonding analyses. The strong Au–thiolate bonding and the stability of the Au–thiolate complexes are consistent with their ubiquity as staples for gold nanoparticles and on gold surfaces.
Co-reporter:Wei-Li Li, Constantin Romanescu, Zachary A. Piazza and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2012 - vol. 14(Issue 39) pp:NaN13669-13669
Publication Date(Web):2012/08/20
DOI:10.1039/C2CP42218B
A class of transition-metal-centered aromatic boron wheels (Dnh-M©Bnq−) have been recently produced and characterized according to an electronic design principle. Here we investigate the interplay between electronic and geometric requirements for the molecular wheels using the case of VB10−, which is isoelectronic to the decacoordinated molecular wheels, Ta©B10− and Nb©B10−. Photoelectron spectra of VB10− are observed to be broad and complicated with relatively low electron binding energies, in contrast to the simple and high electron binding energies observed for the molecular wheels of its heavier congeners. An unbiased global minimum search found the most stable isomer of VB10− to be a singlet “boat”-like structure (C2), in which the V atom is coordinated to a quasi-planar B10 unit. A similar triplet C2v boat-like isomer is found to be almost degenerate to the C2 structure, whereas the beautiful molecular wheel structure, D10h-V©B10−, is significantly higher in energy on the potential energy surface. Therefore, even though the VB10− system fulfills the electronic requirement to form a D10h-M©B10− aromatic molecular wheel, the V atom is too small to stabilize the ten-membered boron ring.
Co-reporter:Tian Jian, Wan-Lu Li, Xin Chen, Teng-Teng Chen, Gary V. Lopez, Jun Li and Lai-Sheng Wang
Chemical Science (2010-Present) 2016 - vol. 7(Issue 12) pp:NaN7027-7027
Publication Date(Web):2016/07/25
DOI:10.1039/C6SC02623K
Metal-doped boron clusters provide new opportunities to design nanoclusters with interesting structures and bonding. A cobalt-doped boron cluster, CoB18−, has been observed recently to be planar and can be viewed as a motif for metallo-borophenes, whereas the D9d drum isomer as a motif for metallo-boronanotubes is found to be much higher in energy. Hence, whether larger doped boron drums are possible is still an open question. Here we report that for RhB18− the drum and quasi-planar structures become much closer in energy and co-exist experimentally, revealing a competition between the metallo-boronanotube and metallo-borophene structures. Photoelectron spectroscopy of RhB18− shows a complicated spectral pattern, suggesting the presence of two isomers. Quantum chemistry studies indicate that the D9d drum isomer and a quasi-planar isomer (Cs) compete for the global minimum. The enhanced stability of the drum isomer in RhB18− is due to the less contracted Rh4d orbitals, which can have favorable interactions with the B18 drum motif. Chemical bonding analyses show that the quasi-planar isomer of RhB18− is aromatic with 10 π electrons, whereas the observed RhB18− drum cluster sets a new record for coordination number of eighteen among metal complexes. The current finding shows that the size of the boron drum can be tuned by appropriate metal dopants, suggesting that even larger boron drums with 5d, 6d transition metal, lanthanide or actinide metal atoms are possible.
Co-reporter:Hai-Ru Li, Tian Jian, Wei-Li Li, Chang-Qing Miao, Ying-Jin Wang, Qiang Chen, Xue-Mei Luo, Kang Wang, Hua-Jin Zhai, Si-Dian Li and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2016 - vol. 18(Issue 42) pp:NaN29155-29155
Publication Date(Web):2016/09/23
DOI:10.1039/C6CP05420J
Size-selected boron clusters have been found to be predominantly planar or quasi-planar (2D) in the small size regime with the appearance of three-dimensional (3D) borospherene cages of larger sizes. A seashell-like B28− cluster was previously shown to be the smallest borospherene, which competes with a quasi-planar isomer for the global minimum. Here we report a study on the structures and bonding of the B29− and B29 clusters using photoelectron spectroscopy (PES) and first-principles calculations and demonstrate the continued competition between the 2D and borospherene structures. The PES spectrum of B29− displays a complex pattern with evidence of low-lying isomers. Global-minimum searches and extensive theoretical calculations revealed a complicated potential energy surface for B29− with five low-lying isomers, among which the lowest three were shown to contribute to the experimental spectrum. A 3D seashell-like Cs (2, 1A′) isomer, featuring two heptagons on the waist and one octagon at the bottom, is the global minimum for B29−, followed by a 2D C1 (3, 1A) isomer with a hexagonal hole and a stingray-shaped 2D Cs (1, 1A′) isomer with a pentagonal hole. However, by taking into account the entropic effects, the stingray-shaped isomer 1 was shown to be the lowest in energy at room temperature and was found to dominate the PES spectrum. Isomers 2 and 3, which have lower electron binding energies, were also found to be present in the experiment. Chemical bonding analyses showed that isomer 1 is an all-boron analogue of benzo[ghi]fluoranthene (C18H10), whereas the borospherene isomer 2 possesses 18π electrons, conforming to the 2(N + 1)2 electron counting rule for spherical aromaticity. For the B29 neutral cluster, the seashell-like borospherene isomer is the global minimum, significantly lower in energy than the stingray-shaped quasi-planar structure.
Co-reporter:Timur R. Galeev, Alexander S. Ivanov, Constantin Romanescu, Wei-Li Li, Konstantin V. Bozhenko, Lai-Sheng Wang and Alexander I. Boldyrev
Physical Chemistry Chemical Physics 2011 - vol. 13(Issue 19) pp:NaN8810-8810
Publication Date(Web):2011/04/12
DOI:10.1039/C1CP20359B
In this joint experimental and theoretical work we present a novel type of structural transition occurring in the series of CxB8−x− (x = 1–8) mixed clusters upon increase of the carbon content from x = 2 to x = 3. The wheel to ring transition is surprising because it is rather planar-to-linear type of transition to be expected in the series since B8, B8−, B82− and CB7− are known to possess wheel-type global minimum structures while C8 is linear.
Co-reporter:Hui Bai, Hua-Jin Zhai, Si-Dian Li and Lai-Sheng Wang
Physical Chemistry Chemical Physics 2013 - vol. 15(Issue 24) pp:NaN9653-9653
Publication Date(Web):2013/04/17
DOI:10.1039/C3CP50167A
We report a photoelectron spectroscopy and density-functional theory study of the B12Au− and B13O− clusters and their neutrals, which are shown to be six π electron aromatic compounds between the quasi-planar all-boron B12 benzene-analogue and a monovalent Au or BO ligand. Electron affinities of B12Au and B13O are measured to be 3.48 ± 0.04 and 3.90 ± 0.04 eV, respectively. Structural searches are performed for B12Au− and B13O−, which are compared with the isovalent B12H− cluster. The global minima of B12Au− and B13O− both feature an almost intact B12 cluster with the Au and BO ligands bonded to its periphery, respectively. For B12Au−, a low-lying isomer is also identified, which is only 0.4 kcal mol−1 above the global minimum, in agreement with the experimental observation of a weakly populated isomer in the cluster beam of B12Au−. These aromatic compound clusters provide new examples for the Au/H isolobal analogy and the boronyl (BO) chemistry.
Co-reporter:Hou-Ji Cao, Qianyi Zhao, Qian-Fan Zhang, Jiaxuan Li, Ewan J. M. Hamilton, Jie Zhang, Lai-Sheng Wang and Xuenian Chen
Dalton Transactions 2016 - vol. 45(Issue 25) pp:NaN10199-10199
Publication Date(Web):2016/04/28
DOI:10.1039/C6DT01272H
Agostic interactions are often used to activate inert C–H bonds, and thus facilitate new reactions. We report the first example of designed catalysts based on the agostic interaction. Novel copper(I) complexes [BBN(pzx)2]Cu(PPh3)n (BBN = 9-borabicyclo[3.3.1]nonane; pzx = 3-substituted pyrazole; x = H, n = 2; x = Me, n = 1) and {[BBN(pziPr)2]Cu}2 have been synthesized and characterized. Single crystal studies of the three compounds show weak intramolecular C–H⋯Cu interactions which can be assigned as agostic or anagostic interactions. Catalytic studies of these complexes toward carbenoid insertion into N–H bonds indicate these weak interactions act as a “switch” which will be turned “on” if interacting with the substrate and “off” if eliminating the product and regenerating the weak interaction. The process of the “switch” turning “on” or “off”, which is related to the catalytic effect, is found to be influenced by both steric effects and the solvent: a less sterically hindered catalyst in non-coordinating benzene results in high yield, while a more sterically hindered catalyst in coordinating THF results in relatively low yield.
Co-reporter:Dao-Ling Huang, Hong-Tao Liu, Chuan-Gang Ning, Guo-Zhu Zhu and Lai-Sheng Wang
Chemical Science (2010-Present) 2015 - vol. 6(Issue 5) pp:NaN3138-3138
Publication Date(Web):2015/03/17
DOI:10.1039/C5SC00704F
Deprotonated thymine can exist in two different forms, depending on which of its two N sites is deprotonated: N1[T–H]− or N3[T–H]−. Here we report a photodetachment study of the N1[T–H]− isomer cooled in a cryogenic ion trap and the observation of an excited dipole-bound state. Eighteen vibrational levels of the dipole-bound state are observed, and its vibrational ground state is found to be 238 ± 5 cm−1 below the detachment threshold of N1[T–H]−. The electron affinity of the deprotonated thymine radical (N1[T–H]˙) is measured accurately to be 26322 ± 5 cm−1 (3.2635 ± 0.0006 eV). By tuning the detachment laser to the sixteen vibrational levels of the dipole-bound state that are above the detachment threshold, highly non-Franck–Condon resonant-enhanced photoelectron spectra are obtained due to state- and mode-selective vibrational autodetachment. Much richer vibrational information is obtained for the deprotonated thymine radical from the photodetachment and resonant-enhanced photoelectron spectroscopy. Eleven fundamental vibrational frequencies in the low-frequency regime are obtained for the N1[T–H]˙ radical, including the two lowest-frequency internal rotational modes of the methyl group at 70 ± 8 cm−1 and 92 ± 5 cm−1.