Relative stability of planar versus double-ring tubular isomers of neutral and anionic boron cluster B20 and B20-.

High-level ab initio molecular-orbital methods have been employed to determine the relative stability among four neutral and anionic B20 isomers, particularly the double-ring tubular isomer versus three low-lying planar isomers. Calculations with the fourth-order Moller-Plessset perturbation theory [MP4(SDQ)] and Dunning's correlation consistent polarized valence triple zeta basis set as well as with the coupled-cluster method including single, double, and noniteratively perturbative triple excitations and the 6-311G(d) basis set show that the double-ring tubular isomer is appreciably lower in energy than the three planar isomers and is thus likely the global minimum of neutral B20 cluster. In contrast, calculations with the MP4(SDQ) level of theory and 6-311+G(d) basis set show that the double-ring anion isomer is appreciably higher in energy than two of the three planar isomers. In addition, the temperature effects on the relative stability of both 10B20- and 11B20- anion isomers are examined using the density-functional theory. It is found that the three planar anion isomers become increasingly more stable than the double-ring isomer with increasing the temperature. These results are consistent with the previous conclusion based on a joint experimental/simulated anion photoelectron spectroscopy study [B. Kiran et al., Proc. Natl. Acad. Sci. U.S.A. 102, 961 (2005)], that is, the double-ring anion isomer is notably absent from the experimental spectra. The high stability of the double-ring neutral isomer of B20 can be attributed in part to the strong aromaticity as characterized by its large negative nucleus-independent chemical shift. The high-level ab initio calculations suggest that the planar-to-tubular structural transition starts at B20 for neutral clusters but should occur beyond the size of B20- for the anion clusters.

[1]  Rodney J. Bartlett,et al.  Theory and implementation of the MBPT density matrix. An application to one-electron properties , 1988 .

[2]  M. Plesset,et al.  Note on an Approximation Treatment for Many-Electron Systems , 1934 .

[3]  Parr,et al.  Development of the Colle-Salvetti correlation-energy formula into a functional of the electron density. , 1988, Physical review. B, Condensed matter.

[4]  Ayhan Demirbas,et al.  Hydrogen and Boron as Recent Alternative Motor Fuels , 2005 .

[5]  X. Zeng,et al.  Metallic single-walled silicon nanotubes. , 2004, Proceedings of the National Academy of Sciences of the United States of America.

[6]  G. Seifert,et al.  Analysis of Aromatic Delocalization: Individual Molecular Orbital Contributions to Nucleus-Independent Chemical Shifts , 2003 .

[7]  Michael J. Frisch,et al.  MP2 energy evaluation by direct methods , 1988 .

[8]  D. Astruc,et al.  Gold nanoparticles: assembly, supramolecular chemistry, quantum-size-related properties, and applications toward biology, catalysis, and nanotechnology. , 2004, Chemical reviews.

[9]  M. Head‐Gordon,et al.  A fifth-order perturbation comparison of electron correlation theories , 1989 .

[10]  A. Quandt,et al.  Nanotubules of bare boron clusters: Ab initio and density functional study , 1997 .

[11]  Manabu Oumi,et al.  A doubles correction to electronic excited states from configuration interaction in the space of single substitutions , 1994 .

[12]  Martin Head-Gordon,et al.  Quadratic configuration interaction. A general technique for determining electron correlation energies , 1987 .

[13]  L. Hanley,et al.  Collision-induced dissociation and ab initio studies of boron cluster ions: determination of structures and stabilities , 1988 .

[14]  Martin Head-Gordon,et al.  Analytic MP2 frequencies without fifth-order storage. Theory and application to bifurcated hydrogen bonds in the water hexamer , 1994 .

[15]  Wei An,et al.  Ab initio calculation of bowl, cage, and ring isomers of C20 and C20-. , 2005, The Journal of chemical physics.

[16]  S. Bulusu,et al.  Planar-to-tubular structural transition in boron clusters: B20 as the embryo of single-walled boron nanotubes. , 2005, Proceedings of the National Academy of Sciences of the United States of America.

[17]  S. Yoo,et al.  Structures and stability of medium-sized silicon clusters. III. Reexamination of motif transition in growth pattern from Si15 to Si20. , 2005, The Journal of chemical physics.

[18]  M. Dresselhaus,et al.  Physical properties of carbon nanotubes , 1998 .

[19]  Burke,et al.  Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.

[20]  H. Mao,et al.  Superconductivity in Boron , 2001, Science.

[21]  Paul von Ragué Schleyer,et al.  Nucleus-Independent Chemical Shifts:  A Simple and Efficient Aromaticity Probe. , 1996, Journal of the American Chemical Society.

[22]  P. Buseck,et al.  Icosahedral packing of B12 icosahedra in boron suboxide (B6O) , 1998, Nature.

[23]  Jun Li,et al.  Hydrocarbon analogues of boron clusters — planarity, aromaticity and antiaromaticity , 2003, Nature materials.

[24]  Donald G. Truhlar,et al.  Multi-coefficient extrapolated density functional theory for thermochemistry and thermochemical kinetics , 2005 .

[25]  Svein Saebo,et al.  Avoiding the integral storage bottleneck in LCAO calculations of electron correlation , 1989 .

[26]  Frank Weinhold,et al.  Natural chemical shielding analysis of nuclear magnetic resonance shielding tensors from gauge-including atomic orbital calculations , 1997 .

[27]  I. Boustani,et al.  New quasi-planar surfaces of bare boron , 1997 .

[28]  Perkins,et al.  Direct Observation of (B12)(B12)12 Supericosahedra as the Basic Structural Element in YB66. , 1996, Physical review letters.

[29]  Michael J. Frisch,et al.  Semi-direct algorithms for the MP2 energy and gradient , 1990 .

[30]  P. Schleyer,et al.  Evidence for d orbital aromaticity in square planar coinage metal clusters. , 2005, Journal of the American Chemical Society.

[31]  Angel Rubio,et al.  Ab initio study of B32 clusters: competition between spherical, quasiplanar and tubular isomers , 1999 .

[32]  I. Boustani,et al.  Ab initiodensity functional investigation ofB24clusters: Rings, tubes, planes, and cages , 2003, physics/0305103.

[33]  T. H. Dunning Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen , 1989 .

[34]  P. Schleyer,et al.  Antiaromaticity in bare deltahedral silicon clusters satisfying Wade's and Hirsch's rules: an apparent correlation of antiaromaticity with high symmetry. , 2004, Journal of the American Chemical Society.

[35]  Anastassia N Alexandrova,et al.  Hepta- and octacoordinate boron in molecular wheels of eight- and nine-atom boron clusters: observation and confirmation. , 2003, Angewandte Chemie.

[36]  Manabu Oumi,et al.  A perturbative correction to restricted open shell configuration interaction with single substitutions for excited states of radicals , 1995 .

[37]  S. Yamaoka,et al.  High-Temperature Cubic Boron Nitride P-N Junction Diode Made at High Pressure , 1987, Science.

[38]  J. S. Binkley,et al.  Electron correlation theories and their application to the study of simple reaction potential surfaces , 1978 .

[39]  Analytical MBPT(4) gradients , 1988 .

[40]  A. Becke Density-functional thermochemistry. III. The role of exact exchange , 1993 .

[41]  I. Boustani New Convex and Spherical Structures of Bare Boron Clusters , 1997 .

[42]  The planar-to-tubular structural transition in boron clusters from optical absorption. , 2005, The Journal of chemical physics.

[43]  I. Boustani,et al.  Systematic ab initio investigation of bare boron clusters:mDetermination of the geometryand electronic structures of B n (n=2–14) , 1997 .

[44]  K. Burke,et al.  Generalized Gradient Approximation Made Simple [Phys. Rev. Lett. 77, 3865 (1996)] , 1997 .

[45]  D. Meinköhn,et al.  The ignition of boron particles , 1985 .

[46]  Andreas Hirsch,et al.  Spherical Aromaticity in Ih Symmetrical Fullerenes: The 2(N+1)2 Rule. , 2000, Angewandte Chemie.

[47]  J. Aihara,et al.  Verification of the 2(N + 1)2 rule for fullerenes , 2003 .

[48]  Xiao Cheng Zeng,et al.  Au42: an alternative icosahedral golden fullerene cage. , 2005, Journal of the American Chemical Society.

[49]  Hong Wei Jin,et al.  Structure and Stability of B5, B5+, and B5- Clusters , 2002 .

[50]  John A. Pople,et al.  Approximate fourth-order perturbation theory of the electron correlation energy , 1978 .