A short yet very weak dative bond: structure, bonding, and energetic properties of N(2)-BH(3)

The structure, bonding, and energetic properties of the N(2)-BH(3) complex are reported as characterized by density functional theory (DFT) and post-Hartree-Fock (HF) calculations. The equilibrium structure of the complex exhibits a short B-N distance near 1.6 A, comparable to that of a strong acid-...

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Veröffentlicht in:The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 2010-02, Vol.114 (7), p.2628-2636
Hauptverfasser: Smith, Elizabeth L, Sadowsky, Daniel, Phillips, James A, Cramer, Christopher J, Giesen, David J
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container_title The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory
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creator Smith, Elizabeth L
Sadowsky, Daniel
Phillips, James A
Cramer, Christopher J
Giesen, David J
description The structure, bonding, and energetic properties of the N(2)-BH(3) complex are reported as characterized by density functional theory (DFT) and post-Hartree-Fock (HF) calculations. The equilibrium structure of the complex exhibits a short B-N distance near 1.6 A, comparable to that of a strong acid-base complex like H(3)N-BH(3). However, the binding energy is only 5.7 kcal/mol at the CCSD(T)/6-311+G(2df,2dp) level of theory, which is reminiscent of a weak, nonbonded complex. Natural bond orbital (NBO) and atoms in molecules (AIM) analyses of the electron density from both DFT and post-HF calculations do indicate that the extent of charge transfer and covalent character in the B-N dative bond is only somewhat less than in comparable systems with fairly large binding energies (e.g., H(3)N-BH(3) and OC-BH(3)). Energy decomposition analysis indicates key differences between the N(2), CO, and NH(3) complexes, primarily associated with the natures of the lone pairs involved (sp vs sp(3)) and the donor/acceptor characteristics of the relevant occupied and virtual orbitals, both sigma and pi. Also, CCSD/6-311+G(2df,2dp) calculations indicate that the B-N distance potential is rather anharmonic and exhibits a flat, shelf-like region ranging from 2.1 to 2.5 A that lies about 1.5 kcal/mol above the minimum at 1.67 A. However, this region is more sloped and lies about 2.5 kcal/mol above the equilibrium region according to the CCSD(T)/6-311+G(2df,2dp)//CCSD/6-311+G(2df,2dp) potential. A 1D analysis of the vibrational motion along the B-N stretching coordinate in the CCSD/6-311+G(2df,2dp) potential indicates that the average B-N distance in the ground vibrational state is 1.71 A, about 0.04 A longer than the equilibrium distance. Furthermore, the vibrationally averaged distance obtained via an analysis of the CCSD(T)/6-311+G(2df,2dp)//CCSD/6-311+G(2df,2dp) potential was found to be 0.03 A longer than the CCSD(T)/6-311+G(2df,2dp) minimum.
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The equilibrium structure of the complex exhibits a short B-N distance near 1.6 A, comparable to that of a strong acid-base complex like H(3)N-BH(3). However, the binding energy is only 5.7 kcal/mol at the CCSD(T)/6-311+G(2df,2dp) level of theory, which is reminiscent of a weak, nonbonded complex. Natural bond orbital (NBO) and atoms in molecules (AIM) analyses of the electron density from both DFT and post-HF calculations do indicate that the extent of charge transfer and covalent character in the B-N dative bond is only somewhat less than in comparable systems with fairly large binding energies (e.g., H(3)N-BH(3) and OC-BH(3)). Energy decomposition analysis indicates key differences between the N(2), CO, and NH(3) complexes, primarily associated with the natures of the lone pairs involved (sp vs sp(3)) and the donor/acceptor characteristics of the relevant occupied and virtual orbitals, both sigma and pi. Also, CCSD/6-311+G(2df,2dp) calculations indicate that the B-N distance potential is rather anharmonic and exhibits a flat, shelf-like region ranging from 2.1 to 2.5 A that lies about 1.5 kcal/mol above the minimum at 1.67 A. However, this region is more sloped and lies about 2.5 kcal/mol above the equilibrium region according to the CCSD(T)/6-311+G(2df,2dp)//CCSD/6-311+G(2df,2dp) potential. A 1D analysis of the vibrational motion along the B-N stretching coordinate in the CCSD/6-311+G(2df,2dp) potential indicates that the average B-N distance in the ground vibrational state is 1.71 A, about 0.04 A longer than the equilibrium distance. Furthermore, the vibrationally averaged distance obtained via an analysis of the CCSD(T)/6-311+G(2df,2dp)//CCSD/6-311+G(2df,2dp) potential was found to be 0.03 A longer than the CCSD(T)/6-311+G(2df,2dp) minimum.</description><identifier>EISSN: 1520-5215</identifier><identifier>DOI: 10.1021/jp909059n</identifier><identifier>PMID: 20121205</identifier><language>eng</language><publisher>United States</publisher><ispartof>The journal of physical chemistry. 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A, Molecules, spectroscopy, kinetics, environment, &amp; general theory</jtitle><addtitle>J Phys Chem A</addtitle><date>2010-02-25</date><risdate>2010</risdate><volume>114</volume><issue>7</issue><spage>2628</spage><epage>2636</epage><pages>2628-2636</pages><eissn>1520-5215</eissn><abstract>The structure, bonding, and energetic properties of the N(2)-BH(3) complex are reported as characterized by density functional theory (DFT) and post-Hartree-Fock (HF) calculations. The equilibrium structure of the complex exhibits a short B-N distance near 1.6 A, comparable to that of a strong acid-base complex like H(3)N-BH(3). However, the binding energy is only 5.7 kcal/mol at the CCSD(T)/6-311+G(2df,2dp) level of theory, which is reminiscent of a weak, nonbonded complex. Natural bond orbital (NBO) and atoms in molecules (AIM) analyses of the electron density from both DFT and post-HF calculations do indicate that the extent of charge transfer and covalent character in the B-N dative bond is only somewhat less than in comparable systems with fairly large binding energies (e.g., H(3)N-BH(3) and OC-BH(3)). Energy decomposition analysis indicates key differences between the N(2), CO, and NH(3) complexes, primarily associated with the natures of the lone pairs involved (sp vs sp(3)) and the donor/acceptor characteristics of the relevant occupied and virtual orbitals, both sigma and pi. Also, CCSD/6-311+G(2df,2dp) calculations indicate that the B-N distance potential is rather anharmonic and exhibits a flat, shelf-like region ranging from 2.1 to 2.5 A that lies about 1.5 kcal/mol above the minimum at 1.67 A. However, this region is more sloped and lies about 2.5 kcal/mol above the equilibrium region according to the CCSD(T)/6-311+G(2df,2dp)//CCSD/6-311+G(2df,2dp) potential. A 1D analysis of the vibrational motion along the B-N stretching coordinate in the CCSD/6-311+G(2df,2dp) potential indicates that the average B-N distance in the ground vibrational state is 1.71 A, about 0.04 A longer than the equilibrium distance. Furthermore, the vibrationally averaged distance obtained via an analysis of the CCSD(T)/6-311+G(2df,2dp)//CCSD/6-311+G(2df,2dp) potential was found to be 0.03 A longer than the CCSD(T)/6-311+G(2df,2dp) minimum.</abstract><cop>United States</cop><pmid>20121205</pmid><doi>10.1021/jp909059n</doi><tpages>9</tpages></addata></record>
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title A short yet very weak dative bond: structure, bonding, and energetic properties of N(2)-BH(3)
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