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Hydrogen Bond versus Anti-Hydrogen Bond: A Comparative Analysis Based on the Electron Density Topology
The theory of atoms in molecules is used to examine the nature of anti-hydrogen bond (anti-H bond) interaction. Contrary to what is found in normal hydrogen bond (H bond) complexes, which are characterized by lengthening of the X−H bond and a red shift of its stretching frequency, the anti-H bond le...
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Published in: | The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 1999-08, Vol.103 (32), p.6394-6401 |
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container_end_page | 6401 |
container_issue | 32 |
container_start_page | 6394 |
container_title | The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory |
container_volume | 103 |
creator | Cubero, E Orozco, M Hobza, P Luque, F. J |
description | The theory of atoms in molecules is used to examine the nature of anti-hydrogen bond (anti-H bond) interaction. Contrary to what is found in normal hydrogen bond (H bond) complexes, which are characterized by lengthening of the X−H bond and a red shift of its stretching frequency, the anti-H bond leads to a shortening of the X−H bond length and a blue shift of its vibrational frequency. The topological properties of the electron density have been determined for a series of C−H···π complexes, which exhibit either anti-H bond or normal H bond character, as well as for the complexes C6H5F···HCCl3 and C6H6···HF, which are representative cases of anti- and normal H bonds. Inspection of the set of topological criteria utilized to characterize conventional H bonds shows no relevant difference in the two classes of H···π complexes. Analysis of the results suggests that the specific features of the anti-H bond originates from the redistribution of electron density in the C−H bond induced upon complexation, which in turn evidences the different response − dispersion versus electrostatic− of the interacting monomer for stabilizing the complex. |
doi_str_mv | 10.1021/jp990258f |
format | article |
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J</creator><creatorcontrib>Cubero, E ; Orozco, M ; Hobza, P ; Luque, F. J</creatorcontrib><description>The theory of atoms in molecules is used to examine the nature of anti-hydrogen bond (anti-H bond) interaction. Contrary to what is found in normal hydrogen bond (H bond) complexes, which are characterized by lengthening of the X−H bond and a red shift of its stretching frequency, the anti-H bond leads to a shortening of the X−H bond length and a blue shift of its vibrational frequency. The topological properties of the electron density have been determined for a series of C−H···π complexes, which exhibit either anti-H bond or normal H bond character, as well as for the complexes C6H5F···HCCl3 and C6H6···HF, which are representative cases of anti- and normal H bonds. Inspection of the set of topological criteria utilized to characterize conventional H bonds shows no relevant difference in the two classes of H···π complexes. Analysis of the results suggests that the specific features of the anti-H bond originates from the redistribution of electron density in the C−H bond induced upon complexation, which in turn evidences the different response − dispersion versus electrostatic− of the interacting monomer for stabilizing the complex.</description><identifier>ISSN: 1089-5639</identifier><identifier>EISSN: 1520-5215</identifier><identifier>DOI: 10.1021/jp990258f</identifier><language>eng</language><publisher>American Chemical Society</publisher><ispartof>The journal of physical chemistry. 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Inspection of the set of topological criteria utilized to characterize conventional H bonds shows no relevant difference in the two classes of H···π complexes. Analysis of the results suggests that the specific features of the anti-H bond originates from the redistribution of electron density in the C−H bond induced upon complexation, which in turn evidences the different response − dispersion versus electrostatic− of the interacting monomer for stabilizing the complex.</description><issn>1089-5639</issn><issn>1520-5215</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1999</creationdate><recordtype>article</recordtype><recordid>eNptkD1PwzAQQC0EEqUw8A-8MDC42E6cNmz9DlIFSBQxWk58LilpHNlpRTZW_ia_hKCiSkhMd6d7esND6JLRHqOc3ayrOKZcDMwR6jDBKRGcieN2p4OYiCiIT9GZ92tKKQt42EF50mhnV1DikS013oHzW4-HZZ2TP5_br49PPMRju6mUU3W-gxZSReNzj0fKg8a2xPUr4GkBWe3aYwKlz-sGL21lC7tqztGJUYWHi9_ZRc-z6XKckMXD_G48XBDFY1ETnWoFiutAhIYZFkLMdShSPtA6ggCE0RCJNOMpmBAiyjNueNQPqNZxqJlmQRdd772Zs947MLJy-Ua5RjIqfxrJQ6OWJXs29zW8H0Dl3mTr7Au5fHySk2Se3L-ImZy3_NWeV5mXa7t1bQL_j_cbYAN3hw</recordid><startdate>19990812</startdate><enddate>19990812</enddate><creator>Cubero, E</creator><creator>Orozco, M</creator><creator>Hobza, P</creator><creator>Luque, F. 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Contrary to what is found in normal hydrogen bond (H bond) complexes, which are characterized by lengthening of the X−H bond and a red shift of its stretching frequency, the anti-H bond leads to a shortening of the X−H bond length and a blue shift of its vibrational frequency. The topological properties of the electron density have been determined for a series of C−H···π complexes, which exhibit either anti-H bond or normal H bond character, as well as for the complexes C6H5F···HCCl3 and C6H6···HF, which are representative cases of anti- and normal H bonds. Inspection of the set of topological criteria utilized to characterize conventional H bonds shows no relevant difference in the two classes of H···π complexes. Analysis of the results suggests that the specific features of the anti-H bond originates from the redistribution of electron density in the C−H bond induced upon complexation, which in turn evidences the different response − dispersion versus electrostatic− of the interacting monomer for stabilizing the complex.</abstract><pub>American Chemical Society</pub><doi>10.1021/jp990258f</doi><tpages>8</tpages></addata></record> |
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title | Hydrogen Bond versus Anti-Hydrogen Bond: A Comparative Analysis Based on the Electron Density Topology |
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