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Effect of quantum nuclear motion on hydrogen bonding
This work considers how the properties of hydrogen bonded complexes, X-H⋯Y, are modified by the quantum motion of the shared proton. Using a simple two-diabatic state model Hamiltonian, the analysis of the symmetric case, where the donor (X) and acceptor (Y) have the same proton affinity, is carried...
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Published in: | The Journal of chemical physics 2014-05, Vol.140 (17), p.174508-174508 |
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container_end_page | 174508 |
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container_title | The Journal of chemical physics |
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creator | McKenzie, Ross H Bekker, Christiaan Athokpam, Bijyalaxmi Ramesh, Sai G |
description | This work considers how the properties of hydrogen bonded complexes, X-H⋯Y, are modified by the quantum motion of the shared proton. Using a simple two-diabatic state model Hamiltonian, the analysis of the symmetric case, where the donor (X) and acceptor (Y) have the same proton affinity, is carried out. For quantitative comparisons, a parametrization specific to the O-H⋯O complexes is used. The vibrational energy levels of the one-dimensional ground state adiabatic potential of the model are used to make quantitative comparisons with a vast body of condensed phase data, spanning a donor-acceptor separation (R) range of about 2.4-3.0 Å, i.e., from strong to weak hydrogen bonds. The position of the proton (which determines the X-H bond length) and its longitudinal vibrational frequency, along with the isotope effects in both are described quantitatively. An analysis of the secondary geometric isotope effect, using a simple extension of the two-state model, yields an improved agreement of the predicted variation with R of frequency isotope effects. The role of bending modes is also considered: their quantum effects compete with those of the stretching mode for weak to moderate H-bond strengths. In spite of the economy in the parametrization of the model used, it offers key insights into the defining features of H-bonds, and semi-quantitatively captures several trends. |
doi_str_mv | 10.1063/1.4873352 |
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Using a simple two-diabatic state model Hamiltonian, the analysis of the symmetric case, where the donor (X) and acceptor (Y) have the same proton affinity, is carried out. For quantitative comparisons, a parametrization specific to the O-H⋯O complexes is used. The vibrational energy levels of the one-dimensional ground state adiabatic potential of the model are used to make quantitative comparisons with a vast body of condensed phase data, spanning a donor-acceptor separation (R) range of about 2.4-3.0 Å, i.e., from strong to weak hydrogen bonds. The position of the proton (which determines the X-H bond length) and its longitudinal vibrational frequency, along with the isotope effects in both are described quantitatively. An analysis of the secondary geometric isotope effect, using a simple extension of the two-state model, yields an improved agreement of the predicted variation with R of frequency isotope effects. The role of bending modes is also considered: their quantum effects compete with those of the stretching mode for weak to moderate H-bond strengths. 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Using a simple two-diabatic state model Hamiltonian, the analysis of the symmetric case, where the donor (X) and acceptor (Y) have the same proton affinity, is carried out. For quantitative comparisons, a parametrization specific to the O-H⋯O complexes is used. The vibrational energy levels of the one-dimensional ground state adiabatic potential of the model are used to make quantitative comparisons with a vast body of condensed phase data, spanning a donor-acceptor separation (R) range of about 2.4-3.0 Å, i.e., from strong to weak hydrogen bonds. The position of the proton (which determines the X-H bond length) and its longitudinal vibrational frequency, along with the isotope effects in both are described quantitatively. An analysis of the secondary geometric isotope effect, using a simple extension of the two-state model, yields an improved agreement of the predicted variation with R of frequency isotope effects. The role of bending modes is also considered: their quantum effects compete with those of the stretching mode for weak to moderate H-bond strengths. In spite of the economy in the parametrization of the model used, it offers key insights into the defining features of H-bonds, and semi-quantitatively captures several trends.</description><subject>BOND LENGTHS</subject><subject>Bonding strength</subject><subject>Energy levels</subject><subject>GROUND STATES</subject><subject>HAMILTONIANS</subject><subject>HYDROGEN</subject><subject>Hydrogen bonding</subject><subject>Hydrogen bonds</subject><subject>INORGANIC, ORGANIC, PHYSICAL AND ANALYTICAL CHEMISTRY</subject><subject>Isotope effect</subject><subject>ISOTOPE EFFECTS</subject><subject>Parameterization</subject><subject>PROTONS</subject><issn>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNpF0M9LwzAUB_AgipvTg_-AFLzoofO9JE3ao4z5AwZe9BzaNNk62mRr2oP_vZHNCYF3-fB9L19CbhHmCII94ZznkrGMnpEpQl6kUhRwTqYAFNNCgJiQqxC2AICS8ksyoTxHFFxOCV9aa_SQeJvsx9INY5e4Ubem7JPOD413SXyb77r3a-OSyru6cetrcmHLNpib45yRr5fl5-ItXX28vi-eV6nmnA5pxeISZnlpNegSZaV5kTHBS8BKoGXUVhwLwTKE2ta1riLjzAC3nGoNFZuR-0OuD0Ojgm4GozfaOxcvVpTSjBbIono4qF3v96MJg-qaoE3bls74MSjMKOMgmSz-A09068fexT8oilSKTOY8j-rxoHTvQ-iNVbu-6cr-WyGo38IVqmPh0d4dE8eqM_VJ_jXMfgB2-3ev</recordid><startdate>20140507</startdate><enddate>20140507</enddate><creator>McKenzie, Ross H</creator><creator>Bekker, Christiaan</creator><creator>Athokpam, Bijyalaxmi</creator><creator>Ramesh, Sai G</creator><general>American Institute of Physics</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><scope>OTOTI</scope></search><sort><creationdate>20140507</creationdate><title>Effect of quantum nuclear motion on hydrogen bonding</title><author>McKenzie, Ross H ; Bekker, Christiaan ; Athokpam, Bijyalaxmi ; Ramesh, Sai G</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c442t-b31163f4afc0ca17bc495364a01b61f32fb41963510dfddcbc0c43e04f42cc0b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>BOND LENGTHS</topic><topic>Bonding strength</topic><topic>Energy levels</topic><topic>GROUND STATES</topic><topic>HAMILTONIANS</topic><topic>HYDROGEN</topic><topic>Hydrogen bonding</topic><topic>Hydrogen bonds</topic><topic>INORGANIC, ORGANIC, PHYSICAL AND ANALYTICAL CHEMISTRY</topic><topic>Isotope effect</topic><topic>ISOTOPE EFFECTS</topic><topic>Parameterization</topic><topic>PROTONS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>McKenzie, Ross H</creatorcontrib><creatorcontrib>Bekker, Christiaan</creatorcontrib><creatorcontrib>Athokpam, Bijyalaxmi</creatorcontrib><creatorcontrib>Ramesh, Sai G</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>McKenzie, Ross H</au><au>Bekker, Christiaan</au><au>Athokpam, Bijyalaxmi</au><au>Ramesh, Sai G</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of quantum nuclear motion on hydrogen bonding</atitle><jtitle>The Journal of chemical physics</jtitle><addtitle>J Chem Phys</addtitle><date>2014-05-07</date><risdate>2014</risdate><volume>140</volume><issue>17</issue><spage>174508</spage><epage>174508</epage><pages>174508-174508</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><abstract>This work considers how the properties of hydrogen bonded complexes, X-H⋯Y, are modified by the quantum motion of the shared proton. Using a simple two-diabatic state model Hamiltonian, the analysis of the symmetric case, where the donor (X) and acceptor (Y) have the same proton affinity, is carried out. For quantitative comparisons, a parametrization specific to the O-H⋯O complexes is used. The vibrational energy levels of the one-dimensional ground state adiabatic potential of the model are used to make quantitative comparisons with a vast body of condensed phase data, spanning a donor-acceptor separation (R) range of about 2.4-3.0 Å, i.e., from strong to weak hydrogen bonds. The position of the proton (which determines the X-H bond length) and its longitudinal vibrational frequency, along with the isotope effects in both are described quantitatively. An analysis of the secondary geometric isotope effect, using a simple extension of the two-state model, yields an improved agreement of the predicted variation with R of frequency isotope effects. The role of bending modes is also considered: their quantum effects compete with those of the stretching mode for weak to moderate H-bond strengths. In spite of the economy in the parametrization of the model used, it offers key insights into the defining features of H-bonds, and semi-quantitatively captures several trends.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>24811647</pmid><doi>10.1063/1.4873352</doi><tpages>1</tpages><oa>free_for_read</oa></addata></record> |
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subjects | BOND LENGTHS Bonding strength Energy levels GROUND STATES HAMILTONIANS HYDROGEN Hydrogen bonding Hydrogen bonds INORGANIC, ORGANIC, PHYSICAL AND ANALYTICAL CHEMISTRY Isotope effect ISOTOPE EFFECTS Parameterization PROTONS |
title | Effect of quantum nuclear motion on hydrogen bonding |
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