CCSD(T) Complete Basis Set Limit Relative Energies for Low-Lying Water Hexamer Structures

被引:184
作者
Bates, Desiree M. [1 ]
Tschumper, Gregory S. [1 ]
机构
[1] Univ Mississippi, Dept Chem & Biochem, University, MS 38677 USA
基金
美国国家科学基金会;
关键词
COUPLED-CLUSTER CALCULATIONS; PI-PI INTERACTIONS; BINDING-ENERGIES; MOLLER-PLESSET; VIBRATIONAL FREQUENCIES; CAGE FORM; SPECTRA; SPECTROSCOPY; COMPUTATIONS; MOLECULES;
D O I
10.1021/jp8105919
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
MP2 and CCSD(T) complete basis set (CBS) limit relative electronic energies (Delta E-e) have been determined for eight low-lying structures of the water hexamer by combining explicitly correlated MP2-R12 computations with higher-order correlation corrections from CCSD(T) calculations. Higher-order correlation effects are quite substantial and increase Delta E-e by at least +0.19 kcal mol(-1) and as much as +0.59 kcal mol(-1). The effects from zero-point vibrational energy (ZPVE) have been assessed from unscaled harmonic vibrational frequencies computed at the MP2 level with a correlation consistent triple-zeta basis set (cc-pVTZ for H and aug-cc-pVTZ for O). ZPVE effects are even more significant than higher-order correlation effects and are uniformly negative, decreasing the relative energies by -0.16 kcal mol(-1) to -1.61 kcal mol(-1). Although it has been widely accepted that the cage becomes the lowest-energy structure after ZPVE effects are included [Nature 1996, 381, 501-503], the prism is consistently the most stable structure in this work, lying 0.06 kcal mol(-1) below the nearly isoenergetic cage isomer at the electronic MP2 CBS limit, 0.25 kcal mol(-1) below at the electronic CCSD(T) CBS limit, and 0.09 kcal mol(-1) below at the harmonic ZPVE corrected CCSD(T) CBS limit. Moreover, application of any uniform scaling factor less than unity to correct for anharmonicity further stabilizes the prism and increases the relative energies of the other structures.
引用
收藏
页码:3555 / 3559
页数:5
相关论文
共 57 条
  • [1] Anchoring the potential energy surface of the cyclic water trimer
    Anderson, JA
    Crager, K
    Fedoroff, L
    Tschumper, GS
    [J]. JOURNAL OF CHEMICAL PHYSICS, 2004, 121 (22) : 11023 - 11029
  • [2] [Anonymous], 2017, J MOL STRUCT, DOI DOI 10.1016/J.MOLSTRUC.2017.03.014
  • [3] [Anonymous], 2020, MOLPRO VERSION 2020
  • [4] Probing the effects of heterogeneity on delocalized π•••π interaction energies
    Bates, Desiree M.
    Anderson, Julie A.
    Oloyede, Ponmile
    Tschumper, Gregory S.
    [J]. PHYSICAL CHEMISTRY CHEMICAL PHYSICS, 2008, 10 (19) : 2775 - 2779
  • [5] CALCULATION OF SMALL MOLECULAR INTERACTIONS BY DIFFERENCES OF SEPARATE TOTAL ENERGIES - SOME PROCEDURES WITH REDUCED ERRORS
    BOYS, SF
    BERNARDI, F
    [J]. MOLECULAR PHYSICS, 1970, 19 (04) : 553 - &
  • [6] Non-covalent interactions in biomacromolecules
    Cerny, Jiri
    Hobza, Pavel
    [J]. PHYSICAL CHEMISTRY CHEMICAL PHYSICS, 2007, 9 (39) : 5291 - 5303
  • [7] PS13:: An open-source ab initio electronic structure package
    Crawford, T. Daniel
    Sherrill, C. David
    Valeev, Edward F.
    Fermann, Justin T.
    King, Rollin A.
    Leininger, Matthew L.
    Brown, Shawn T.
    Janssen, Curtis L.
    Seidl, Edward T.
    Kenny, Joseph P.
    Allen, Wesley D.
    [J]. JOURNAL OF COMPUTATIONAL CHEMISTRY, 2007, 28 (09) : 1610 - 1616
  • [8] Assessment of the accuracy of density functionals for prediction of relative energies and geometries of low-lying isomers of water hexamers
    Dahlke, Erin E.
    Olson, Ryan M.
    Leverentz, Hannah R.
    Truhlar, Donald G.
    [J]. JOURNAL OF PHYSICAL CHEMISTRY A, 2008, 112 (17) : 3976 - 3984
  • [9] On the contribution of vibrational anharmonicity to the binding energies of water clusters
    Diri, K
    Myshakin, EM
    Jordan, KD
    [J]. JOURNAL OF PHYSICAL CHEMISTRY A, 2005, 109 (17) : 4005 - 4009
  • [10] On the T-shaped structures of the benzene dimer
    DiStasio, Robert A., Jr.
    von Helden, Gert
    Steele, Ryan P.
    Head-Gordon, Martin
    [J]. CHEMICAL PHYSICS LETTERS, 2007, 437 (4-6) : 277 - 283