Abstract:In spite of a spate of studies of various water clusters, a few theoretical studies on the water heptamer are available. State-of-the-art ab initio calculations are thus carried out on twelve possible water heptamer structures to explore the conformation as well as spectroscopic properties of this water cluster. Two three-dimensional cagelike structures comprised of seven-membered cyclic rings with three additional hydrogen bondings were found to be the lowest-lying energy heptamer conformers. The global minim… Show more
“…Shields et al 70 applied Eq. (6) at the MP2/ADZ//MP2/6-31G* level and Richard et al used the 1 /2-1 /2 mixing ratio at MP2/AVXZ (X = D, T, Q, 5), 94 while Kim et al 54 reported that the average of the uncorrected and BSSE-corrected binding energies "is nearly invariant to the basis sets larger than TZ2P++ for the water hexamer." The contribution of the present study consists of the fact that the mixing ratio between D e and D e CP (previously suggested in a heuristic manner) is determined via a least-mean-squares approach from a larger dataset that encompasses clusters of various sizes.…”
Section: A Validation Using the Results For The (H 2 O) 2-68 Clustersmentioning
confidence: 99%
“…50 The binding energy of the water heptamer has been reported at both the MP2 and CCSD(T) theories. Acelas et al 76 studied five different structures at the MP2/6-311++G(d,p) and CCSD(T)/6-311++G(d,p) levels, while Kim et al 54 reported ten different isomers at MP2 with similar quality basis sets. The octamer and endecamer systems have been treated with MP2 by one of us 43 employing as large basis sets as aug-cc-pV5Z.…”
We report MP2 and Coupled Cluster Singles, Doubles, and perturbative Triples [CCSD(T)] binding energies with basis sets up to pentuple zeta quality for the (H2O)m=2-6,8 water clusters. Our best CCSD(T)/Complete Basis Set (CBS) estimates are -4.99 ± 0.04 kcal/mol (dimer), -15.8 ± 0.1 kcal/mol (trimer), -27.4 ± 0.1 kcal/mol (tetramer), -35.9 ± 0.3 kcal/mol (pentamer), -46.2 ± 0.3 kcal/mol (prism hexamer), -45.9 ± 0.3 kcal/mol (cage hexamer), -45.4 ± 0.3 kcal/mol (book hexamer), -44.3 ± 0.3 kcal/mol (ring hexamer), -73.0 ± 0.5 kcal/mol (D2d octamer), and -72.9 ± 0.5 kcal/mol (S4 octamer). We have found that the percentage of both the uncorrected (De) and basis set superposition error-corrected (De (CP)) binding energies recovered with respect to the CBS limit falls into a narrow range on either sides of the CBS limit for each basis set for all clusters. In addition, this range decreases upon increasing the basis set. Relatively accurate estimates (within <0.5%) of the CBS limits can be obtained when using the "23, 13" (for the AVDZ set) or the "12, 12" (for the AVTZ, AVQZ, and AV5Z sets) mixing ratio between De and De (CP). These mixing rations are determined via a least-mean-squares approach from a dataset that encompasses clusters of various sizes. Based on those findings, we propose an accurate and efficient computational protocol that can be presently used to estimate accurate binding energies of water clusters containing up to 30 molecules (for CCSD(T)) and up to 100 molecules (for MP2).
“…Shields et al 70 applied Eq. (6) at the MP2/ADZ//MP2/6-31G* level and Richard et al used the 1 /2-1 /2 mixing ratio at MP2/AVXZ (X = D, T, Q, 5), 94 while Kim et al 54 reported that the average of the uncorrected and BSSE-corrected binding energies "is nearly invariant to the basis sets larger than TZ2P++ for the water hexamer." The contribution of the present study consists of the fact that the mixing ratio between D e and D e CP (previously suggested in a heuristic manner) is determined via a least-mean-squares approach from a larger dataset that encompasses clusters of various sizes.…”
Section: A Validation Using the Results For The (H 2 O) 2-68 Clustersmentioning
confidence: 99%
“…50 The binding energy of the water heptamer has been reported at both the MP2 and CCSD(T) theories. Acelas et al 76 studied five different structures at the MP2/6-311++G(d,p) and CCSD(T)/6-311++G(d,p) levels, while Kim et al 54 reported ten different isomers at MP2 with similar quality basis sets. The octamer and endecamer systems have been treated with MP2 by one of us 43 employing as large basis sets as aug-cc-pV5Z.…”
We report MP2 and Coupled Cluster Singles, Doubles, and perturbative Triples [CCSD(T)] binding energies with basis sets up to pentuple zeta quality for the (H2O)m=2-6,8 water clusters. Our best CCSD(T)/Complete Basis Set (CBS) estimates are -4.99 ± 0.04 kcal/mol (dimer), -15.8 ± 0.1 kcal/mol (trimer), -27.4 ± 0.1 kcal/mol (tetramer), -35.9 ± 0.3 kcal/mol (pentamer), -46.2 ± 0.3 kcal/mol (prism hexamer), -45.9 ± 0.3 kcal/mol (cage hexamer), -45.4 ± 0.3 kcal/mol (book hexamer), -44.3 ± 0.3 kcal/mol (ring hexamer), -73.0 ± 0.5 kcal/mol (D2d octamer), and -72.9 ± 0.5 kcal/mol (S4 octamer). We have found that the percentage of both the uncorrected (De) and basis set superposition error-corrected (De (CP)) binding energies recovered with respect to the CBS limit falls into a narrow range on either sides of the CBS limit for each basis set for all clusters. In addition, this range decreases upon increasing the basis set. Relatively accurate estimates (within <0.5%) of the CBS limits can be obtained when using the "23, 13" (for the AVDZ set) or the "12, 12" (for the AVTZ, AVQZ, and AV5Z sets) mixing ratio between De and De (CP). These mixing rations are determined via a least-mean-squares approach from a dataset that encompasses clusters of various sizes. Based on those findings, we propose an accurate and efficient computational protocol that can be presently used to estimate accurate binding energies of water clusters containing up to 30 molecules (for CCSD(T)) and up to 100 molecules (for MP2).
“…It is interesting to compare the relative stability of the clusters from the hydrogen bonding analysis and the second order difference in energy (D 2 E) analysis. As shown in Figure 2d, although there is only one HB per each water molecule in the cyclic structure of (H 2 O) [3][4][5] , the HB strength is very strong in (H 2 O) [4][5] . Therefore the second order difference in energy (D 2 E) of these two clusters, especially (H 2 O) 4 is positive.…”
Section: Energetic Stabilitymentioning
confidence: 91%
“…There are a larger number of energetically competing isomers for hexamer, including ring, book, bag, prism, cage, and boat structures [14][15][16][17][18][28][29][30][31]. For water cluster (H 2 O) n , n = 7-10, the structures are either an octamer ((H 2 O) 8 ) or derivatives of the water octamer [4][5][6][7][8]27].…”
“…There exist multiple low-lying isomers, which can be classified as Prism, Cage, and Chair conformations ( Figure 6). 50,51,189,196 A Prism structure has been calculated as the lowest energy heptamer with conventional MP2 calculations 51,196 and with RI-MP2 extrapolations to the estimated CBS limit.…”
Although the first ab initio Hartree-Fock computations of the water dimer were reported more than four decades ago, the detailed characterization of water clusters with sophisticated electronic structure techniques remains an important and vibrant area of research. The field of computational quantum chemistry has made significant advances since those pioneering studies. Geometry optimizations of the water dimer can now be carried out at the CCSDTQ level, and CCSD(T) energies can be computed with the aug-cc-pVTZ basis for clusters as large as (H 2 O) 17 . Some of these high-level studies are starting to reveal that the electronic structure is harder to describe for some hydrogen bonds than others. For example, discrepancies between MP2 and CCSD(T) energetics tend to increase when there are qualitative differences in the hydrogen-bonding networks of the water clusters being studied. This review highlights the recent and exciting work in this area and provides an overview of popular strategies for generating reliable properties and benchmark quality energetics for water clusters with correlated wavefunction methods. C 2013 John Wiley & Sons, Ltd.
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