Abstract
The diffusion Monte Carlo (DMC) method is applied to the water monomer, dimer, and hexamer using q-TIP4P/F, one of the most simple empirical water models with flexible monomers. The bias in the time step (Δτ) and population size (Nw) is investigated. For the binding energies, the bias in Δτ cancels nearly completely, whereas a noticeable bias in Nw remains. However, for the isotope shift (e.g, in the dimer binding energies between (H2O)2 and (D2O)2), the systematic errors in Nw do cancel. Consequently, very accurate results for the latter (within ∼0.01 kcal/mol) are obtained with moderate numerical effort (Nw ∼ 10(3)). For the water hexamer and its (D2O)6 isotopomer, the DMC results as a function of Nw are examined for the cage and prism isomers. For a given isomer, the issue of the walker population leaking out of the corresponding basin of attraction is addressed by using appropriate geometric constraints. The population size bias for the hexamer is more severe, and to maintain accuracy similar to that of the dimer, Nw must be increased by ∼2 orders of magnitude. Fortunately, when the energy difference between the cage and prism is taken, the biases cancel, thereby reducing the systematic errors to within ∼0.01 kcal/mol when using a population of Nw = 4.8 × 10(5) walkers. Consequently, a very accurate result for the isotope shift is also obtained. Notably, both the quantum and isotope effects for the prism-cage energy difference are small.
Highlights
Diffusion Monte Carlo (DMC)[1,2,3,4] has engendered significant attention in the literature because it is one of the few numerical methods that enable the computation of the ground state of many-body systems
Some examples of systems that have been examined with DMC are Bose condensates of parahydrogen and helium[9,10,11,12]; sheets of graphite and diamond[13]; fcc crystallized xenon at 0 K[7]; HF, HCN, and SF6 trapped in clusters of argon and helium[3, 14]; and water clusters with a special emphasis placed on the water hexamer[15,16,17,18,19,20,21,22]
We find that our DMC estimates of D0 for both (H2O)2 and (D2O)2 are about 1.5 kcal/mol higher than the experimental values reported in refs. 34, 35, which is a clear indication of the failure of the q-TIP4P/F potential energy surface (PES) in describing accurately the energetics of small water clusters
Summary
Assessing the Performance of the Diffusion Monte Carlo Method as Applied to the Water Monomer, Dimer, and Hexamer. For the isotope shift, (e.g, in the dimer binding energies between (H2O) and (D2O)2) the systematic errors in Nw do cancel. For the water hexamer and its (D2O) isotopomer the DMC results as a function of Nw are examined for the cage and prism isomers. When the energy difference between cage and prism is taken, the biases cancel, thereby reducing the systematic errors to within ∼ 0.01 kcal/mol when using a population of Nw = 4.8 × 105 walkers. A very accurate result for the isotope shift is obtained. Both the quantum and the isotope effects for the prism-cage energy difference are small
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