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. Author manuscript; available in PMC: 2019 Dec 13.
Published in final edited form as: Faraday Discuss. 2018 Dec 13;212(0):467–497. doi: 10.1039/c8fd00092a

Table 4.

Values of C(T) in cm6/mol2 for D2O using various approximations and potentials and interpolated from experimental sources. The rigid-monomer calculations used potentials evaluated at the average ground rovibrational state geometry of D2O. The uncertainties are the statistical uncertainties of the calculation.

Temperature (K)
300 500 600 700 1000
value unc value unc value unc value unc value unc
CCpol−8sf (rigid) −2.53 ×106 4×104 9158 125 5277 50 2970 12 871 3
CCpol−8sf+CCpol3 (rigid, classical) −1.97 ×107 4×105 −13291 453 −197 140 878 63 605 12
CCpol−8sf+CCpol3 (rigid, semiclassical) −1.14×107 3×105 −10431 423 129 110 1031 40 592 14
CCpol−8sf+CCpol3 (rigid) −1.18×107 3×105 −10937 445 −85 144 1042 56 582 11
CCpol−8sf + CCpol3 (flexible) −1.07 ×107 3×105 −11966 499 103 193 1057 62 683 17
MB−pol (rigid) −1.34×107 4×105 −14751 406 −1664 134 144 49 385 12
MB−pol (flexible) −1.61×107 5×105 −19018 513 −1987 131 −15 58 351 15
Kell78 −17500 790 1320