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85033177261
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note
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Molar polarizabilities were calculated using the Clausius-Mossotti equation from Ref. 35 with index of refraction data and density from Ref. 12.
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38
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0000760197
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Calculated using the Clausius-Mossotti equation from Ref. 35, the dielectric constant for liquid methane from Ref. 12, and density from K. R. Ramaprasad, J. Caldwell, and D. S. McClure, Icarus 35, 400 (1978).
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85033183051
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HyperChem by Hypercube is a commercial software package which incorporates a friendly graphics interface with a variety of molecular modelling, semiempirical, and ab initio methods.
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V. V. Vasilyev, Acta Chim. Hungarica 130, 743 (1993); these calculations to n = 16 have been reproduced and extended it to n = 136, M. D. Tissandier, A. D. Earhart, S. I. Muhammad, and J. V. Coe, in preparation: M. D. Tissandier, Ph.D. thesis, The Ohio State University (1997).
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V. V. Vasilyev, Acta Chim. Hungarica 130, 743 (1993); these calculations to n = 16 have been reproduced and extended it to n = 136, M. D. Tissandier, A. D. Earhart, S. I. Muhammad, and J. V. Coe, in preparation: M. D. Tissandier, Ph.D. thesis, The Ohio State University (1997).
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85033183240
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Ph.D. thesis, The Ohio State University
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V. V. Vasilyev, Acta Chim. Hungarica 130, 743 (1993); these calculations to n = 16 have been reproduced and extended it to n = 136, M. D. Tissandier, A. D. Earhart, S. I. Muhammad, and J. V. Coe, in preparation: M. D. Tissandier, Ph.D. thesis, The Ohio State University (1997).
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s/T)/∂(1/T) determines the 0.226 eV value of the constant. 55 One could also use 0.443 eV for this constant to give a relation which roughly connects bulk to the calculated cluster values from I. P. Buffy and W. B. Brown, Chem. Phys. Lett. 109, 59 (1984), avoiding the offset issue.
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s/T)/∂(1/T) determines the 0.226 eV value of the constant. 55 One could also use 0.443 eV for this constant to give a relation which roughly connects bulk to the calculated cluster values from I. P. Buffy and W. B. Brown, Chem. Phys. Lett. 109, 59 (1984), avoiding the offset issue.
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Olesik, S.V.1
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85033179863
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note
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0 and the known optical polarizability of water, see the last paragraph of Sec. II A.
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63
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85033187888
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note
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w) vs 1/T.
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26444521590
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85033160024
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note
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The adiabatic energetic threshold determined in this work for seeing a hydrated electron from photoexcitation of water is 5.3 eV, so the observed threshold of 6.5 eV lies 1.2 eV above the minimum hydrated electron energy level, but 6.5 eV is not enough to access the conduction band, particularly when the associated reorganization energies are considered (see Fig. 5). The 10.06 eV PET of water suggests that 6.5 eV photons are about 3.6 eV shy of reaching the conduction band which is even too far to invoke electron-trapping states (however, lower values of the PET can change these arguments).
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67
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85033172288
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note
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Figure 2 in the present work shows why the photoemission threshold of water does not determine the vacuum level as tentatively assumed in Fig. 3 of Ref. 8.
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