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Early molecular beam investigations of traditional ionic systems such as alkali and alkali-earth halides are reviewed in: Martin, T. P. Phys. Rep. 1983, 95, 167-199
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Early molecular beam investigations of traditional ionic systems such as alkali and alkali-earth halides are reviewed in: Martin, T. P. Phys. Rep. 1983, 95, 167-199.
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28544443382
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Canongia Lopes, J. N.; Deschamps, J.; Padua, A. A. H. J. Phys. Chem. B 2004, 108, 2038-2047.
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16
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4043134657
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See also (Additions and corrections): Canongia Lopes, J. N.; Deschamps, J.; Padua, A. A. H. J. Phys. Chem. B 2004, 108, 11250.
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See also (Additions and corrections): Canongia Lopes, J. N.; Deschamps, J.; Padua, A. A. H. J. Phys. Chem. B 2004, 108, 11250.
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17
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84906363065
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jj and differ from the popular Berthelot rules. Canongia Lopes, J. N.; and Padua, A. A. H. private communication. This point is discussed and clarified in: Canongia Lopes, J. N.; Padua, A. A. H. J. Phys. Chem. B 2006, 110, 19586-19592.
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jj and differ from the popular Berthelot rules. Canongia Lopes, J. N.; and Padua, A. A. H. private communication. This point is discussed and clarified in: Canongia Lopes, J. N.; Padua, A. A. H. J. Phys. Chem. B 2006, 110, 19586-19592.
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18
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84906391504
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The confining potential identically vanishes within a sphere whose radius R is significantly larger than the expected cluster radius. For r > R̄, the potential is given by VConf, σ(r, R̄)2, with α, 0.1 kJ/mol/Å2
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2.
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19
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28844497946
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Choudhury, A. R.; Winterton, N.; Steiner, A.; Cooper, A. I.; Johnson, K. A. J. Am. Chem. Soc. 2005, 127, 16792-16793.
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Winterton, N.2
Steiner, A.3
Cooper, A.I.4
Johnson, K.A.5
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20
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84906406167
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-
The computed lattice parameters are a, 10.318, b, 12.243, c, 21.877, α, 90.47, β, 97.52, and γ, 90.114 (lengths are in Å, and angles, in degrees) to be compared with the experimental values: a, 10.222, b, 12.534, c, 22.541, α, 90.0, β, 93.281, and γ, 90.0
-
The computed lattice parameters are a = 10.318, b = 12.243, c = 21.877, α = 90.47, β = 97.52, and γ = 90.114 (lengths are in Å, and angles, in degrees) to be compared with the experimental values: a = 10.222, b = 12.534, c = 22.541, α = 90.0, β = 93.281, and γ = 90.0).
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21
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33644909351
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Arce, A.; Rodriguez, H.; Soto, A. Fluid Phase Equilib. 2006, 242, 164-168.
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Arce, A.1
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84906377285
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∞ ∼ 2 is a property shared by most RTIL; see: Hu, Y.-F.; Xu, C.-M. Chem. Rev. 2006, in press.
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∞ ∼ 2 is a property shared by most RTIL; see: Hu, Y.-F.; Xu, C.-M. Chem. Rev. 2006, in press.
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23
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84906406165
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Smith, W.; Leslie, M.; Forester, T. R. DL-POLY, v2.14; Daresbury Laboratories: Daresbury, Warrington WA4 4AD, U.K., 2003.
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Smith, W.; Leslie, M.; Forester, T. R. DL-POLY, v2.14; Daresbury Laboratories: Daresbury, Warrington WA4 4AD, U.K., 2003.
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24
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84906406166
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Computations have been performed using the CPMD 3.0 program, written by J. Hutter; Max-Planck-Institut für Festkörperforschung: Stuttgart, 1996.
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Computations have been performed using the CPMD 3.0 program, written by J. Hutter; Max-Planck-Institut für Festkörperforschung: Stuttgart, 1996.
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26
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A short review on [bmim][Cl] and [bmim][Br] polymorphism is contained in: Hamaguchi, H.-O.; Ozawa, R. Adv. Chem. Phys. 2005, 131, 85-104.
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A short review on [bmim][Cl] and [bmim][Br] polymorphism is contained in: Hamaguchi, H.-O.; Ozawa, R. Adv. Chem. Phys. 2005, 131, 85-104.
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37
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39
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84906363061
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The vibrational frequencies of the smallest species ((1, 0), (0, 1), (1, 1) and (2, 2)) are available as supporting information. The frequencies of all other clusters are available from the authors.
-
The vibrational frequencies of the smallest species ((1, 0), (0, 1), (1, 1) and (2, 2)) are available as supporting information. The frequencies of all other clusters are available from the authors.
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40
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84906377284
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This seemingly small cell contains, in fact, 64 [bmim][Tf] pairs, corresponding to 2112 atoms
-
This seemingly small cell contains, in fact, 64 [bmim][Tf] pairs, corresponding to 2112 atoms.
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41
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3342914021
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