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It should be noted that the large number of molecules within 5 Å of the pore surface is due primarily to two factors: the space available (which increases as 2πr moving away from the pore axis) and attractive interactions with the surface. This number, however, and the populations plotted in Figure 4 (the radial density is not shown) should not be interpreted to mean that the pore interior is vacated. On the contrary, it is similar in density to the bulk liquid
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It should be noted that the large number of molecules within 5 Å of the pore surface is due primarily to two factors: the space available (which increases as 2πr moving away from the pore axis) and attractive interactions with the surface. This number, however, and the populations plotted in Figure 4 (the radial density is not shown) should not be interpreted to mean that the pore interior is vacated. On the contrary, it is similar in density to the bulk liquid.
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The optical Kerr effect measurements measure collective orienta-tional reorientation as opposed to our calculations based on individual molecules. Moreover, they are related to C2(t, 〈P2[e(0) ·e(t)]〉 rather than the Crot(t) in eq 13 which is presented in Figure 12. Our simulations also give a triexponential decay for C2(t) with time constants of ∼0.3, 3.3, and 52 ps
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2(t) with time constants of ∼0.3, 3.3, and 52 ps.
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