-
4
-
-
0000423373
-
-
P. E. Parris, M. Kuś, D. H. Dunlap, and V. M. Kenkre, Phys. Rev. E 56, 5295 (1997).PLEEE8
-
(1997)
Phys. Rev. E
, vol.56
, pp. 5295
-
-
Parris, P.E.1
Kuś, M.2
Dunlap, D.H.3
Kenkre, V.M.4
-
14
-
-
0031386041
-
-
P. E. Parris, D. H. Dunlap, and V. M. Kenkre, J. Polym. Sci., Part B: Polym. Phys. 35, 2803 (1997).JPBPEM
-
(1997)
J. Polym. Sci., Part B: Polym. Phys.
, vol.35
, pp. 2803
-
-
Parris, P.E.1
Dunlap, D.H.2
Kenkre, V.M.3
-
16
-
-
33746331761
-
-
M. Lax, Phys. Rev. 109, 1921 (1958).PHRVAO
-
(1958)
Phys. Rev.
, vol.109
, pp. 1921
-
-
Lax, M.1
-
17
-
-
85036398489
-
-
See, e.g., Katja Lindenberg and Bruce J. West, The Nonequilibrium Statistical Mechanics of Open and Closed Systems (VCH, New York, 1990), p. 42
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See, e.g., Katja Lindenberg and Bruce J. West, The Nonequilibrium Statistical Mechanics of Open and Closed Systems (VCH, New York, 1990), p. 42.
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33746286993
-
-
S. A. Visser, J. A. Sinicropi, E. H. Magin, and P. M. Borsenberger, Proc. SPIE 3144, 110 (1987)
-
(1987)
Proc. SPIE
, vol.3144
, pp. 110
-
-
Visser, S.A.1
Sinicropi, J.A.2
Magin, E.H.3
Borsenberger, P.M.4
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21
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85036202828
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For simplicity, we assume that there is a single extremum. The analysis should be repeated for additional extrema if present
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For simplicity, we assume that there is a single extremum. The analysis should be repeated for additional extrema if present.
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85036394436
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As another example of the general asymptotic formula, we mention the rectangular pulse density function which results in Eq. (5.7) for the correlation function. Application of Eq. (6.3) gives the transcendental equation [Formula Presented]whose solution [Formula Presented] has to be obtained numerically. It is trivial, however, to calculate the mobility for any parameter values through a computer algorithm which first solves the above equation and substitutes the solution in Eq. (6.8) to obtain the mobility
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As another example of the general asymptotic formula, we mention the rectangular pulse density function which results in Eq. (5.7) for the correlation function. Application of Eq. (6.3) gives the transcendental equation (ym/σ)2wqEkT+e-(s+w)ym[1+(s+w)ym]-e-sym(1+sym)=0,whose solution ym has to be obtained numerically. It is trivial, however, to calculate the mobility for any parameter values through a computer algorithm which first solves the above equation and substitutes the solution in Eq. (6.8) to obtain the mobility.
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85036233084
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See, e.g., J. M. Ziman, Principles of the Theory of Solids (Cambridge University Press, Cambridge, 1979), p. 215
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See, e.g., J. M. Ziman, Principles of the Theory of Solids (Cambridge University Press, Cambridge, 1979), p. 215.
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