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4243247178
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0000854388
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38
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47
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85037878476
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In our previous work (Ref. 26), (Formula presented) had a dip at (Formula presented) without reaching zero value. This stemmed from using (Formula presented) value rather than (Formula presented), due to numerical concerns in that computation. This is the reason for the minor discrepancy between (Formula presented) results presented here and in Ref. 26
-
In our previous work (Ref. 26), (Formula presented) had a dip at (Formula presented) without reaching zero value. This stemmed from using (Formula presented) value rather than (Formula presented), due to numerical concerns in that computation. This is the reason for the minor discrepancy between (Formula presented) results presented here and in Ref. 26.
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48
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85037901583
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The vanishing of (Formula presented) can most easily be seen by considering the ratio (Formula presented), which appears in the integrand [Eq. (3)]. At (Formula presented) the denominator tends to infinity while the numerator remains finite.
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The vanishing of (Formula presented) can most easily be seen by considering the ratio (Formula presented), which appears in the integrand [Eq. (3)]. At (Formula presented) the denominator tends to infinity while the numerator remains finite.
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51
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0039324467
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H. E. DeWitt Plenum, New York F. J. Rogers
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A. Holas, in Strongly Coupled Plasma Physics, edited by F. J. Rogers and H. E. DeWitt (Plenum, New York, 1987).
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Strongly Coupled Plasma Physics
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Holas, A.1
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0001142860
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See, for instance, N. Iwamoto, E. Krotscheck, and D. Pines, Phys. Rev. B 29, 3936 (1984).
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Phys. Rev. B
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Iwamoto, N.1
Krotscheck, E.2
Pines, D.3
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