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note
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In this case the Padé-Borel resummation based on the [(l - 1)/1] Padé approximant for the Borel transform is recovered.
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41
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43
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0000434658
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Up to script O sign(ε) we recover the result of C. Jayaprakash and H. J. Katz, Phys. Rev. B 16, 3987 (1977), the √ε term is twice as large as in B. N. Shalaev, Zh. Éksp. Teor. Fiz. 73, 2301 (1977) [Sov. Phys. JETP 46, 1204 (1977)].
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44
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0000434658
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Up to script O sign(ε) we recover the result of C. Jayaprakash and H. J. Katz, Phys. Rev. B 16, 3987 (1977), the √ε term is twice as large as in B. N. Shalaev, Zh. Éksp. Teor. Fiz. 73, 2301 (1977) [Sov. Phys. JETP 46, 1204 (1977)].
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Zh. Éksp. Teor. Fiz.
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Shalaev, B.N.1
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45
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0000434658
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Up to script O sign(ε) we recover the result of C. Jayaprakash and H. J. Katz, Phys. Rev. B 16, 3987 (1977), the √ε term is twice as large as in B. N. Shalaev, Zh. Éksp. Teor. Fiz. 73, 2301 (1977) [Sov. Phys. JETP 46, 1204 (1977)].
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Sov. Phys. JETP
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