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1
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0000433883
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A. F. Andreev, Zh. Eksp. Teor. Fiz. 46, 1823 (1964) [Sov. Phys. JETP 19, 1228 (1964)].
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(1964)
Sov. Phys. JETP
, vol.19
, pp. 1228
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-
Andreev, A.F.1
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7
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0000640071
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-
The BTK conductance for an orifice of radius a separating bulk S and N reservoirs is (Formula presented) A and B are the Andreev and normal reflection probabilities, f is the Fermi function, Z is proportional to the barrier height, Γ is the inelastic scattering rate, and (Formula presented) is the single spin density of states at the Fermi level. See Ref. 2 and Pleceník, M. Grajcar, Š. Benačka, P. Seidel, and A. Pfuch, Phys. Rev. B 49, 10 016 (1994);
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(1994)
Phys. Rev. B
, vol.49
, pp. 10 016
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Grajcar, M.1
Benačka, B.2
Seidel, P.3
Pfuch, A.4
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11
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85037909235
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The BTK transmission coefficient is (Formula presented) (see Ref. 2
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The BTK transmission coefficient is (Formula presented) (see Ref. 2).
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12
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0001657711
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Zh. Eksp. Teor. Fiz. 48, 984 (1965)
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Yu. V. Sharvin, Zh. Eksp. Teor. Fiz. 48, 984 (1965) [Sov. Phys. JETP 21, 655 (1965)].
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(1965)
Sov. Phys. JETP
, vol.21
, pp. 655
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-
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13
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85037907214
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S. V. Vonsovsky, Yu. A. Izyumov, and E. Z. Kurmaev, Superconductivity of Transition Metals, Their Alloys, and Compounds (Spring-Verlag, Berlin, 1982), p. 203.
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S. V. Vonsovsky, Yu. A. Izyumov, and E. Z. Kurmaev, Superconductivity of Transition Metals, Their Alloys, and Compounds (Spring-Verlag, Berlin, 1982), p. 203.
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15
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84955024817
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H. J. Mathieu, M. Datta, and D. Landolt, J. Vac. Sci. Technol. A 3 (2), 331 (1985).
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(1985)
J. Vac. Sci. Technol. A
, vol.3
, Issue.2
, pp. 331
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Mathieu, H.J.1
Datta, M.2
Landolt, D.3
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17
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85037898799
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K. C. Liu, Ph.D. thesis, MIT, 1979, p. 51.
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K. C. Liu, Ph.D. thesis, MIT, 1979, p. 51.
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18
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85037877325
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See, for example, P. G. deGennes, Superconductivity of Metals and Alloys (Addison Wesley, New York, 1989), p. 11.
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See, for example, P. G. deGennes, Superconductivity of Metals and Alloys (Addison Wesley, New York, 1989), p. 11.
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-
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21
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85037886595
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(Formula presented) varies from 0.817 in the Sharvin limit (Formula presented) to 1.18 in the Maxwell limit (Formula presented)
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(Formula presented) varies from 0.817 in the Sharvin limit (Formula presented) to 1.18 in the Maxwell limit (Formula presented)
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-
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24
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85037874369
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see also P. S. Westbrook, Ph.D. thesis, MIT, 1998. Note that these values take into account a phonon trapping factor of 10. Our estimate of this factor comes from our own measurement of it which is described in an unpublished manuscript;
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Note that these values take into account a phonon trapping factor of 10. Our estimate of this factor comes from our own measurement of it which is described in an unpublished manuscript;see also P. S. Westbrook, Ph.D. thesis, MIT, 1998.
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