Anomalous temperature dependence of the magnetic field penetration depth in superconducting UBe13

See Stewart, G.R.: Rev. Mod. Phys.56, 755 (1984), and references therein

See Lee, P.A., Rice, T.M., Serene, J.W., Sham, L.J., Wilkins, J.W.: Comm. Solid State Phys. (to be published) and references therein

Ott, H.R., Rudigier, H., Rice, T.M., Ueda, K., Fisk, Z., Smith, J.L.: Phys. Rev. Lett.50, 159 (1983)

MacLaughlin, D.E., Cheng Tien, Clark, W.G., Lan, M.D., Fisk, Z., Smith, J.L., Ott, H.R.: Phys. Rev. Lett.53, 1833 (1984)

Bishop, D.J., Varma, C.M., Batlogg, B., Bucher, E.: Phys. Rev. Lett.53, 1009 (1984)

Golding, B., Bishop, D.J., Batlogg, B., Haemerle, W.H., Smith, J.L., Fisk, Z., Ott, H.R.: Phys. Rev. Lett.55, 2479 (1985)

Maple, M.B., Chen, J.W., Lambert, S.E., Fisk, Z., Smith, J.L., Ott, H.R., Brooks, J.S., Naughton, M.J.: Phys. Rev. Lett.54, 477 (1985)

Alekseevskii, N.E., Narozhnyi, V.N., Wizhankovskii, V.I., Nikolaev, E.G., Khlybov, E.P.: JETP40, 1241 (1984)

Leggett, A.J.: Phys. Rev. A140, 1869 (1965)

Andres, K., Wudl, F., Mc. Whan, D.B., Thomas, G.A., Nalewajck, D., Stevens, A.L.: Phys. Rev. Lett.45, 1449 (1980)

Tai, P.C.L., Beasley, M.R., Tinkham, M.: Phys. Rev. B11, 411 (1975)

Balian, R., Werthamer, N.R.: Phys. Rev.131, 1553 (1963)

Millis, A.: Preprint

Combescot, R.: J. Low Temp. Phys.18, 537 (1975)

Daw El Beit, M.S.: Univ. Sussex Ph.D. Thesis, 1982

Ambegaokar, V., DeGennes, P.G., Rainer, D.: Phys. Rev. A9, 2676 (1974)

For a similar calculation, see Leggett, A.J.: Rev. Mod. Phys.47, 331 (1975)

Ohkawa, F.J., Fukuyama, H.: J. Phys. Soc. Jpn.53, 4345 (1984)

Overhauser, A.W., Appel, J.: Phys. Rev. B31, 193 (1985)

Valls, O.T., Tesanovic, Z.: Phys. Rev. Lett.53, 1497 (1984)

Pfitzner, M., W�lfle, P.: Phys. Rev. B33, 2003 (1986)

Bedell, K.S., Quader, K.F.: Phys. Rev. B32, 3296 (1985). In general no simple relation betweenm */m andF 1 s can be expected to hold. In Fermi liquid theory as applied by Bedell and Quader, the ratiom */(1+F 1 s /3) defines another massm ?, which reduces to the crystalline massm only in the Galilean-invariant case. Note that in the present workm always refers to the crystalline mass, whilem * contains, in addition interaction effects

Varma, C.M.: Phys. Rev. Lett.55, 2723 (1985)

Rice, T.M., Ueda, K.: Phys. Rev. Lett.55, 995 (1985)

Ueda, K., Rice, T.M.: In: Proceedings of the 8th Taniguchi Symposium, ?Theory of Heavy Fermions and Valence Fluctuations?, Kazuya, T. (ed.), Berlin, Heidelberg, New York: Springer 1985

Abrikosov, A.A., Gor'kov, L.P.: Sov. Phys. JETP12, 1243 (1961)

Skalski, S., Betbeder-Matibet, O., Weiss, P.R.: Phys. Rev.136, A1500 (1964)

Einzel, D., Hirschfeld, P.: (to be published)

Ott, H.R., Rudigier, H., Fisk, Z., Smith, J.L.: Phys. Rev. Lett.50, 1595 (1983)

Hirschfeld, P., Vollhardt, D., W�lfle, P.: Solid State Commun.59, 111 (1986)

Schmitt-Rink, S., Miyake, K., Varma, C.M.: (to be published)