-
3
-
-
0000004829
-
-
VAN ALBADA M. P. and LAGENDIJK A., Phys. Rev. Lett., 55 (1985) 2692; WOLF P.-E. and MARET G., Phys. Rev. Lett., 55 (1985) 2696.
-
(1985)
Phys. Rev. Lett.
, vol.55
, pp. 2696
-
-
Wolf, P.-E.1
Maret, G.2
-
4
-
-
4243320784
-
-
BAYER G. and NIEDERDRÄNK T., Phys. Rev. Lett., 70 (1993) 3884; TOURIN A., DERODE A., ROUX P., VAN TIGGELEN B. A. and FINK M., Phys. Rev. Lett., 79 (1997) 3637.
-
(1993)
Phys. Rev. Lett.
, vol.70
, pp. 3884
-
-
Bayer, G.1
Niederdränk, T.2
-
5
-
-
0000177573
-
-
BAYER G. and NIEDERDRÄNK T., Phys. Rev. Lett., 70 (1993) 3884; TOURIN A., DERODE A., ROUX P., VAN TIGGELEN B. A. and FINK M., Phys. Rev. Lett., 79 (1997) 3637.
-
(1997)
Phys. Rev. Lett.
, vol.79
, pp. 3637
-
-
Tourin, A.1
Derode, A.2
Roux, P.3
Van Tiggelen, B.A.4
Fink, M.5
-
6
-
-
0000184236
-
-
LABEYRIE G., DE TOMASI F., BERNARD J.-C., MÜLLER C. A., MINIATURA C. and KAISER R., Phys. Rev. Lett., 83 (1999) 5266.
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 5266
-
-
Labeyrie, G.1
De Tomasi, F.2
Bernard, J.-C.3
Müller, C.A.4
Miniatura, C.5
Kaiser, R.6
-
7
-
-
0000613407
-
-
WIERSMA D. S., VAN ALBADA M. P., VAN TIGGELEN B. A. and LAGENDIJK A., Phys. Rev. Lett., 74 (1995) 4193.
-
(1995)
Phys. Rev. Lett.
, vol.74
, pp. 4193
-
-
Wiersma, D.S.1
Van Albada, M.P.2
Van Tiggelen, B.A.3
Lagendijk, A.4
-
8
-
-
0001762391
-
-
GENACK A. Z., SEBBAH P., STOYTCHEV M. and VAN TIGGELEN B. A., Phys. Rev. Lett., 82 (1999) 715.
-
(1999)
Phys. Rev. Lett.
, vol.82
, pp. 715
-
-
Genack, A.Z.1
Sebbah, P.2
Stoytchev, M.3
Van Tiggelen, B.A.4
-
9
-
-
0000969911
-
-
VAN TIGGELEN B. A., SEBBAH P., STOYTCHEV M. and GENACK A. Z., Phys. Rev. E, 59 (1999) 7166.
-
(1999)
Phys. Rev. E
, vol.59
, pp. 7166
-
-
Van Tiggelen, B.A.1
Sebbah, P.2
Stoytchev, M.3
Genack, A.Z.4
-
10
-
-
0000583178
-
-
BOLTON-HEATON C. J., LAMBERT C. J., FAL'KO V. I., PRIGODIN V. and EPSTEIN A. J., Phys. Rev. B, 60 (1999) 10569.
-
(1999)
Phys. Rev. B
, vol.60
, pp. 10569
-
-
Bolton-Heaton, C.J.1
Lambert, C.J.2
Fal'ko, V.I.3
Prigodin, V.4
Epstein, A.J.5
-
17
-
-
0001712510
-
-
note
-
The numerical coefficients are given by Ql/L = 4/5π, 3/10 and φ̄′c/L = π/3, 4/3 for two-, three-dimensional scattering. (Reference [7] gives a different result for Q.) These expressions are valid up to corrections of order l/L. More accurate formulas that account for these ballistic corrections are given in eq. (18).
-
-
-
-
19
-
-
0033893533
-
-
SCHOMERUS H., FRAHM K. M., PATRA M. and BEENAKKER C. W. J., Physica A, 278 (2000) 469.
-
(2000)
Physica A
, vol.278
, pp. 469
-
-
Schomerus, H.1
Frahm, K.M.2
Patra, M.3
Beenakker, C.W.J.4
-
20
-
-
0000674797
-
-
BARANGER H. U., DIVINCENZO D. P., JALABERT R. A. and STONE A. D., Phys. Rev. B, 44 (1991) 10637.
-
(1991)
Phys. Rev. B
, vol.44
, pp. 10637
-
-
Baranger, H.U.1
DiVincenzo, D.P.2
Jalabert, R.A.3
Stone, A.D.4
-
21
-
-
0001839109
-
-
note
-
2l/4c = 34.5a/c for two-dimensional scattering, as a consequence of the anisotropic dispersion relation on a square lattice.
-
-
-
|