-
1
-
-
11944274056
-
-
M. H. Anderson, J. R. Ensher, M. R. Matthews, C. E. Wieman, and E. A. Cornell, Science 269, 198 (1995).
-
(1995)
Science
, vol.269
, pp. 198
-
-
Anderson, M.H.1
Ensher, J.R.2
Matthews, M.R.3
Wieman, C.E.4
Cornell, E.A.5
-
2
-
-
4243132347
-
-
C. C. Bradley, C. A. Sackett, J. J. Tollett, and R. G. Hulet, Phys. Rev. Lett. 75, 1687 (1995).
-
(1995)
Phys. Rev. Lett.
, vol.75
, pp. 1687
-
-
Bradley, C.C.1
Sackett, C.A.2
Tollett, J.J.3
Hulet, R.G.4
-
3
-
-
0000137664
-
-
M. O. Mewes, M. R. Andrews, N. J. van Druten, D. M. Kurn, D. S. Durfee, C. G. Townsend, and W. Ketterle, Phys. Rev. Lett. 77, 416 (1996);
-
(1996)
Phys. Rev. Lett.
, vol.77
, pp. 416
-
-
Mewes, M.O.1
Andrews, M.R.2
van Druten, N.J.3
Kurn, D.M.4
Durfee, D.S.5
Townsend, C.G.6
Ketterle, W.7
-
4
-
-
5344260733
-
-
Phys. Rev. Lett.M. O. MewesM. R. AndrewsN. J. van DrutenD. M. KurnD. S. DurfeeC. G. TownsendW. Ketterle77, 988 (1996).
-
(1996)
, vol.77
, pp. 988
-
-
Mewes, M.O.1
Andrews, M.R.2
van Druten, N.J.3
Kurn, D.M.4
Durfee, D.S.5
Townsend, C.G.6
Ketterle, W.7
-
7
-
-
4243124386
-
-
M. Edwards, P. A. Ruprecht, K. Burnett, R. J. Dodd, and C. W. Clark, Phys. Rev. Lett. 77, 1671 (1996).
-
(1996)
Phys. Rev. Lett.
, vol.77
, pp. 1671
-
-
Edwards, M.1
Ruprecht, P.A.2
Burnett, K.3
Dodd, R.J.4
Clark, C.W.5
-
9
-
-
85037244762
-
-
Phys. Rev. Lett
-
A. Smerzi et al, Phys. Rev. Lett. (to be published);
-
-
-
Smerzi, A.1
-
10
-
-
85037198064
-
-
S. Raghavan et al, e-print cond-mat/99706220.
-
-
-
Raghavan, S.1
-
15
-
-
85037201569
-
-
A more direct argument goes as follows. Rewrite Eq. (6) as (Formula presented), and let (Formula presented) be a solution of (Formula presented) with boundary conditions (Formula presented) (Formula presented). Identifying (Formula presented) and integrating by parts, we obtain (Formula presented). A drawback of this reasoning is that (Formula presented) is not guaranteed everywhere
-
A more direct argument goes as follows. Rewrite Eq. (6) as (Formula presented), and let (Formula presented) be a solution of (Formula presented) with boundary conditions (Formula presented) (Formula presented). Identifying (Formula presented) and integrating by parts, we obtain (Formula presented). A drawback of this reasoning is that (Formula presented) is not guaranteed everywhere.
-
-
-
-
20
-
-
0003605397
-
-
World Scientific, Singapore
-
Y. Imry, in Directions in Condensed Matter, edited by G. Grinstein and E. Mazenko (World Scientific, Singapore, 1986).
-
(1986)
Directions in Condensed Matter
-
-
Imry, Y.1
-
21
-
-
85037215443
-
-
A more accurate calculation which exactly accounts for the thermal population of all channels (but yet assumes an energy-independent mean value of (Formula presented) would replace (Formula presented) by (Formula presented)
-
A more accurate calculation which exactly accounts for the thermal population of all channels (but yet assumes an energy-independent mean value of (Formula presented) would replace (Formula presented) by (Formula presented).
-
-
-
|