-
1
-
-
85037196952
-
-
E. Arimondo, Progress in Optics XXXV, edited by E. Wolf (North-Holland, Amsterdam, 1996), pp. 259–354
-
E. Arimondo, Progress in Optics XXXV, edited by E. Wolf (North-Holland, Amsterdam, 1996), pp. 259–354.
-
-
-
-
3
-
-
0031188367
-
-
for review of the subject, see S. E. Harris, Phys. Today 50(7), 36 (1997).
-
Phys. Today
, vol.50
, pp. 36
-
-
Harris, S.E.1
-
11
-
-
6244263472
-
-
Phys. Rev. Lett.A. S. Zibrov et al, 75, 1499 (1995).
-
(1995)
, vol.75
, pp. 1499
-
-
Zibrov, A.S.1
-
14
-
-
26744470550
-
-
K. Bergmann and B. W. Shore, in Molecular Dynamics and Spectroscopy by Stimulated Emission Pumping, edited by H. L. Dai and R. W. Field (World Scientific, Singapore, 1995), p. 315
-
J. Oreg, F. T. Hioe, and J. H. Eberly, Phys. Rev. A 29, 690 (1984);K. Bergmann and B. W. Shore, in Molecular Dynamics and Spectroscopy by Stimulated Emission Pumping, edited by H. L. Dai and R. W. Field (World Scientific, Singapore, 1995), p. 315.
-
(1984)
Phys. Rev. A
, vol.29
, pp. 690
-
-
Oreg, J.1
Hioe, F.T.2
Eberly, J.H.3
-
16
-
-
0004241917
-
-
Academic Press, New York
-
B. Young, M. Kasevich, and S. Chu, in Atom Interferometry, edited by P. Berman (Academic Press, New York, 1997), p. 363.
-
(1997)
Atom Interferometry
, pp. 363
-
-
Young, B.1
Kasevich, M.2
Chu, S.3
-
23
-
-
0000418187
-
-
Phys. Rev. Lett.M. Lukin et al, 79, 2959 (1997).
-
(1997)
, vol.79
, pp. 2959
-
-
Lukin, M.1
-
25
-
-
4243501174
-
-
We note that a careful choice of hyperfine and Zeeman sublevels should be made in order to minimize the effect of spin-exchange interaction, which preserves the total spin, e.g., Happer and Tang [Phys. Rev. Lett. 31, 273 (1973)] observed narrow (Formula presented) resonances at densities (Formula presented). These interactions as well as Doppler and collisional broadening of the optical polarizations have here been taken into account for the estimates of refractivity.
-
(1973)
Phys. Rev. Lett.
, vol.31
, pp. 273
-
-
HapperTang1
-
26
-
-
85037237045
-
-
We further note that although the atomic response of the different systems in Fig. 11 on the probe field is similar, the propagation dynamics of the other fields can differ. In particular, a dense atomic ensemble can give rise to a nonlinear generation of fields components, which can significantly modify double-dark lines
-
We further note that although the atomic response of the different systems in Fig. 11 on the probe field is similar, the propagation dynamics of the other fields can differ. In particular, a dense atomic ensemble can give rise to a nonlinear generation of fields components, which can significantly modify double-dark lines.
-
-
-
-
28
-
-
0000328947
-
-
T. Pellizzari, S. A. Gardiner, J. I. Cirac, and P. Zoller, Phys. Rev. Lett. 75, 3788 (1995).
-
(1995)
Phys. Rev. Lett.
, vol.75
, pp. 3788
-
-
Pellizzari, T.1
Gardiner, S.A.2
Cirac, J.I.3
Zoller, P.4
-
29
-
-
85037182469
-
-
M. O. Scully et al., in Proceedings of International Workshop on Coherent Control of Charge Carrier Dynamics in Semiconductors, edited by W. Potz and W. A. Schröder (Kluwer, Dordrecht, in press)
-
M. O. Scully et al., in Proceedings of International Workshop on Coherent Control of Charge Carrier Dynamics in Semiconductors, edited by W. Potz and W. A. Schröder (Kluwer, Dordrecht, in press).
-
-
-
|