-
2
-
-
3543071519
-
-
A.S. Parkins, P. Marte, P. Zoller, and H.J. Kimble, Phys. Rev. Lett. 71, 3095 (1993)
-
(1993)
Phys. Rev. Lett.
, vol.71
, pp. 3095
-
-
Parkins, A.S.1
Marte, P.2
Zoller, P.3
Kimble, H.J.4
-
3
-
-
13444296350
-
-
A.S. Parkins, P. Marte, P. Zoller, O. Carnal, and H.J. Kimble, Phys. Rev. A 51, 1578 (1995).
-
(1995)
Phys. Rev. A
, vol.51
, pp. 1578
-
-
Parkins, A.S.1
Marte, P.2
Zoller, P.3
Carnal, O.4
Kimble, H.J.5
-
4
-
-
0027927309
-
-
B.M. Garraway, B. Sherman, H. Moya-Cessa, P.L. Knight, and G. Kurizki, Phys. Rev. A 49, 535 (1994).
-
(1994)
Phys. Rev. A
, vol.49
, pp. 535
-
-
Garraway, B.M.1
Sherman, B.2
Moya-Cessa, H.3
Knight, P.L.4
Kurizki, G.5
-
6
-
-
3843151527
-
-
D.M. Meekhof, C. Monroe, B.E. King, W.M. Itano, and D.J. Wineland, Phys. Rev. Lett. 76, 1796 (1996).
-
(1996)
Phys. Rev. Lett.
, vol.76
, pp. 1796
-
-
Meekhof, D.M.1
Monroe, C.2
King, B.E.3
Itano, W.M.4
Wineland, D.J.5
-
7
-
-
0342860967
-
-
C. Monroe, D.M. Meekhof, B.E. King, and D.J. Wineland, Science 272, 1131 (1996).
-
(1996)
Science
, vol.272
, pp. 1131
-
-
Monroe, C.1
Meekhof, D.M.2
King, B.E.3
Wineland, D.J.4
-
14
-
-
35949006753
-
-
Phys. Rev. AJ. Janszky, P. Domokos, S. Szabó, and P. Adam, 51, 4191 (1995)
-
(1995)
, vol.51
, pp. 4191
-
-
Janszky, J.1
Domokos, P.2
Szabó, S.3
Adam, P.4
-
15
-
-
2142720373
-
-
Phys. Rev. AS. Szabó, P. Adam, J. Janszky, and P. Domokos, 53, 2698 (1996)
-
(1996)
, vol.53
, pp. 2698
-
-
Szabó, S.1
Adam, P.2
Janszky, J.3
Domokos, P.4
-
23
-
-
85037244019
-
-
The integrals that have to be calculated in Eq. (8) read (Formula presented) For different parities of n and ν they vanish; otherwise they can be expressed as a hypergeometric function (Formula presented) as (Formula presented)for even indices, and(Formula presented)for odd indices [cf. Eqs. (7.376.2 and 7.376.3) in I. S. Gradsh-teyn and I. M. Ryzhik, Table of Integrals, Series, and Products (Academic, New York, 1963)]
-
The integrals that have to be calculated in Eq. (8) read (Formula presented) For different parities of n and ν they vanish; otherwise they can be expressed as a hypergeometric function (Formula presented) as (Formula presented)for even indices, and(Formula presented)for odd indices [cf. Eqs. (7.376.2 and 7.376.3) in I. S. Gradsh-teyn and I. M. Ryzhik, Table of Integrals, Series, and Products (Academic, New York, 1963)].
-
-
-
-
27
-
-
85037189764
-
-
When driving the atom in a Raman scheme the individual phases of the two lasers are replaced by phase differences so that disturbations due to phase fluctuations can be suppressed efficiently
-
When driving the atom in a Raman scheme the individual phases of the two lasers are replaced by phase differences so that disturbations due to phase fluctuations can be suppressed efficiently.
-
-
-
|