-
2
-
-
0037487112
-
-
edited by G. Scoles (Oxford University Press, New York)
-
S. Stolte, in Atomic and Molecular Beam Methods, edited by G. Scoles (Oxford University Press, New York, 1988), Vol. 1, p. 631.
-
(1988)
Atomic and Molecular Beam Methods
, vol.1
, pp. 631
-
-
Stolte, S.1
-
4
-
-
0001659516
-
-
H. J. Loesch and J. Remscheid, J. Chem. Phys. 93, 4779 (1990); J. Phys. Chem. 95, 8194 (1991).
-
(1991)
J. Phys. Chem.
, vol.95
, pp. 8194
-
-
-
8
-
-
0000276422
-
-
W. Kim and P. M. Felker, J. Chem. Phys. 104, 1147 (1996); 108, 6763 (1998).
-
(1998)
J. Chem. Phys.
, vol.108
, pp. 6763
-
-
-
9
-
-
0042139624
-
-
J. Sakai, C. P. Safvan, J. J. Larsen, K. M. Hilligsoe, K. Hald, and H. Stapelfeldt, J. Chem. Phys. 110, 10235 (1999).
-
(1999)
J. Chem. Phys.
, vol.110
, pp. 10235
-
-
Sakai, J.1
Safvan, C.P.2
Larsen, J.J.3
Hilligsoe, K.M.4
Hald, K.5
Stapelfeldt, H.6
-
11
-
-
4244196784
-
-
in Ref. 2
-
For a review of state selection by optical methods, see K. Bergman, in Ref. 2, p. 293.
-
Phys. Rev. Lett.
, pp. 293
-
-
Bergman, K.1
-
12
-
-
0000818870
-
-
A. F. Linskens, N. Dam, J. Reuss, and B. Sartakov, J. Chem. Phys. 101, 9384 (1994).
-
(1994)
J. Chem. Phys.
, vol.101
, pp. 9384
-
-
Linskens, A.F.1
Dam, N.2
Reuss, J.3
Sartakov, B.4
-
15
-
-
0000662212
-
-
B. Girard, N. Billy, J. Vigue, and J. C. Lehmann, Chem. Phys. Lett. 102, 168 (1983).
-
(1983)
Chem. Phys. Lett.
, vol.102
, pp. 168
-
-
Girard, B.1
Billy, N.2
Vigue, J.3
Lehmann, J.C.4
-
16
-
-
0002521931
-
-
B. Girard, G. O. Sitz, R. N. Zare, N. Billy, and J. Vigue, J. Chem. Phys. 97, 26 (1992).
-
(1992)
J. Chem. Phys.
, vol.97
, pp. 26
-
-
Girard, B.1
Sitz, G.O.2
Zare, R.N.3
Billy, N.4
Vigue, J.5
-
17
-
-
0000846822
-
-
M. A. Quesada, A. M. F. Lau, D. H. Parker, and D. W. Chandler, Phys. Rev. A 36, 4107 (1987).
-
(1987)
Phys. Rev. A
, vol.36
, pp. 4107
-
-
Quesada, M.A.1
Lau, A.M.F.2
Parker, D.H.3
Chandler, D.W.4
-
18
-
-
0028423876
-
-
S. Xu, G. Sha, B. Jiang, W. Sun, X. Chen, and C. Zhang, J. Chem. Phys. 100, 6122 (1994).
-
(1994)
J. Chem. Phys.
, vol.100
, pp. 6122
-
-
Xu, S.1
Sha, G.2
Jiang, B.3
Sun, W.4
Chen, X.5
Zhang, C.6
-
20
-
-
0000388509
-
-
A. D. Rudert, J. Martin, H. Zacharias, and J. B. Halpern, Chem. Phys. Lett. 294, 381 (1998).
-
(1998)
Chem. Phys. Lett.
, vol.294
, pp. 381
-
-
Rudert, A.D.1
Martin, J.2
Zacharias, H.3
Halpern, J.B.4
-
21
-
-
0000481674
-
-
J. Qi, G. Lazarov, X. Wang, L. Li, L. M. Narducci, A. M. Lyyra, and F. C. Spano, Phys. Rev. Lett. 83, 288 (1999).
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 288
-
-
Qi, J.1
Lazarov, G.2
Wang, X.3
Li, L.4
Narducci, L.M.5
Lyyra, A.M.6
Spano, F.C.7
-
22
-
-
4243977862
-
-
A. M. Lyyra, H. Wang, T. J. Whang, and W. C. Stwalley, Phys. Rev. Lett. 66, 2724 (1991).
-
(1991)
Phys. Rev. Lett.
, vol.66
, pp. 2724
-
-
Lyyra, A.M.1
Wang, H.2
Whang, T.J.3
Stwalley, W.C.4
-
25
-
-
0342440441
-
-
note
-
1| by 17% and 11%, respectively. Full numerical integration of Eq. (13a) reveals that these differences lead to comparable changes in the linewidths as compared to the linewidth calculated using wave vectors of uniform magnitude.
-
-
-
-
29
-
-
14344274368
-
-
U. Gaubatz, P. Rudecki, S. Schiemann, and K. Bergmann, J. Chem. Phys. 92, 5363 (1990).
-
(1990)
J. Chem. Phys.
, vol.92
, pp. 5363
-
-
Gaubatz, U.1
Rudecki, P.2
Schiemann, S.3
Bergmann, K.4
-
32
-
-
0343310006
-
-
note
-
Even for arbitrary coupling laser powers the second large terms in Eqs. (B1) and (B2) contribute little to the overall signal. In all of our calculations, these terms accounted for less than 5% to the entire signal.
-
-
-
|