-
1
-
-
0001046654
-
-
G. Reiser, W. Habenicht, K. Müller-Dethlefs, and E. W. Schlag, Chem. Phys. Lett. 152, 119 (1988).
-
(1988)
Chem. Phys. Lett.
, vol.152
, pp. 119
-
-
Reiser, G.1
Habenicht, W.2
Müller-Dethlefs, K.3
Schlag, E.W.4
-
2
-
-
85033038984
-
-
Ph.D. thesis, Würzburg University, Germany
-
B. Buhler, Ph.D. thesis, Würzburg University, Germany, 1990.
-
(1990)
-
-
Buhler, B.1
-
9
-
-
0000902334
-
-
W. G. Scherzer, H. L. Selzle, E. W. Schlag, and R. D. Levine, Phys. Rev. Lett. 72, 1435 (1994).
-
(1994)
Phys. Rev. Lett.
, vol.72
, pp. 1435
-
-
Scherzer, W.G.1
Selzle, H.L.2
Schlag, E.W.3
Levine, R.D.4
-
17
-
-
0003637009
-
-
edited by I. Powis, T. Baer, and C. Y. Ng Wiley, New York
-
E. D. Grant, in High Resolution Laser Photoionization and Photoelectron Studies, edited by I. Powis, T. Baer, and C. Y. Ng (Wiley, New York, 1995).
-
(1995)
High Resolution Laser Photoionization and Photoelectron Studies
-
-
Grant, E.D.1
-
18
-
-
85033071523
-
-
F. Merkt and T. P. Softley, in Ref. 16
-
F. Merkt and T. P. Softley, in Ref. 16.
-
-
-
-
22
-
-
36449009266
-
-
E. Rabani, R. D. Levine, A. Mühlpfordt, and E. Even, J. Chem. Phys. 102, 1619 (1995),
-
(1995)
J. Chem. Phys.
, vol.102
, pp. 1619
-
-
Rabani, E.1
Levine, R.D.2
Mühlpfordt, A.3
Even, E.4
-
29
-
-
33645802227
-
-
Ph.D. thesis, Hebrew University, Jerusalem
-
L. Y. Baranov, Ph.D. thesis, Hebrew University, Jerusalem, 1996.
-
(1996)
-
-
Baranov, L.Y.1
-
30
-
-
85033059712
-
-
note
-
27,28 and it arises because the correction to the near threshold approximation for matrix elements can and does become large compared to the leading term. When the leading term vanishes, what is nominally a correction becomes the first nonvanishing contribution.
-
-
-
-
34
-
-
85033037980
-
-
in press
-
F. Remade, R. D. Levine, E. W. Schlag, H. L. Selzle, and A. Held, J. Phys. Chem. (in press).
-
J. Phys. Chem.
-
-
Remade, F.1
Levine, R.D.2
Schlag, E.W.3
Selzle, H.L.4
Held, A.5
-
35
-
-
0001318389
-
-
C. Bordas, P. F. Brevet, M. Broyer, J. Chevaleyre, P. Labastie, and J. P. Perrot, Phys. Rev. Lett. 60, 917 (1988).
-
(1988)
Phys. Rev. Lett.
, vol.60
, pp. 917
-
-
Bordas, C.1
Brevet, P.F.2
Broyer, M.3
Chevaleyre, J.4
Labastie, P.5
Perrot, J.P.6
-
38
-
-
84913019261
-
-
C. Bordas, P. Brevet, M. Broyer, J. Chevaleyre, and P. Labastie, Europhys. Lett. 3, 789 (1987).
-
(1987)
Europhys. Lett.
, vol.3
, pp. 789
-
-
Bordas, C.1
Brevet, P.2
Broyer, M.3
Chevaleyre, J.4
Labastie, P.5
-
41
-
-
0011514016
-
-
E. Rabani, L. Y. Baranov, R. D. Levine, and U. Even, Chem. Phys. Lett. 221, 473 (1994).
-
(1994)
Chem. Phys. Lett.
, vol.221
, pp. 473
-
-
Rabani, E.1
Baranov, L.Y.2
Levine, R.D.3
Even, U.4
-
42
-
-
85033041645
-
-
But much less so for a dipolar anisotropy, cf. Ref. 27
-
But much less so for a dipolar anisotropy, cf. Ref. 27.
-
-
-
-
43
-
-
85033043468
-
-
note
-
5F (a.u.)=1. For a higher field the density of Rydberg states is essentially uniform in energy. At lower fields the density of states is "bumpy" so that a state of a given series is not necessarily almost isoenergetic with a state of another series. Note that because the field mixes l states, two quasi degenerate states can effectively interact.
-
-
-
-
54
-
-
85033054263
-
-
This is not always warranted (see Ref. 52), but is a realistic approximation when the matrix elements of QVP are only slowly varying with energy
-
This is not always warranted (see Ref. 52), but is a realistic approximation when the matrix elements of QVP are only slowly varying with energy.
-
-
-
-
58
-
-
0001107120
-
-
R. B. Bernstein, A. Dalgarno, H. Massey, and I. C. Percival, Proc. R. Soc. London Ser. A 274, 427 (1963).
-
(1963)
Proc. R. Soc. London Ser. A
, vol.274
, pp. 427
-
-
Bernstein, R.B.1
Dalgarno, A.2
Massey, H.3
Percival, I.C.4
-
61
-
-
85033060475
-
-
note
-
Explicit analytic results, following Gordon (Ref. 59) are given in Ref. 26 but the computation of the required generalized hypergeometric function is not trivial even though, for integer quantum number, the generalized hypergeometric function is a finite polynomial. The problem is that there is extensive cancellation of terms and more stable numerical methods are discussed in Ref. 27. An exception, discussed in the appendix, is when for one of the states, l=n-1.
-
-
-
-
62
-
-
0004285220
-
-
Cambridge University Press, Cambridge
-
T. F. Gallagher, Rydberg Atoms (Cambridge University Press, Cambridge, 1994).
-
(1994)
Rydberg Atoms
-
-
Gallagher, T.F.1
-
66
-
-
0000916001
-
-
M. L. Zimmerman, M. G. Littman, M. M. Kash, and D. Kleppner, Phys. Rev. A 20, 2251 (1979).
-
(1979)
Phys. Rev. A
, vol.20
, pp. 2251
-
-
Zimmerman, M.L.1
Littman, M.G.2
Kash, M.M.3
Kleppner, D.4
-
68
-
-
0001381828
-
-
A. Mühlpfordt, U. Even, E. Rabani, and R. D. Levine, Phys. Rev. A 51, 3922 (1995).
-
(1995)
Phys. Rev. A
, vol.51
, pp. 3922
-
-
Mühlpfordt, A.1
Even, U.2
Rabani, E.3
Levine, R.D.4
-
70
-
-
36449001534
-
-
M. J. Vrakking, I. Fischer, D. M. Villeneuve, and A. Stolow, J. Chem. Phys. 103, 4538 (1995).
-
(1995)
J. Chem. Phys.
, vol.103
, pp. 4538
-
-
Vrakking, M.J.1
Fischer, I.2
Villeneuve, D.M.3
Stolow, A.4
-
71
-
-
85033053319
-
-
note
-
+ (see Ref. 36) with the larger equilibrium distance. It is in close agreement with the unpublished ab initio results of Dr. F. Masnou-Seeuws. After this work was completed, Prof. U. Kaldor informed us that his ab initio computed value is 23 a.u. which is even higher than the 18 a.u. which we used.
-
-
-
-
73
-
-
0000573224
-
-
for a classical interpretation and F. Benvenuto, G. Casati, and D. L. Shepelyansky, Phys. Rev. Lett. 72, 1818 (1994) for a strictly quantal localization. The second bottleneck discussed here is the bottleneck discussed in Refs. 19 and 54 and is similar to the bottleneck discussed by M. Bixon and J. Jortner in the preprint "The Dynamics of Predissociating High Rydberg States of NO."
-
(1994)
Phys. Rev. Lett.
, vol.72
, pp. 1818
-
-
Benvenuto, F.1
Casati, G.2
Shepelyansky, D.L.3
-
76
-
-
85033052449
-
-
note
-
2l+1 from the one that we are using here.
-
-
-
|