-
2
-
-
0001002329
-
-
C. Cornaggia, J. Lavancier, D. Normand, J. Morellec, and H. Liu, Phys. Rev. A 42, 5464 (1990).
-
(1990)
Phys. Rev. A
, vol.42
, pp. 5464
-
-
Cornaggia, C.1
Lavancier, J.2
Normand, D.3
Morellec, J.4
Liu, H.5
-
4
-
-
4243101578
-
-
D. T. Strickland, Y. Beaudoin, P. Dietrich, and P. Corkum, Phys. Rev. Lett. 68, 2755 (1992).
-
(1992)
Phys. Rev. Lett.
, vol.68
, pp. 2755
-
-
Strickland, D.T.1
Beaudoin, Y.2
Dietrich, P.3
Corkum, P.4
-
6
-
-
0000333026
-
-
F. Ilkov, T. D. G. Walsh, S. Turgeon, and S. L. Chin, Phys. Rev. A 51, 2695 (1995).
-
(1995)
Phys. Rev. A
, vol.51
, pp. 2695
-
-
Ilkov, F.1
Walsh, T.D.G.2
Turgeon, S.3
Chin, S.L.4
-
11
-
-
25944476161
-
-
A. Zavriyev, P. H. Bucksbaum, H. G. Muller, and D. W. Schumacher, Phys. Rev. A 42, 5500 (1990).
-
(1990)
Phys. Rev. A
, vol.42
, pp. 5500
-
-
Zavriyev, A.1
Bucksbaum, P.H.2
Muller, H.G.3
Schumacher, D.W.4
-
12
-
-
0010302969
-
-
B. Yang, M. Saed, L. F. Di Mauro, A. Zavriyev, and P. H. Bucksbaum, Phys. Rev. A 44, 1033 (1991).
-
(1991)
Phys. Rev. A
, vol.44
, pp. 1033
-
-
Yang, B.1
Saed, M.2
Di Mauro, L.F.3
Zavriyev, A.4
Bucksbaum, P.H.5
-
13
-
-
5844376333
-
-
A. Giusti-Suzor, X. He, O. Atabek, and F. H. Mies, Phys. Rev. Lett. 64, 515 (1990).
-
(1990)
Phys. Rev. Lett.
, vol.64
, pp. 515
-
-
Giusti-Suzor, A.1
He, X.2
Atabek, O.3
Mies, F.H.4
-
15
-
-
0038088669
-
-
H. Abou-Rachid, T. Nguyen-Dang, R. Chaudhury, and X. He, J. Chem. Phys. 97, 5497 (1992).
-
(1992)
J. Chem. Phys.
, vol.97
, pp. 5497
-
-
Abou-Rachid, H.1
Nguyen-Dang, T.2
Chaudhury, R.3
He, X.4
-
25
-
-
0142196447
-
-
T. T. Nguyen-Dang, F. Châteauneuf, O. Atabek, and X. He, Phys. Rev. A 51, 1387 (1995).
-
(1995)
Phys. Rev. A
, vol.51
, pp. 1387
-
-
Nguyen-Dang, T.T.1
Châteauneuf, F.2
Atabek, O.3
He, X.4
-
28
-
-
85034292894
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note
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That no special dynamical effect is introduced by the 12 fs-FWHM turn-off part of (Latin small letter esh sign) is well demonstrated by the convergence of the time-dependent kinetic energy spectra of Fig. 3 toward the final spectrum (which is taken after the pulse is over), of Fig. 2. It is thus expected that with a longer turn-off, as is typical of experimentally achievable pulses, the dynamical situations described below will remain entirely valid.
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33
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85034297382
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note
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Per fragments, the experimental kinetic energy spectra cover the range 0.6-1.5 eV. The relative kinetic energy of the dissociated molecular ion is twice that of a fragment.
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34
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85034285403
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note
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0 [note the difference in scale on the ordinate axes of panels (a) and (b)].
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35
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85034283051
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note
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g〉 manifold.
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36
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85034274576
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note
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± + pℏω lies within the designated zone. Thus, any pair of Floquet levels in a given Brillouin zone is separated by a distance which can never exceed twice the photon energy.
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38
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85034296005
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note
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-3 a.u. This displacement is due to the fact that, in the same zone where the state k = 0 has previously been identified (corresponding to some given n in the zeroth-order notation |v=0,n〉), it is the dressed state v=1,n - 2〉 and not |v=1,n〉 which represents this k = 1 resonance in zeroth order. Likewise, the abscissae of the subsequent panels of Fig. 12 have been shifted by 2mℏω to correctly position newly identified resonances with respect to the k = 0 Floquet states.
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39
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2842515744
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U. Fano, Phys. Rev. 124, 1866 (1961).
-
(1961)
Phys. Rev.
, vol.124
, pp. 1866
-
-
Fano, U.1
-
40
-
-
0001316761
-
-
T. T. Nguyen-Dang, F. Châteauneuf, S. Manoli, O. Atabek, and A. Keller, Phys. Rev. A 56, 2142 (1997).
-
(1997)
Phys. Rev. A
, vol.56
, pp. 2142
-
-
Nguyen-Dang, T.T.1
Châteauneuf, F.2
Manoli, S.3
Atabek, O.4
Keller, A.5
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