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18
-
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85015754677
-
-
note
-
Note that very recently a generalization of the CDW-EIS, GCDW-EIS, was proposed in Ref. [19].
-
-
-
-
19
-
-
0037017320
-
-
D.S.F. Crothers, D.M. McSherry, S.F.C. O'Rourke, M.B. Shah, C. McGrath, and H.B. Gilbody, Phys. Rev. Lett. 88, 053201 (2002).
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McGrath, C.5
Gilbody, H.B.6
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20
-
-
85015791882
-
-
Q of the momentum Q that gives a factor π
-
Q of the momentum Q that gives a factor π.
-
-
-
-
21
-
-
85015799507
-
-
note
-
Within the first-order theory the target can be also ionized solely by the (single) p-n interaction provided the momentum transferred to the target nucleus is so huge (on the target scale) that the recoil velocity of the latter becomes of order of the typical electron velocity ∼1 a.u. in the target initial state. Such a "knock-out" mechanism, however, is not considered here since it would result in negligible cross sections.
-
-
-
-
22
-
-
85015737644
-
-
k
-
k.
-
-
-
-
23
-
-
85015728240
-
-
note
-
At this point we note that the role of the p-n interaction for the singly differential (in β) cross section for helium ionization by high-velocity protons and deuterons in collisions with large Q was investigated experimentally and theoretically in Refs. [24] and [15].
-
-
-
-
24
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0009489668
-
-
E.Y. Kamber, C.L. Cocke, S. Cheng, J.H. McGuire, and S.L. Varghese, J. Phys. B 21, L455 (1988); A. Salin, ibid. 22, 3901 (1989); R.E. Olson, J. Ullrich, R. Dörner, and H. Schmidt-Böcking, Phys. Rev. A 40, 2843 (1989); J. Phys. B 22, 3901 (1989); F.G. Kristensen and E. Horsdal-Pedersen, ibid. 23, 4129 (1990); X. Fang and J.F. Reading, Nucl. Instrum. Methods Phys. Res. B 53, 453 (1991); H. Fukuda, I. Shimamura, L. Vegh, and T. Watanabe, Phys. Rev. A 44, 1565 (1991); A. Gensmantel, J. Ullrich, R. Dörner, R.E. Olson, K. Ullmann, E. Forberich, S. Lencinas, and H. Schmidt-Böcking, ibid. 45, 4572 (1992); W.R. DeHaven, C. Dilley, A. Landers, E.Y. Kamber, and C.L. Cocke, ibid. 57, 292 (1998).
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25
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0001534991
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E.Y. Kamber, C.L. Cocke, S. Cheng, J.H. McGuire, and S.L. Varghese, J. Phys. B 21, L455 (1988); A. Salin, ibid. 22, 3901 (1989); R.E. Olson, J. Ullrich, R. Dörner, and H. Schmidt-Böcking, Phys. Rev. A 40, 2843 (1989); J. Phys. B 22, 3901 (1989); F.G. Kristensen and E. Horsdal-Pedersen, ibid. 23, 4129 (1990); X. Fang and J.F. Reading, Nucl. Instrum. Methods Phys. Res. B 53, 453 (1991); H. Fukuda, I. Shimamura, L. Vegh, and T. Watanabe, Phys. Rev. A 44, 1565 (1991); A. Gensmantel, J. Ullrich, R. Dörner, R.E. Olson, K. Ullmann, E. Forberich, S. Lencinas, and H. Schmidt-Böcking, ibid. 45, 4572 (1992); W.R. DeHaven, C. Dilley, A. Landers, E.Y. Kamber, and C.L. Cocke, ibid. 57, 292 (1998).
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E.Y. Kamber, C.L. Cocke, S. Cheng, J.H. McGuire, and S.L. Varghese, J. Phys. B 21, L455 (1988); A. Salin, ibid. 22, 3901 (1989); R.E. Olson, J. Ullrich, R. Dörner, and H. Schmidt-Böcking, Phys. Rev. A 40, 2843 (1989); J. Phys. B 22, 3901 (1989); F.G. Kristensen and E. Horsdal-Pedersen, ibid. 23, 4129 (1990); X. Fang and J.F. Reading, Nucl. Instrum. Methods Phys. Res. B 53, 453 (1991); H. Fukuda, I. Shimamura, L. Vegh, and T. Watanabe, Phys. Rev. A 44, 1565 (1991); A. Gensmantel, J. Ullrich, R. Dörner, R.E. Olson, K. Ullmann, E. Forberich, S. Lencinas, and H. Schmidt-Böcking, ibid. 45, 4572 (1992); W.R. DeHaven, C. Dilley, A. Landers, E.Y. Kamber, and C.L. Cocke, ibid. 57, 292 (1998).
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E.Y. Kamber, C.L. Cocke, S. Cheng, J.H. McGuire, and S.L. Varghese, J. Phys. B 21, L455 (1988); A. Salin, ibid. 22, 3901 (1989); R.E. Olson, J. Ullrich, R. Dörner, and H. Schmidt-Böcking, Phys. Rev. A 40, 2843 (1989); J. Phys. B 22, 3901 (1989); F.G. Kristensen and E. Horsdal-Pedersen, ibid. 23, 4129 (1990); X. Fang and J.F. Reading, Nucl. Instrum. Methods Phys. Res. B 53, 453 (1991); H. Fukuda, I. Shimamura, L. Vegh, and T. Watanabe, Phys. Rev. A 44, 1565 (1991); A. Gensmantel, J. Ullrich, R. Dörner, R.E. Olson, K. Ullmann, E. Forberich, S. Lencinas, and H. Schmidt-Böcking, ibid. 45, 4572 (1992); W.R. DeHaven, C. Dilley, A. Landers, E.Y. Kamber, and C.L. Cocke, ibid. 57, 292 (1998).
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E.Y. Kamber, C.L. Cocke, S. Cheng, J.H. McGuire, and S.L. Varghese, J. Phys. B 21, L455 (1988); A. Salin, ibid. 22, 3901 (1989); R.E. Olson, J. Ullrich, R. Dörner, and H. Schmidt-Böcking, Phys. Rev. A 40, 2843 (1989); J. Phys. B 22, 3901 (1989); F.G. Kristensen and E. Horsdal-Pedersen, ibid. 23, 4129 (1990); X. Fang and J.F. Reading, Nucl. Instrum. Methods Phys. Res. B 53, 453 (1991); H. Fukuda, I. Shimamura, L. Vegh, and T. Watanabe, Phys. Rev. A 44, 1565 (1991); A. Gensmantel, J. Ullrich, R. Dörner, R.E. Olson, K. Ullmann, E. Forberich, S. Lencinas, and H. Schmidt-Böcking, ibid. 45, 4572 (1992); W.R. DeHaven, C. Dilley, A. Landers, E.Y. Kamber, and C.L. Cocke, ibid. 57, 292 (1998).
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Cocke, C.L.5
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33
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85015801511
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note
-
Due to the presence of the eikonal phase in the initial state, the CDW-EIS approach also includes the "precollision" effect. In this paper the term "postcollision" denotes the total effect of both postcollision and precollision interactions.
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35
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A.B. Voitkiv, J. Phys. B 29, 5433 (1996); A.B. Voitkiv, N. Grün and W. Scheid, ibid. 32, 3923 (1999).
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85015793888
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k≤4 a.u
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k≤4 a.u.
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38
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0038419343
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R. Dörner, V. Mergel, O. Jagutzki, L. Spielberger, J. Ullrich, R. Moshammer, and H. Schmidt-Böcking, Phys. Rep. 330, 95 (2000).
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Schmidt-Böcking, H.7
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