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[13] pointed out that in fact the series of the dipole resonances terminate because of the lifting of the hydrogen degeneracy caused by the relativistic splitting. A related comment is given in our Sec. IV
-
M. Gailitis and R. Damburg [13] pointed out that in fact the series of the dipole resonances terminate because of the lifting of the hydrogen degeneracy caused by the relativistic splitting. A related comment is given in our Sec. IV.
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Damburg, R.2
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M. Halka, H. C. Bryant, E. P. Mackerrow, W. Miller, A. H. Mohagheghi, C. Y. Tang, S. Cohen, J. B. Donahue, A. Hsu, C. R. Quick, J. Tiee, and K. Rozsa, Phys. Rev. A 44, 6127 (1991).
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Cohen, S.7
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0 resonances have been predicted, e.g., between n = 4 and 7, by J. Z. Tang and I. Shimamura, Phys. Rev. A 51, R1738 (1995). This paper pays attention to the Wannier states up to the n = 7 threshold. Such results were obtained much earlier by C. A. Nicolaides and Y. Komninos, [ibid. 35, 999 (1987)] for the Wannier states up to the n =10 threshold.
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53
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0 resonances have been predicted, e.g., between n = 4 and 7, by J. Z. Tang and I. Shimamura, Phys. Rev. A 51, R1738 (1995). This paper pays attention to the Wannier states up to the n = 7 threshold. Such results were obtained much earlier by C. A. Nicolaides and Y. Komninos, [ibid. 35, 999 (1987)] for the Wannier states up to the n =10 threshold.
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85015721017
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note
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The use of unoptimized bound hydrogenic functions in a single diagonalization without the contribution of the open channels cannot establish the correspondence of a root with a resonance state.
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C. A. Nicolaides and D. R. Beck, Phys. Lett. 65A, 11 (1978); C. A. Nicolaides, H. J. Gotsis, M. Chrysos, and Y. Komninos, Chem. Phys. Lett. 168, 570 (1990).
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100
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0000887720
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H. C. Bryant, D. A. Clark, K. B. Butterfield, C. A. Frost, H. Sharifian, H. Tootoonchi, J. B. Donahue, P. A. M. Gram, M. E. Hamm, R. W. Hamm, J. C. Pratt, M. A. Yates, and W. W. Smith, Phys. Rev. A 27, 2889 (1983).
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Donahue, J.B.7
Gram, P.A.M.8
Hamm, M.E.9
Hamm, R.W.10
Pratt, J.C.11
Yates, M.A.12
Smith, W.W.13
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101
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0001478183
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M. Halka, H. C. Bryant, C. Johnstone, B. Marchini, W. Miller, A. H. Mohagheghi, C. Y. Tang, K. B. Butterfield, D. A. Clark, S. Cohen, J. B. Donahue, P. A. M. Gram, R. W. Hamm, A. Hsu, D. W. MacArthur, E. P. MacKerrow, C. R. Quick, J. Tiee, and K. Rózsa, Phys. Rev. A 46, 6942 (1992).
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Halka, M.1
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Johnstone, C.3
Marchini, B.4
Miller, W.5
Mohagheghi, A.H.6
Tang, C.Y.7
Butterfield, K.B.8
Clark, D.A.9
Cohen, S.10
Donahue, J.B.11
Gram, P.A.M.12
Hamm, R.W.13
Hsu, A.14
MacArthur, D.W.15
MacKerrow, E.P.16
Quick, C.R.17
Tiee, J.18
Rózsa, K.19
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103
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85015726476
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Tables containing the wave-function characteristics for all the states under consideration can be obtained from ftp://ftp.phys.uni.torun.pl/pub/publications/ifiz/mirekb/H_/tab_I.ps.
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