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1
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3042864659
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January
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See, for instance, the special issue of J. Opt. Soc. Am. B, 13 (1), January 1996.
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(1996)
J. Opt. Soc. Am. B
, vol.13
, Issue.1 SPEC. ISSUE
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9
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0012195553
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ZON B. A., MANAKOV N. L. and RAPOPORT L. P., Yad. Fiz., 15 (1972) 508 (Sov. J. Nucl. Phys., 15 (1972) 282).
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(1972)
Sov. J. Nucl. Phys.
, vol.15
, pp. 282
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11
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0347328164
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HOSTLER L., J. Math. Phys., 24 (1983) 2366; 28 (1987) 2984.
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(1987)
J. Math. Phys.
, vol.28
, pp. 2984
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14
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33947602873
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ZAPRYAGAEV S. A. and MANAKOV N. L., Yad. Fiz., 23 (1976) 917 (Sov. J. Nucl. Phys., 23 (1976) 482).
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(1976)
Sov. J. Nucl. Phys.
, vol.23
, pp. 482
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17
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3042864658
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LE A. T., LE V. H., KOMAROV L. I. and ROMANOVA T. S., J. Phys. B, 29 (1996) 2897.
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(1996)
J. Phys. B
, vol.29
, pp. 2897
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Le, A.T.1
Le, V.H.2
Komarov, L.I.3
Romanova, T.S.4
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19
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0012041015
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BROWN G. E., PEIERLS R. E. and WOODWARD J. B., Proc. R. Soc. London, Ser. A, 227 (1954) 51; BRENNER S., BROWN G. E. and WOODWARD J. B., Proc. R. Soc. London, Ser. A, 227 (1954) 59.
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(1954)
Proc. R. Soc. London, Ser. A
, vol.227
, pp. 51
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Brown, G.E.1
Peierls, R.E.2
Woodward, J.B.3
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20
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0344445026
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BROWN G. E., PEIERLS R. E. and WOODWARD J. B., Proc. R. Soc. London, Ser. A, 227 (1954) 51; BRENNER S., BROWN G. E. and WOODWARD J. B., Proc. R. Soc. London, Ser. A, 227 (1954) 59.
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(1954)
Proc. R. Soc. London, Ser. A
, vol.227
, pp. 59
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Brenner, S.1
Brown, G.E.2
Woodward, J.B.3
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23
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3042934849
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note
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Although it is implicitly contained in the treatment of Zapryagaev and Manakov, see ref. [13], our expression is new in the sense that the dependence in terms of Sturmian functions is made explicit.
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24
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0028480390
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RON A., GOLDBERG I. B., STEIN J., MANSON S. T., PRATT R. H. and YIN R. Y., Phys. Rev. A, 50 (1994) 1312.
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(1994)
Phys. Rev. A
, vol.50
, pp. 1312
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Ron, A.1
Goldberg, I.B.2
Stein, J.3
Manson, S.T.4
Pratt, R.H.5
Yin, R.Y.6
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25
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0013404878
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COSTESCU A., BERGSTROM P. M. jr., DINU C. and PRATT R. H., Phys. Rev. A, 50 (1994) 1390.
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(1994)
Phys. Rev. A
, vol.50
, pp. 1390
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Costescu, A.1
Bergstrom Jr., P.M.2
Dinu, C.3
Pratt, R.H.4
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26
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3042974159
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note
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Note that, for a given Z, the ratio of the results for the dipole approximation to the ones with retardation included is the same to within a fraction of a percent, for both the non-relativistic and relativistic treatments.
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