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1
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S. Adachi, M. Chiba, T. Hirose, S. Nagayama, Y. Nakamitsu, T. Sato, and T. Yamada, Phys. Rev. Lett. 65, 2634 (1990).
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Adachi, S.1
Chiba, M.2
Hirose, T.3
Nagayama, S.4
Nakamitsu, Y.5
Sato, T.6
Yamada, T.7
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2
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0001347172
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H. von Busch, P. Thirolf, C. Ender, D. Habs, F. Köck, T. Schulze, and D. Schwalm, Phys. Lett. B 325, 300 (1994).
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von Busch, H.1
Thirolf, P.2
Ender, C.3
Habs, D.4
Köck, F.5
Schulze, T.6
Schwalm, D.7
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3
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5844384993
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S. Adachi, M. Chiba, T. Hirose, S. Nagayama, Y. Nakamitsu, T. Sato, and T. Yamada, Phys. Rev. A 49, 3201 (1994).
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Adachi, S.1
Chiba, M.2
Hirose, T.3
Nagayama, S.4
Nakamitsu, Y.5
Sato, T.6
Yamada, T.7
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4
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0000046229
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J. Yang, M. Chiba, R. Hamatsu, T. Hirose, T. Matsumoto, and J. Yu, Phys. Rev. A 54, 1952 (1996).
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Phys. Rev. A
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Yang, J.1
Chiba, M.2
Hamatsu, R.3
Hirose, T.4
Matsumoto, T.5
Yu, J.6
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6
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85037207312
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We use the conventions and natural units (Formula presented) (Formula presented) of J. D. Bjorken and S. D. Drell [Relativistic Quantum Mechanics (McGraw-Hill, New York, 1964)]. The symbol (Formula presented) represents the electron mass
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We use the conventions and natural units (Formula presented) (Formula presented) of J. D. Bjorken and S. D. Drell [Relativistic Quantum Mechanics (McGraw-Hill, New York, 1964)]. The symbol (Formula presented) represents the electron mass.
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9
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0242629974
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A. Billoire, R. Lacaze, A. Morel, and H. Navelet, Phys. Lett. B 78, 140(1978).
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Phys. Lett. B
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Billoire, A.1
Lacaze, R.2
Morel, A.3
Navelet, H.4
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12
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0000812225
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G. P. Lepage, P. B. Mackenzie, K. H. Streng, and P. M. Zerwas, Phys. Rev. A 28, 3090 (1983).
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Lepage, G.P.1
Mackenzie, P.B.2
Streng, K.H.3
Zerwas, P.M.4
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13
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85037244545
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S. Adachi, Bachelor thesis, Tokyo Metropolitan University, 1990 (unpublished). (This reference was obtained from
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S. Adachi, Bachelor thesis, Tokyo Metropolitan University, 1990 (unpublished). (This reference was obtained from 1.)
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17
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85037191293
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We choose to absorb a factor of (Formula presented) (where (Formula presented) is the bound-state mass) into the wave function. This leads to a different normalization for the wave function compared to
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We choose to absorb a factor of (Formula presented) (where (Formula presented) is the bound-state mass) into the wave function. This leads to a different normalization for the wave function compared to 15.
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20
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85037242870
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The wave-function factor Ψ is the integral over relative momentum (Formula presented) of a bound-state wave function (Formula presented) To lowest-order approximation, (Formula presented) can be neglected in the rest of the graph compared to the other momentum variables, for which the scale is set by the electron mass. See
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The wave-function factor Ψ is the integral over relative momentum (Formula presented) of a bound-state wave function (Formula presented) To lowest-order approximation, (Formula presented) can be neglected in the rest of the graph compared to the other momentum variables, for which the scale is set by the electron mass. See 15 and 17.
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21
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85037208648
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Konrad-Zuse-Zentrum, Berlin
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REDUCE User’s Manual 3.6, edited by A. C. Hearn and J. P. Fitch (Konrad-Zuse-Zentrum, Berlin, 1996).
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(1996)
REDUCE User’s Manual 3.6
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25
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85037193486
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P. Labelle, Ph.D. thesis, Cornell University, 1994 (unpublished)
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P. Labelle, Ph.D. thesis, Cornell University, 1994 (unpublished).
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