-
4
-
-
0032487270
-
-
J. Edelmann, N. Kaiser, G. Piller, and W. Weise, Nucl. Phys. A641, 119 (1998).
-
(1998)
Nucl. Phys.
, vol.A641
, pp. 119
-
-
Edelmann, J.1
Kaiser, N.2
Piller, G.3
Weise, W.4
-
13
-
-
4244014993
-
-
Jefferson Lab E94010 Collaboration, M. Amarian, Phys. Rev. Lett. 89, 242301 (2002).
-
(2002)
Phys. Rev. Lett.
, vol.89
, pp. 242301
-
-
Amarian, M.1
-
14
-
-
0035218471
-
-
B. Kubis and Ulf-G. Meißner, Nucl. Phys. A679, 698 (2001).
-
(2001)
Nucl. Phys.
, vol.A679
, pp. 698
-
-
Kubis, B.1
-
16
-
-
85039031685
-
-
A similar method was used e.g. in Refs
-
A similar method was used e.g. in Refs. 3443.
-
-
-
-
23
-
-
0001177394
-
-
M. Anselmino, B.L. Ioffe, and E. Leader, Yad. Fiz. 49, 214 (1989) [Sov. J. Nucl. Phys. 49, 136 (1989)].
-
(1989)
Sov. J. Nucl. Phys.
, vol.49
, pp. 136
-
-
Anselmino, M.1
Ioffe, B.L.2
Leader, E.3
-
25
-
-
0001189679
-
-
V. Bernard, N. Kaiser, J. Kambor, and U.-G. Meißner, Nucl. Phys. B388, 315 (1992).
-
(1992)
Nucl. Phys.
, vol.B388
, pp. 315
-
-
Bernard, V.1
Kaiser, N.2
Kambor, J.3
Meißner, U.-G.4
-
26
-
-
0001286924
-
-
N. Fettes, U.-G. Meißner, M. Mojžiš, and S. Steininger, Ann. Phys. (N.Y.) 283, 273 (2000)
-
(2000)
Ann. Phys. (N.Y.)
, vol.283
, pp. 273
-
-
Fettes, N.1
Meißner, U.-G.2
Mojžiš, M.3
Steininger, S.4
-
30
-
-
0040946661
-
-
V. Bernard, N. Kaiser, U.-G. Meißner, and A. Schmidt, Phys. Lett. B 319, 269 (1993)
-
(1993)
Phys. Lett. B
, vol.319
, pp. 269
-
-
Bernard, V.1
Kaiser, N.2
Meißner, U.-G.3
Schmidt, A.4
-
37
-
-
85039018684
-
-
We remark that in some terms of higher order we did not replace the combinations of the LECs (Formula presented) and (Formula presented) by (Formula presented) and (Formula presented) in
-
We remark that in some terms of higher order we did not replace the combinations of the LECs (Formula presented) and (Formula presented) by (Formula presented) and (Formula presented) in 9 which leads to slightly different results for the structure functions.
-
-
-
-
38
-
-
85038993044
-
-
We remark that the theoretical band based on our preliminary calculation shown in
-
We remark that the theoretical band based on our preliminary calculation shown in 13 is somewhat broader because we allowed for the delta coupling (Formula presented) which we now consider excluded.
-
-
-
-
39
-
-
85039015802
-
-
Note that one has to be careful when comparing the large mass limit from the IR calculation with the HBCHPT results. For example, the LECs used in
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Note that one has to be careful when comparing the large mass limit from the IR calculation with the HBCHPT results. For example, the LECs used in 14 do not correspond to the ones used in the HBCHPT calculation of 33 and thus a seemingly contradicting result emerges.
-
-
-
-
40
-
-
0032565502
-
-
V. Bernard, H.W. Fearing, T.R. Hemmert, and U.-G. Meißner, Nucl. Phys. A635, 121 (1998)
-
(1998)
Nucl. Phys.
, vol.A635
, pp. 121
-
-
Bernard, V.1
Fearing, H.W.2
Hemmert, T.R.3
Meißner, U.-G.4
-
42
-
-
85039012368
-
-
Note that the terms of order (Formula presented) (and higher) will be modified by two-loop corrections (but not the terms (Formula presented) and (Formula presented)
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Note that the terms of order (Formula presented) (and higher) will be modified by two-loop corrections (but not the terms (Formula presented) and (Formula presented)
-
-
-
-
48
-
-
85038998276
-
-
For fifth order calculations within HBCHPT, see
-
For fifth order calculations within HBCHPT, see 41.
-
-
-
-
51
-
-
0002107858
-
-
P. Büttiker and Ulf-G. Meißner, Nucl. Phys. A668, 97 (2000).
-
(2000)
Nucl. Phys.
, vol.A668
, pp. 97
-
-
Büttiker, P.1
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