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3
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0000590686
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M. Bando, T. Kugo, S. Uehara, K. Yamawaki, and T.! Yanagida, Phys. Rev. Lett. 54, 1215 (1985).
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Phys. Rev. Lett.
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Bando, M.1
Kugo, T.2
Uehara, S.3
Yamawaki, K.4
Yanagida, T.5
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6
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0000898887
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F.R. Brown, H. Chen, N.H. Christ, Z. Dong, R.D. Mawhinney,W. Shaffer, and A. Vaccarino, Phys. Rev. D 46, 5655 (1992);
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Phys. Rev. D
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Brown, F.R.1
Chen, H.2
Christ, N.H.3
Dong, Z.4
Mawhinney, R.D.5
Shaffer, W.6
Vaccarino, A.7
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7
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4243270164
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Y. Iwasaki, K. Kanaya, S. Sakai, and T. Yoshié, Phys. Rev.Lett. 69, 21 (1992);
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Iwasaki, Y.1
Kanaya, K.2
Sakai, S.3
Yoshié, T.4
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8
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0032261114
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Y. Iwasaki, K. Kanaya, S. Kaya, S. Sakai,and T. Yoshié, Prog. Theor. Phys. Suppl. 131, 415 (1998).
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Prog. Theor. Phys. Suppl.
, vol.131
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Iwasaki, Y.1
Kanaya, K.2
Kaya, S.3
Sakai, S.4
Yoshié, T.5
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12
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33744705639
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21, 1661 (1980).
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Phys. Rev. D
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-
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18
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33645956227
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B147, 448 (1979).
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(1979)
Nucl. Phys.B
, vol.B147
, pp. 448
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19
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33750646591
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Such dependences are assigned to the parameters Z2(A) a°d Zi(A). This situation is similar to that for the high energy parameters in chiral perturbation theory 15J.
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Such dependences are assigned to the parameters Z2(A) a°d Zi(A). This situation is similar to that for the high energy parameters in chiral perturbation theory [15J.
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-
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-
20
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-
85107714725
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-
2 term depend on the renormalization point p. of QCD, and that those generate a small dependence of the bare parameters of the HLS on fj.. It is reasonable to take p. to be equal to the matching scale A.
-
2 term depend on the renormalization point p. of QCD, and that those generate a small dependence of the bare parameters of the HLS on fj.. It is reasonable to take p. to be equal to the matching scale A.
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-
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22
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26144470001
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Nucl. Phys. B250, 465 (1985).
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(1985)
Nucl. Phys. B
, vol.250
, pp. 465
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-
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23
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33750647063
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The RGE for F\ for /j.
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The RGE for F\ for /j.
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-
-
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25
-
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33750675593
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Note that the existence of kinetic type p-y mixing from the j3term was needed to explain the experimental data of F(p-e+e~) 17J.
-
Note that the existence of kinetic type p-y mixing from the j3term was needed to explain the experimental data of F(p-e+e~) [17J.
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-
-
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26
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33750663415
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One might think of the matching by the Borel transformationof the correlators. However, agreement of the predicted values,especially gp, is not as remarkably good as that for the presentcase.
-
One might think of the matching by the Borel transformationof the correlators. However, agreement of the predicted values,especially gp, is not as remarkably good as that for the presentcase.
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28
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33748640053
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G. Ecker, J. Gasser, A. Pich, and E. De Rafaël, Nucl. Phys.B321, 311 (1989).
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Nucl. Phys.B
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Ecker, G.1
Gasser, J.2
Pich, A.3
De Rafaël, E.4
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29
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33750652754
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See, e.g., Ref. 17J.
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See, e.g., Ref. [17J.
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-
-
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33
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0001127121
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Prog. Theor. Phys. 73, 1541 (1985).
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(1985)
Prog. Theor. Phys.
, vol.73
, pp. 1541
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-
-
35
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0000472797
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-
Prog. Theor. Phys. 91, 801 (1994).
-
(1994)
Prog. Theor. Phys.
, vol.91
, pp. 801
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-
-
36
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33750679063
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-
The contribution from the higher derivative term is neglectedin the expression of gp;r!7 given in Eq. (6.3), i.e., gpjr_=Spd«P;0,0 = gp(0;0,0).
-
The contribution from the higher derivative term is neglectedin the expression of gp;r!7 given in Eq. (6.3), i.e., gpjr_=Spd«P;0,0) = gp(0;0,0).
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-
-
-
37
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-
33750650074
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-
The parameter choice A = //ip does not work, either.
-
The parameter choice A = //ip does not work, either.
-
-
-
-
42
-
-
33750636673
-
-
note
-
One might think that there exists a cr-tadpole contribution tothe Ä-Ä two-point function with the vertex from the secondterm of Sj£CT) in Eq. (B21). However, the vertex is exactlycanceled with the vertex from 2cr-4Jc)r-4(rCT). Thus there isno {7-tadpole contribution to the Ä-Ä two-point function.Similar cancellations occur between contributions from thefirst term of 2-4CT) and I.j'-ffitf'"'to V-V as well as toV-V.
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