-
1
-
-
0001020047
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-
For a collection of original papers and comments, see Vacuum Structure and QCD Sum Rules, edited by M. A. Shifman (North-Holland, Amsterdam, 1992). See also S. Narison, QCD Spectral Sum Rules (World Scientific, Singapore, 1989).
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M.A. Shifman, A.I. Vainshtein, and V.I. Zakharov, Nucl. Phys. B147, 385 (1979).For a collection of original papers and comments, see Vacuum Structure and QCD Sum Rules, edited by M. A. Shifman (North-Holland, Amsterdam, 1992).See also S. Narison, QCD Spectral Sum Rules (World Scientific, Singapore, 1989).
-
(1979)
Nucl. Phys.
, vol.B147
, pp. 385
-
-
Shifman, M.A.1
Vainshtein, A.I.2
Zakharov, V.I.3
-
11
-
-
85038279495
-
-
S. Weinberg, The Quantum Theory of Fields (Cambridge University Press, Cambridge, England, 1996), Vol. II.
-
S. Weinberg, The Quantum Theory of Fields (Cambridge University Press, Cambridge, England, 1996), Vol. II.
-
-
-
-
16
-
-
33748640053
-
-
G. Ecker, J. Gasser, A. Pich, and E. de Rafael, Nucl. Phys. B321, 311 (1989).
-
(1989)
Nucl. Phys.
, vol.B321
, pp. 311
-
-
Ecker, G.1
Gasser, J.2
Pich, A.3
de Rafael, E.4
-
17
-
-
33750649998
-
-
G. Ecker, J. Gasser, H. Leutwyler, A. Pich, and E. de Rafael, Phys. Lett. B 223, 425 (1989).
-
(1989)
Phys. Lett. B
, vol.223
, pp. 425
-
-
Ecker, G.1
Gasser, J.2
Leutwyler, H.3
Pich, A.4
de Rafael, E.5
-
20
-
-
0001889824
-
-
There is a three-gluon operator but it does not contribute to the operator product expansion for any of the correlation functions of operators built out of quark bilinears. See W. Hubschmid and S. Mallik, Nucl. Phys. 207, 29 (1982).
-
(1982)
Nucl. Phys.
, vol.207
, pp. 29
-
-
Hubschmid, W.1
Mallik, S.2
-
21
-
-
85038283773
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-
The sum rules may be improved by incorporating the contribution of the continuum from a certain threshold onwards by estimating the spectral function there from the leading operator in the operator product expansion. Also, the four-quark vacuum matrix element may be reduced to (Formula presented) by the assumption of vacuum dominance. But our point in this paper is already made on the basis of the results [Eq. (4.3)] without this improvement of the spectral side and the reduction of the operator matrix element.
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The sum rules may be improved by incorporating the contribution of the continuum from a certain threshold onwards by estimating the spectral function there from the leading operator in the operator product expansion. Also, the four-quark vacuum matrix element may be reduced to (Formula presented) by the assumption of vacuum dominance. But our point in this paper is already made on the basis of the results [Eq. (4.3)] without this improvement of the spectral side and the reduction of the operator matrix element.
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23
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0000269803
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C. Bernard, A. Duncan, J. LoSecco, and S. Weinberg, Phys. Rev. D 12, 792 (1975). See also Ref. 9.
-
(1975)
Phys. Rev. D
, vol.12
, pp. 792
-
-
Bernard, C.1
Duncan, A.2
LoSecco, J.3
Weinberg, S.4
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