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Volumn 61, Issue 7, 2000, Pages 1-6

Proof of factorization for electroproduction of multiple mesons and exclusive γ*γ production of multiple hadrons

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EID: 17044429732     PISSN: 05562821     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevD.61.074010     Document Type: Article
Times cited : (41)

References (29)
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    • note
    • The number produced is, of course, limited by the quantum numbers of the initial state.
  • 7
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    • For a review of possible phenomenology of such processes see Ref. [8]
    • For a review of possible phenomenology of such processes see Ref. [8].
  • 12
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    • S. Libby and G. Sterman, Phys. Rev. D 18, 3252 (1978); 18, 4737 (1978).
    • (1978) Phys. Rev. D , vol.18 , pp. 4737
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    • G. Sterman, Phys. Rev. D 17, 2789 (1978); 17, 2773 (1978).
    • (1978) Phys. Rev. D , vol.17 , pp. 2789
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    • G. Sterman, Phys. Rev. D 17, 2789 (1978); 17, 2773 (1978).
    • (1978) Phys. Rev. D , vol.17 , pp. 2773
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    • note
    • 1,2).
  • 16
    • 33744704347 scopus 로고    scopus 로고
    • note
    • See Ref. [1] for details on the problem of transversely polarized photons in exclusive, electroproduction of vector mesons.
  • 18
    • 85104160648 scopus 로고    scopus 로고
    • note
    • 3 if the gluons connecting A to H and B to H were all scalar.
  • 19
    • 85104160485 scopus 로고    scopus 로고
    • note
    • -.
  • 22
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    • A. V. Belitsky and D. Müller, Phys. Lett. B 417, 129 (1998); Nucl. Phys. B527, 207 (1998); B537, 397 (1999).
    • (1998) Nucl. Phys. , vol.B527 , pp. 207
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    • A. V. Belitsky and D. Müller, Phys. Lett. B 417, 129 (1998); Nucl. Phys. B527, 207 (1998); B537, 397 (1999).
    • (1999) Nucl. Phys. , vol.B537 , pp. 397
  • 24
    • 33744604877 scopus 로고    scopus 로고
    • note
    • For example, the mass shell condition in deeply virtual Compton scattering or exclusive vector meson production and the fact that we chose the component of the produced mesons to be large determines the skewedness parameter to be equal to x in the above two cases. Note however, that for other final states the skewedness parameter is different from x.
  • 26
    • 33744617262 scopus 로고    scopus 로고
    • note
    • The real γ fluctuating into an initial hadronic state.
  • 27
    • 33744625227 scopus 로고    scopus 로고
    • See arguments in Sec. II E for more details
    • See arguments in Sec. II E for more details.
  • 28
    • 33744684854 scopus 로고    scopus 로고
    • See Ref. [3] for a detailed discussion on the problems associated with this particular situation
    • See Ref. [3] for a detailed discussion on the problems associated with this particular situation.
  • 29
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    • note
    • This is merely a matter of convenience, rather than necessity. One could have taken the incoming real photon to travel along the + direction and then only the labeling of the outgoing particles in Eq. (4) would change.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.