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Volumn 56, Issue 1, 1997, Pages R8-R11

Light front treatment of the nucleus: Implications for deep inelastic scattering

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0031497129     PISSN: 05562813     EISSN: 1089490X     Source Type: Journal    
DOI: 10.1103/PhysRevC.56.R8     Document Type: Article
Times cited : (22)

References (33)
  • 4
    • 85035281780 scopus 로고    scopus 로고
    • There is space to list only a few reviews. R. L. Jaffe, in Relativistic Dynamics and Quark-Nuclear Physics, edited by M. B. Johnson and A. Picklesimer
    • There is space to list only a few reviews. R. L. Jaffe, in Relativistic Dynamics and Quark-Nuclear Physics, edited by M. B. Johnson and A. Picklesimer (unpublished)
  • 14
    • 85035298966 scopus 로고    scopus 로고
    • Our notation is that a four vector (Formula presented) is defined by the plus, minus, and perpendicular components as ((Formula presented) (Formula presented)) and (Formula presented)(Formula presented)(Formula presented)(Formula presented)(Formula presented)
    • Our notation is that a four vector (Formula presented) is defined by the plus, minus, and perpendicular components as ((Formula presented) (Formula presented)) and (Formula presented)(Formula presented)(Formula presented)(Formula presented)(Formula presented)
  • 15
    • 85035292710 scopus 로고    scopus 로고
    • The use of scalar mesons is meant as a simple representation of the two pion exchange potential which causes much of the medium range attraction between nucleons, as well as the effects of a fundamental scalar meson. Thus the pion is an important implicit part of the present Lagrangian
    • The use of scalar mesons is meant as a simple representation of the two pion exchange potential which causes much of the medium range attraction between nucleons, as well as the effects of a fundamental scalar meson. Thus the pion is an important implicit part of the present Lagrangian.
  • 16
    • 0004241061 scopus 로고
    • ANUPBZ, Report IU-NTC-96-17, nucl-th/9701058, 1997
    • B. D. Serot and J. D. Walecka, Adv. Nucl. Phys. 16, 1 (1986);ANUPBZ Report IU-NTC-96-17, nucl-th/9701058, 1997.
    • (1986) Adv. Nucl. Phys. , vol.16 , pp. 1
    • Serot, B.D.1    Walecka, J.D.2
  • 18
    • 85035307357 scopus 로고
    • 7, 1147 (1973).
    • (1973) , vol.7 , pp. 1147
  • 20
    • 85035291924 scopus 로고
    • 7, 1780 (1974).
    • (1974) , vol.7 , pp. 1780
  • 24
    • 85035292402 scopus 로고    scopus 로고
    • The same symbol (Formula presented) is used for the nucleon field operator and for its mode functions
    • The same symbol (Formula presented) is used for the nucleon field operator and for its mode functions.
  • 29
    • 85035292485 scopus 로고    scopus 로고
    • Equation (15) is essentially Eq. (5.2) of Frankfurt and Strikman, Ref. 2
    • Equation (15) is essentially Eq. (5.2) of Frankfurt and Strikman, Ref. 2, with our (Formula presented) corresponding to their (Formula presented)


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.