Light Front Treatment of Nuclei and Deep Inelastic Scattering

  • G. A. Miller
Conference paper
Part of the Centre de Physique des Houches book series (LHWINTER, volume 8)

Abstract

A light front treatment of the nuclear wave function is developed and applied, using the mean field approximation, to infinite nuclear matter. The nuclear mesons are shown to carry about a third of the nuclear plus momentum p +; but their momentum distribution has support only at p + = 0, and the mesons do not contribute to nuclear deep inelastic scattering. This zero mode effect occurs because the meson fields are independent of space-time position.

Keywords

Convolution 

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References

  1. [1]
    Aubert J., et al., Phys. Lett. B123 (1982) 275.Google Scholar
  2. [2]
    Arneodo M., Phys. Rep. 240 (1994) 301.ADSCrossRefGoogle Scholar
  3. [3]
    Frankfurt L.L. and Strikman M.I., Phys. Rep. 160 (1988) 235.ADSCrossRefGoogle Scholar
  4. [4]
    Ericson M. and Thomas A.W., Phys. Lett. B128 (1983) 112.Google Scholar
  5. [5]
    Bickerstaff R.P., Birse M.C. and Miller G.A., Phys. Rev. Lett. 53 (1984) 2532.ADSCrossRefGoogle Scholar
  6. [6]
    Alde D.M., et al. Phys. Rev. Lett. 64 (1990) 2479.ADSCrossRefGoogle Scholar
  7. [7]
    Bertsch G.F., Frankfurt L. and Strikman M., Science 259 (1993) 773.ADSCrossRefGoogle Scholar
  8. [8]
    Miller G.A., 1997 preprint, nucl-th/9702036, submitted to Phys. Rev. C.Google Scholar
  9. [9]
    Our notation is that a four vector Aµ is defined by the plus, minus and perpendicular components as (A0 + A3, A0 ‒ A3, A) .Google Scholar
  10. [10]
    The scalar mesons are meant to represent 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.Google Scholar
  11. [11]
    Serot B.D. and Walecka J.D., Adv. Nucl. Phys. 16 (1986) 1;IU-NTC-9617, Jan. 1997 nucl-th/9701058Google Scholar
  12. [12]
    The symbol for the nucleon field operator and the mode functions of that field is taken to be the same -ψ to reduce the amount of notation.Google Scholar
  13. [13]
    Chang S-J., Root R.G. and Yan T-M., Phys. Rev. D7 (1973) 1133; ibid (1973) 1147.ADSGoogle Scholar
  14. [14]
    Yan T-M., Phys. Rev. D7 (1974) 1760; ibid (1974) 1780.Google Scholar
  15. [15]
    Glazek St. and Shakin C.M., Phys. Rev. C44 (1991) 1012.ADSGoogle Scholar
  16. [16]
    Serot B.D. and Furnstahl R.J., Phys. Rev. C43 (1991) 105.Google Scholar
  17. [17]
    Chin S.A. and Walecka J.D., Phys. Lett. B52 (1974) 24.Google Scholar
  18. [18]
    Dieperink A.E. and Miller G.A., Phys. Rev. C44 (1991) 866.ADSCrossRefGoogle Scholar

Copyright information

© Springer-Verlag Berlin Heidelberg 1998

Authors and Affiliations

  • G. A. Miller
    • 1
    • 2
    • 3
  1. 1.Department of PhysicsUniversity of WashingtonSeattleUSA
  2. 2.Stanford Linear Accelerator CenterStanford UniversityStanfordUSA
  3. 3.national Institute for Nuclear TheoryUniversity of WashingtonSeattleUSA

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