메뉴 건너뛰기




Volumn 58, Issue 4, 1998, Pages

Mode regularization, time slicing, Weyl ordering, and phase space path integrals for quantum-mechanical nonlinear sigma models

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0007236644     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.58.044002     Document Type: Article
Times cited : (40)

References (22)
  • 1
    • 85039022160 scopus 로고    scopus 로고
    • For a review, see R. Rajaraman, Solitons and Instantons (North-Holland, Amsterdam 1982)
    • For a review, see R. Rajaraman, Solitons and Instantons (North-Holland, Amsterdam 1982).
  • 3
    • 0011685961 scopus 로고
    • Plenum Press, New York, K. Dietz
    • L. Alvarez-Gaumé, in Supersymmetry, edited by K. Dietz (Plenum Press, New York, 1984).
    • (1984) Supersymmetry
    • Alvarez-Gaumé, L.1
  • 6
    • 0031584006 scopus 로고    scopus 로고
    • At the one-loop level mode regularization reproduces these results, but the energy cutoff does not; see A. Rebhan and P. van Nieuwenhuizen, Nucl. Phys. B508, 449 (1997).
    • (1997) Nucl. Phys. , vol.B508 , pp. 449
    • Rebhan, A.1    van Nieuwenhuizen, P.2
  • 11
    • 36149005338 scopus 로고
    • The latter authors show that Weyl ordering of the result of the first author leads to the (Formula presented) in Eq. (3). Yang-Mills theory in the Coulomb gauge also contains a (Formula presented); see J. Schwinger, Phys. Rev. 127,324 (1962)
    • (1962) Phys. Rev. , vol.127 , pp. 324
    • Schwinger, J.1
  • 22
    • 0000985141 scopus 로고
    • C. Bernard and A. Duncan, Phys. Rev. D 11, 848 (1975). These authors verify Matthews’ theorem by a path integral approach to second order in the coupling constant. However, they assume that all factors (Formula presented) which appear in their derivation may be set equal to zero. They also study as an example the Lagrangian (Formula presented). Again they can only prove Matthews’ theorem if they set all (Formula presented) terms to zero. It would be satisfying if a path integral proof could be given without assuming that (Formula presented) is zero. Conceivably, careful discretization as well as the new ghosts of 34 are required.
    • (1975) Phys. Rev. D , vol.11 , pp. 848
    • Bernard, C.1    Duncan, A.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.