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Volumn 60, Issue 1, 1999, Pages

Gauge independent effective potential and the Higgs boson mass bound

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EID: 17044400906     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.60.016002     Document Type: Article
Times cited : (7)

References (29)
  • 7
    • 85037231724 scopus 로고    scopus 로고
    • G. Vilkovisky, in Quantum Theory of Gravity, edited by S.M. Christensen (Hilger, Bristol, 1983)
    • Vilkovisky, G.1
  • 14
    • 0345880547 scopus 로고
    • H.C. Lee, V. Elias, G. Kunstatter, R.B. Mann, K.S. Viswanathan
    • See, for example, G. Kunstatter, in Super Field Theories, edited by H.C. Lee, V. Elias, G. Kunstatter, R.B. Mann, and K.S. Viswanathan (Plenum, New York, 1987), p. 503.
    • (1987) Super Field Theories , pp. 503
    • Kunstatter, G.1
  • 15
    • 85037199211 scopus 로고    scopus 로고
    • We should point out that the simple replacement of (Formula presented) with (Formula presented), as suggested in Ref
    • We should point out that the simple replacement of (Formula presented) with (Formula presented), as suggested in Ref. 7, is not satisfactory for calculations beyond the one-loop order. An effective action obtained by such a prescription does not generate one-particle irreducible diagrams at the higher loops. A modified construction was proposed by DeWitt in Ref. 8. However, since we are only concerned with one-loop corrections, we shall adhere to the current construction.
  • 17
    • 85037244600 scopus 로고    scopus 로고
    • Although properties of this gauge are discussed in Ref
    • Although properties of this gauge are discussed in Ref. 11, the authors of this paper used another gauge to calculate the effective potential of scalar QED.
  • 18
    • 85037182200 scopus 로고    scopus 로고
    • the current gauge, (Formula presented) since (Formula presented) vanishes. Furthermore, for ghost fields, it is the ghost propagator, rather than its inverse, that will appear in the effective action. This is due to the Grassmannian nature of ghost fields
    • In the current gauge, (Formula presented) since (Formula presented) vanishes. Furthermore, for ghost fields, it is the ghost propagator, rather than its inverse, that will appear in the effective action. This is due to the Grassmannian nature of ghost fields.
  • 19
    • 85037214732 scopus 로고    scopus 로고
    • We have suppressed the fermionic part of the gauge-fixing term. The justification of this simplified treatment is discussed in the first paper of Ref
    • We have suppressed the fermionic part of the gauge-fixing term. The justification of this simplified treatment is discussed in the first paper of Ref. 10.
  • 23
    • 0000539120 scopus 로고
    • For a review on earlier works, see M. Sher, Phys. Rep. 179, 273 (1989).
    • (1989) Phys. Rep. , vol.179 , pp. 273
    • Sher, M.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.