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Volumn 67, Issue 2, 2003, Pages

Mass gap and vacuum energy of the Gross-Neveu model via the 2-point-particle-irreducible expansion

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE; CALCULATION; CHIRALITY; ENERGY; MASS; MATHEMATICAL ANALYSIS; REDUCTION; RELIABILITY; TEMPERATURE DEPENDENCE; VACUUM;

EID: 0037438286     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.67.025011     Document Type: Article
Times cited : (4)

References (29)
  • 3
    • 85038329156 scopus 로고    scopus 로고
    • Al. B. Zamolodchikov (unpublished); see Ref. 5
    • Al. B. Zamolodchikov (unpublished); see Ref. 5.
  • 5
    • 0001681908 scopus 로고    scopus 로고
    • C. Arvanitis, F. Geniet, M. Iacomi, J.-L. Kneur, and A. Neveu, Int. J. Mod. Phys. A 12, 3307 (1997)
    • C. Arvanitis, F. Geniet, M. Iacomi, J.-L. Kneur, and A. Neveu, Int. J. Mod. Phys. A 12, 3307 (1997).
  • 20
    • 85038292337 scopus 로고    scopus 로고
    • At 1 loop 2PPI order, there is no mass renormalization, hence (Formula presented) is the physical mass
    • At 1 loop 2PPI order, there is no mass renormalization, hence (Formula presented) is the physical mass.
  • 21
    • 85038310199 scopus 로고    scopus 로고
    • (Formula presented) is not defined since (Formula presented) We have (Formula presented)
    • (Formula presented) is not defined since (Formula presented) We have (Formula presented)
  • 22
    • 85038336504 scopus 로고    scopus 로고
    • (Formula presented)
    • (Formula presented)
  • 23
    • 85038305062 scopus 로고    scopus 로고
    • We must add a source term, otherwise E cannot be treated as an effective potential in the usual sense
    • We must add a source term, otherwise E cannot be treated as an effective potential in the usual sense.
  • 24
    • 85038309694 scopus 로고    scopus 로고
    • Up to an irrelevant (integration) constant that can be dropped
    • Up to an irrelevant (integration) constant that can be dropped.
  • 25
    • 85038308830 scopus 로고    scopus 로고
    • We notice that (Formula presented) (Formula presented) and (Formula presented) are the same for each MRS
    • We notice that (Formula presented) (Formula presented) and (Formula presented) are the same for each MRS.
  • 26
    • 85038307572 scopus 로고    scopus 로고
    • No (Formula presented) satisfying (Formula presented) was found
    • No (Formula presented) satisfying (Formula presented) was found.
  • 27
    • 85038336704 scopus 로고    scopus 로고
    • Again, no solution for (Formula presented)
    • Again, no solution for (Formula presented)
  • 28
    • 85038334845 scopus 로고    scopus 로고
    • To be more precise, (Formula presented) and (Formula presented) The fact that the error grows fast between (Formula presented) and (Formula presented) and goes slowly to (Formula presented) for (Formula presented) makes us believe it is a rather lucky shot that the energy values are better for small N
    • To be more precise, (Formula presented) and (Formula presented) The fact that the error grows fast between (Formula presented) and (Formula presented) and goes slowly to (Formula presented) for (Formula presented) makes us believe it is a rather lucky shot that the energy values are better for small N.
  • 29
    • 85038313573 scopus 로고    scopus 로고
    • Also for (Formula presented) the error grows between (Formula presented) and (Formula presented) (Formula presented) (Formula presented), and drops slowly to 0 for (Formula presented)
    • Also for (Formula presented) the error grows between (Formula presented) and (Formula presented) (Formula presented) (Formula presented), and drops slowly to 0 for (Formula presented)


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.