메뉴 건너뛰기




Volumn 53, Issue 6, 1996, Pages 3438-3444

Multigrid Monte Carlo method. IV. One-dimensional O(4)-symmetric nonlinear σ model

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0039366050     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.53.3438     Document Type: Article
Times cited : (5)

References (31)
  • 2
    • 33845348550 scopus 로고
    • Lattice '88, Proceedings of the International Symposium, Batavia, Illinois
    • edited by A. S. Kronfeld and P. B. Mackenzie
    • S. L. Adler, in Lattice '88, Proceedings of the International Symposium, Batavia, Illinois, edited by A. S. Kronfeld and P. B. Mackenzie [Nucl. Phys. B (Proc. Suppl.) 9, 437 (1989)].
    • (1989) Nucl. Phys. B (Proc. Suppl.) , vol.9 , pp. 437
    • Adler, S.L.1
  • 3
    • 44949289741 scopus 로고
    • Lattice '89, Proceedings of the International Symposium, Capri, Italy
    • edited by R. Petronizio, et al
    • U. Wolff, in Lattice '89, Proceedings of the International Symposium, Capri, Italy, edited by R. Petronizio, et al. [Nucl. Phys. B (Proc. Suppl.) 17, 93 (1990)].
    • (1990) Nucl. Phys. B (Proc. Suppl.) , vol.17 , pp. 93
    • Wolff, U.1
  • 4
    • 44949280154 scopus 로고
    • Lattice '90, Proceedings of the International Symposium, Tallahassee, Florida
    • edited by U. M. Heller, A. D. Kennedy, and S. Sanielevici
    • A. D. Sokal, in Lattice '90, Proceedings of the International Symposium, Tallahassee, Florida, edited by U. M. Heller, A. D. Kennedy, and S. Sanielevici [Nucl. Phys. B (Proc. Suppl.) 20, 55 (1991)].
    • (1991) Nucl. Phys. B (Proc. Suppl.) , vol.20 , pp. 55
    • Sokal, A.D.1
  • 9
    • 0011680328 scopus 로고
    • Cargèse lectures, edited by G. ‘t Hooft et al. (Plenum, New York, 1988
    • G. Mack, in Nonperturbative Quantum Field Theory, 1987 Cargèse lectures, edited by G. ‘t Hooft et al. (Plenum, New York, 1988).
    • (1987) Nonperturbative Quantum Field Theory
    • Mack, G.1
  • 22
    • 85035228760 scopus 로고    scopus 로고
    • Here, The first author is not responsible for the second author’s sordid past
    • Here “we” refers to the second author only. The first author is not responsible for the second author’s sordid past.
    • We” refers to the second author only
  • 27
    • 85035200753 scopus 로고    scopus 로고
    • Confidence level is the probability that the chi (formula presented) would equal or exceed the observed value, assuming that the underlying statistical model (“null hypothesis”) is correct
    • Confidence level is the probability that the chi (formula presented) would equal or exceed the observed value, assuming that the underlying statistical model (“null hypothesis”) is correct.
  • 28
    • 85035227970 scopus 로고    scopus 로고
    • Our preceding results suggest that we ought to use instead a logarithmic ansatz: e.g., [ τ, A (β, L) approx [ln ξ (β, L) + c (ξ (β, L) / L bbox) ] g-A bbox(ξ (β, L) / L bbox) . ] But it is difficult to know what to use for the function c (ξ (β, L) / L bbox). If one simply uses c equiv 0, the agreement is poor; clearly the additive constant cannot be neglected for our range of L, as is obvious already from Figs. reffig1 and reffig3 and Table reftab3. So we decided to use instead the power law ansatz as a reasonable “phenomenological” fit
    • Our preceding results suggest that we ought to use instead a logarithmic ansatz: e.g., [ τ, A (β, L) approx [ln ξ (β, L) + c (ξ (β, L) / L bbox) ] g-A bbox(ξ (β, L) / L bbox) . ] But it is difficult to know what to use for the function c (ξ (β, L) / L bbox). If one simply uses c equiv 0, the agreement is poor; clearly the additive constant cannot be neglected for our range of L, as is obvious already from Figs. reffig1 and reffig3 and Table reftab3. So we decided to use instead the power law ansatz as a reasonable “phenomenological” fit.
  • 29
    • 85035210082 scopus 로고    scopus 로고
    • It is of course equivalent to use the ansatz [ τ -int, A (β, L) sim (formula presented) -int, A) hat g -A bbox(ξ (β, L) / L bbox), ] and indeed the two ansätze are related by hat g (formula presented) (x). However, to determine whether lim (formula presented) hat (formula presented) (x) is nonzero, it is more convenient to inspect a graph of (formula presented) than one of hat g (formula presented)
    • It is of course equivalent to use the ansatz [ τ -int, A (β, L) sim (formula presented) -int, A) hat g -A bbox(ξ (β, L) / L bbox), ] and indeed the two ansätze are related by hat g (formula presented) (x). However, to determine whether lim (formula presented) hat (formula presented) (x) is nonzero, it is more convenient to inspect a graph of (formula presented) than one of hat g (formula presented).
  • 30
    • 85035239829 scopus 로고    scopus 로고
    • Note that, contrary to much belief, τ (formula presented) =0. For further discussion, see cite1,4
    • Note that, contrary to much belief, τ (formula presented) =0. For further discussion, see cite1,4.
  • 31
    • 85035244749 scopus 로고    scopus 로고
    • All three criteria translate, in different ways, the intuitive idea of using the largest t such that the signal to noise ratio is “not too small.” In particular, criterion (c) comes from the fact that the statistical error bar on ρ (formula presented) (t) is roughly of order [τ (formula presented): see cite1,23,24,25
    • All three criteria translate, in different ways, the intuitive idea of using the largest t such that the signal to noise ratio is “not too small.” In particular, criterion (c) comes from the fact that the statistical error bar on ρ (formula presented) (t) is roughly of order [τ (formula presented): see cite1,23,24,25.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.