1999
DOI: 10.1103/physrevd.60.094508
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Comparison of the O(3) bootstrap σ model with lattice regularization at low energies

Abstract: The renormalized coupling g R defined through the connected four-point function at zero external momentum in the nonlinear O͑3͒ sigma model in two dimensions is computed in the continuum form factor bootstrap approach with an estimated error ϳ0.3%. New high precision data are presented for g R in the latticeregularized theory with the standard action for nearly thermodynamic lattices L/ϳ7 and correlation lengths up to ϳ122 and with the fixed point action for correlation lengths up to ϳ12. The agreement between… Show more

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Cited by 37 publications
(61 citation statements)
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“…In the limit of small x we have 8) consistent with the general result (3.15) for l = 1, 2, the scalar Adler function in the leading order 1/n being just A 0 (z) = (1+M 2 /z) −2 . Note the limit is approached extremely slowly.…”
Section: The Spin Field Structure Functionssupporting
confidence: 72%
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“…In the limit of small x we have 8) consistent with the general result (3.15) for l = 1, 2, the scalar Adler function in the leading order 1/n being just A 0 (z) = (1+M 2 /z) −2 . Note the limit is approached extremely slowly.…”
Section: The Spin Field Structure Functionssupporting
confidence: 72%
“…The possible equivalence of this construction to the continuum limit of the lattice regularized theory has been investigated in ref. [8].…”
Section: O(n) Model and Structure Functionsmentioning
confidence: 99%
“…[6] an alternative was suggested which starts from the observation that the relative momentum 2p n of the two particles is also encoded in the wave function: in the symmetric channels (I = 0, 2) one should have 9) and similarly with sin p n (x − L/2) for the I = 1 channel. Here R is the "interaction range" characterized by the requirement that for a relative distance x > R the two particles propagate essentially freely.…”
Section: Phase Shiftsmentioning
confidence: 99%
“…To avoid the instability, we restrict first the correlation matrix to an M-dimensional subspace (M < N) spanned by the first M eigenvectors of C(t 0 ) with the largest eigenvalues (still stable against the statistical fluctuations) [6,37]. The generalized eigenvalue problem is then written for the new correlation matrix C(t) in this reduced basis.…”
Section: Phase Shiftsmentioning
confidence: 99%
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