Abstract

In this paper we examine analytically the large-N gap equation and its solution for the 2D ℂℙN −1 sigma model defined on a Euclidean spacetime torus of arbitrary shape and size (L, β), β being the inverse temperature. We find that the system has a unique homogeneous phase, with the ℂℙN −1 fields ni acquiring a dynamically generated mass (λ) ≥ Λ2 (analogous to the mass gap of SU(N ) Yang-Mills theory in 4D), for any β and L. Several related topics in the recent literature are discussed. One concerns the possibility, which turns out to be excluded according to our analysis, of a “Higgs-like” — or deconfinement — phase at small L and at zero temperature. Another topics involves “soliton-like” (inhomogeneous) solutions of the generalized gap equation, which we do not find. A related question concerns a possible instability of the standard ℂℙN −1 vacuum on R2, which is shown not to occur. In all cases, the difference in the conclusions can be traced to the existence of certain zeromodes and their proper treatment. The ℂℙN −1 model with twisted boundary conditions is also analyzed. The θ dependence and different limits involving N , β and L are briefly discussed.

Highlights

  • Be related to some physical phenomena in condensed matter physics such as quantum Hall effects [22,23,24,25,26]

  • In this paper we examine analytically the large-N gap equation and its solution for the 2D CPN−1 sigma model defined on a Euclidean spacetime torus of arbitrary shape and size (L, β), β being the inverse temperature

  • We find that the two dimensional CPN−1 sigma models defined with doubly periodic conditions, possesses a unique ground state for any L and β, which goes over, in the L → ∞ and at zero temperature (β → ∞) limit, smoothly to the well-known vacuum with mass generation, and with no global SU(N ) symmetry breaking

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Summary

Small size and low temperatures

At low-temperatures T Λ, the pseudo free energy is obtained from eq (2.9) with aμ = 0 as. In the calculation of the constant and linear terms, the regularization turns out to be crucial and we have used. The gap equation for small λL is given by 0 = ∂Fλ = N L ∂λ 4π. 2(N − 1) 2N degrees of freedom which, due to asymptotic freedom, behave as if they were massless fields. This agrees with the result obtained by Shifman et al [32] strictly at

High temperature and large size
Absence of soliton-like solutions
Uniqueness of the saddle point on the real axis
Maximization of the free energy
Twisted boundary conditions
Concluding remarks
A The coupling constant
B Pauli-Villars regularization
C Poisson summation formula
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