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The large NN vector model with angular velocity

Published 31 Aug 2026 in hep-th, cond-mat.stat-mech, and cond-mat.str-el | (2608.31151v1)

Abstract: We study the free energy of the critical O(N)O(N) vector model at large NN on S<sup>1×</sup>S<sup>2S<sup>{1}\times</sup> S<sup>{2} with an angular velocity μ^\hatμ without the singlet constraint. The leading high-temperature behaviour is determined analytically both as an expansion about μ^r=0\hatμr=0 and μ^<sup>2r<sup>2=1\hatμ<sup>{2}r<sup>{2}=1 where rr is the radius of the sphere. We supplement the analytic results with a numerical analysis that agrees with both the analytical expansions in their respective regimes and smoothly interpolates between them. The leading high-temperature contribution to the free energy develops a pole at μ^<sup>2r<sup>2=1\hatμ<sup>{2}r<sup>{2}=1, in agreement with expectations from the thermal effective field theory. Its residue coincides with that of the massless free theory. Sub-leading terms, however, exhibit non-analytic dependence on the angular velocity and distinguish the critical fixed-point result from the free theory answer. The residue at the pole can also be obtained by placing the O(N)O(N) model on the pp-wave geometry. We show that the residue agrees with that obtained from the direct computation.

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