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Large-$N$ expansion and $\theta$-dependence of $2d$ $CP^{N-1}$ models beyond the leading order
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abstract
We investigate the $\theta$-dependence of 2-dimensional $CP^{N-1}$ models in the large-$N$ limit by lattice simulations. Thanks to a recent algorithm proposed by M. Hasenbusch to improve the critical slowing down of topological modes, combined with simulations at imaginary values of $\theta$, we manage to determine the vacuum energy density up the sixth order in $\theta$ and up to $N = 51$. Our results support analytic predictions, which are known up to the next-to-leading term in $1/N$ for the quadratic term in $\theta$ (topological susceptibility), and up to the leading term for the quartic coefficient $b_2$. Moreover, we give a numerical estimate of further terms in the $1/N$ expansion for both quantities, pointing out that the $1/N$ convergence for the $\theta$-dependence of this class of models is particularly slow.
Forward citations
Cited by 2 Pith papers
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Evidence of a CP broken deconfined phase in 4D SU(2) Yang-Mills theory at $\theta =\pi$ from imaginary $\theta$ simulations
Lattice simulations with analytic continuation suggest that SU(2) Yang-Mills has a deconfined phase with spontaneously broken CP symmetry at theta=pi.
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The imaginary-$\theta$ dependence of the SU($N$) spectrum
The theta-squared curvature of the SU(3) glueball mass and string tension is measured in the continuum, and the N=3 and N=6 data support the expected large-N 1/N^2 scaling.
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