Abstract

We study classical configurations in the ${\mathbb C}P^{N-1}$ model on ${\mathbb R}^{1}\times S^{1}$ with twisted boundary conditions. We focus on specific configurations composed of multiple fractionalized-instantons, termed "neutral bions", which are identified as "perturbative infrared renormalons" by \"{U}nsal and his collaborators. For ${\mathbb Z}_N$ twisted boundary conditions, we consider an explicit ansatz corresponding to topologically trivial configurations containing one fractionalized instanton ($\nu=1/N$) and one fractionalized anti-instanton ($\nu=-1/N$) at large separations, and exhibit the attractive interaction between the instanton constituents and how they behave at shorter separations. We show that the bosonic interaction potential between the constituents as a function of both the separation and $N$ is consistent with the standard separated-instanton calculus even from short to large separations, which indicates that the ansatz enables us to study bions and the related physics for a wide range of separations. We also propose different bion ansatze in a certain non-${\mathbb Z}_{N}$ twisted boundary condition corresponding to the "split" vacuum for $N= 3$ and its extensions for $N\geq 3$. We find that the interaction potential has qualitatively the same asymptotic behavior and $N$-dependence as those of bions for ${\mathbb Z}_{N}$ twisted boundary conditions.

Highlights

  • In order to reach deeper understanding on bions and the associated physics, it is of great importance to study examples in the low-dimensional models such as CP N−1 models [12,13,14], principal chiral models [16, 19] and quantum mechanics [15, 17, 18]

  • We show that the bosonic interaction potential between the constituents as a function of both the separation and N is consistent with the standard separated-instanton calculus even from short to large separations, which indicates that the ansatz enables us to study bions and the related physics for a wide range of separations

  • By looking into N -dependence of the interaction potential as a function of the separation in comparison with the result in the standard instanton calculus (1.1), we show that our ansatz is consistent with (1.1) even from short to large separations

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Summary

ZN twisted boundary conditions

We propose a neutral bion ansatz for a ZN twisted boundary condition in the CP N−1 model on R1 × S1. ZN twisted boundary conditions in a compactified direction is expressed as [12,13,14]. We note that the gauge field defined in the CP N−1 model (2.2) has the same Wilson-loop holonomy for ZN twisted boundary condition. Difference between (3.1) and (3.3) for N = 2 is just superficial and unphysical, since two different ansatz of ω(x) with an overall boundary condition factor e−iπ/2 result in the same projection field P(x) as we will show later. Fractionalized instantons (domain wall-instantons) carry the minimum topological charges in the CP N−1 model on R1 × S1 with a twisted boundary condition [50,51,52]. From subsection we make all the dimensionful quantities and parameters dimensionless by using the compact scale L (L → 1) unless we have a special reason to recover it

Fractionalized instantons
Neutral bions
Bions with non-ZN twisted boundary conditions
Bions for the split twisted boundary condition
Bions in extended split boundary conditions
Summary and discussion
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