The Sum Over Topological Sectors and $θ$ in the 2+1-Dimensional $\mathbb{C}\mathbb{P}^1$ $σ$-Model
Daniel S. Freed, Zohar Komargodski, Nathan Seiberg
TL;DR
This work analyzes the sum over topological sectors in the 2+1 dimensional CP^1 sigma-model and shows that locality and unitarity constrain the theta parameter to θ=0 or θ=π, yielding bosonic/skyrmion statistics. By embedding CP^N in a linear UV theory with U(1) gauge fields and CS couplings, the authors derive a Wess-Zumino term in the IR (for N>1) and a mod 2 invariant (for N=1), linking theta to the spin-statistics of Skyrmions via the Hopf invariant. They then demonstrate how coupling to a TQFT or modifying the UV gauge structure can produce anyon-like behavior, but argue that purely local, well-defined theories demand θ∈{0,π} unless extended by invertible field theories, with a rigorous classification using spin and spin^c bordism via Freed–Hopkins results. The combination of geometric and topological methods establishes precise consistency conditions for theta-terms in the CP^1 model on general 3-manifolds and clarifies when fractional statistics can emerge only through coupling to topological sectors. The findings have implications for condensed-mmatter constructions and for understanding global consistency constraints in quantum field theories with nontrivial topological sectors.
Abstract
We discuss the three spacetime dimensional $\mathbb{C}\mathbb{P}^N$ model and specialize to the $\mathbb{C}\mathbb{P}^1$ model. Because of the Hopf map $π_3(\mathbb{C}\mathbb{P}^1)=\mathbb{Z}$ one might try to couple the model to a periodic $θ$ parameter. However, we argue that only the values $θ=0$ and $θ=π$ are consistent. For these values the Skyrmions in the model are bosons and fermions respectively, rather than being anyons. We also extend the model by coupling it to a topological quantum field theory, such that the Skyrmions are anyons. We use techniques from geometry and topology to construct the $θ=π$ theory on arbitrary 3-manifolds, and use recent results about invertible field theories to prove that no other values of $θ$ satisfy the necessary locality.
