Abstract
We construct a quantum mechanical matrix model that approximates $\mathcal{N}=1$ super-Yang-Mills on $S^3\times\mathbb{R}$. We do so by pulling back the set of left-invariant connections of the gauge bundle onto the real superspace, with the spatial $\mathbb{R}^3$ compactified to $S^3$. We quantize the $\mathcal{N}=1$ $SU(2)$ matrix model in the weak-coupling limit using the Born-Oppenheimer approximation and find that different superselection sectors emerge for the effective gluon dynamics in this regime, reminiscent of different phases of the full quantum theory. We demonstrate that the Born-Oppenheimer quantization is indeed compatible with supersymmetry, albeit in a subtle manner. In fact, we can define effective supercharges that relate the different sectors of the matrix model's Hilbert space. These effective supercharges have a different definition in each phase of the theory.
Highlights
It is hard to overemphasize the importance of Yang-Mills theory [1] in theoretical physics
We quantize the N 1⁄4 1 SUð2Þ matrix model in the weak-coupling limit g ≪ 1, with g the dimensionless gauge coupling constant, using the BornOppenheimer approximation and find that different superselection sectors emerge for the effective gluon dynamics in this regime, reminiscent of different phases of the full quantum theory
We demonstrate that the Born-Oppenheimer quantization is compatible with supersymmetry, albeit in a subtle manner
Summary
It is hard to overemphasize the importance of Yang-Mills theory [1] in theoretical physics. A (0 þ 1)-dimensional reduction of Yang-Mills on S3 × R to a matrix model was obtained in [2] By construction, this model is expected to be valid for a small enough radius ρ of the spatial S3, so that the higher Fourier modes of the quantum fields can be consistently truncated. Mechanical models [14,15,16,17,18] This fact, added to the success of the quantum-mechanical matrix model first proposed in [2] in capturing the variety of important nonperturbative aspects of Yang-Mills theory, motivates us to study a quantum mechanical reduction of SYM theory. We study the quantum phase structure of the model in the weak-coupling regime via Born-Oppenheimer quantization.
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