Mass-deformed super Yang-Mills theory on $$ {\mathbbm{T}}^4 $$: sum over twisted sectors, θ-angle, and CP violation

A bstract We study SU( N ) super Yang-Mills theory with a small gaugino mass m and vacuum angle θ on the four-torus $$ {\mathbbm{T}}^4 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>T</mml:mi> <mml:mn>4</mml:mn> </mml:msup> </mml:math> with ’t Hooft twisted boundary conditions. Introducing a detuning parameter ∆, which measures the deviation from an exactly self-dual $$ {\mathbbm{T}}^4 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>T</mml:mi> <mml:mn>4</mml:mn> </mml:msup> </mml:math> , and working in the limits mLN ≪ Λ LN ≪ 1 and $$ \frac{\left(N-1\right){m}^2{L}^2}{4\pi}\ll \Delta \ll 1 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mfrac> <mml:mrow> <mml:mfenced> <mml:mrow> <mml:mi>N</mml:mi> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:mfenced> <mml:msup> <mml:mi>m</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> <mml:mrow> <mml:mn>4</mml:mn> <mml:mi>π</mml:mi> </mml:mrow> </mml:mfrac> <mml:mo>≪</mml:mo> <mml:mtext>∆</mml:mtext> <mml:mo>≪</mml:mo> <mml:mn>1</mml:mn> </mml:math> , where L is the torus size and Λ the strong-coupling scale, we compute the scalar and pseudo-scalar condensates to leading order in m 2 L 2 /∆. The twists generate fractional-charge instantons, and we show that summing over all such contributions is crucial for reproducing the correct physical observables in the decompactified strong-coupling regime. From a Hamiltonian perspective, the sum over twisted sectors, already at small torus size, projects in the m = 0 limit onto a definite superselection sector of the ℝ 4 theory. In the massless limit, we recover the exact value of the gaugino condensate |〈 λλ 〉| = 16 π 2 Λ 3 , and demonstrate how a spurious U(1) symmetry eliminates all $$ \mathcal{CP} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>CP</mml:mi> </mml:math> -violating effects. Our results are directly testable in lattice simulations, and our method extends naturally to non-supersymmetric gauge theories.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-10-21
DOI
https://doi.org/10.1007/jhep10(2025)182
Citations
1
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
1.87

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article

Mass-deformed super Yang-Mills theory on $$ {\mathbbm{T}}^4 $$: sum over twisted sectors, θ-angle, and CP violation

Mohamed M. Anber, Erich Poppitz
1 citations
Journal of High Energy Physics
Particle physics theoretical and experimental studies
1.87
article

Mass-deformed super Yang-Mills theory on $$ {\mathbbm{T}}^4 $$: sum over twisted sectors, θ-angle, and CP violation

Mohamed M. Anber, Erich Poppitz
article en
1 citations

Abstract

A bstract We study SU( N ) super Yang-Mills theory with a small gaugino mass m and vacuum angle θ on the four-torus $$ {\mathbbm{T}}^4 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>T</mml:mi> <mml:mn>4</mml:mn> </mml:msup> </mml:math> with ’t Hooft twisted boundary conditions. Introducing a detuning parameter ∆, which measures the deviation from an exactly self-dual $$ {\mathbbm{T}}^4 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>T</mml:mi> <mml:mn>4</mml:mn> </mml:msup> </mml:math> , and working in the limits mLN ≪ Λ LN ≪ 1 and $$ \frac{\left(N-1\right){m}^2{L}^2}{4\pi}\ll \Delta \ll 1 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mfrac> <mml:mrow> <mml:mfenced> <mml:mrow> <mml:mi>N</mml:mi> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:mfenced> <mml:msup> <mml:mi>m</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> <mml:mrow> <mml:mn>4</mml:mn> <mml:mi>π</mml:mi> </mml:mrow> </mml:mfrac> <mml:mo>≪</mml:mo> <mml:mtext>∆</mml:mtext> <mml:mo>≪</mml:mo> <mml:mn>1</mml:mn> </mml:math> , where L is the torus size and Λ the strong-coupling scale, we compute the scalar and pseudo-scalar condensates to leading order in m 2 L 2 /∆. The twists generate fractional-charge instantons, and we show that summing over all such contributions is crucial for reproducing the correct physical observables in the decompactified strong-coupling regime. From a Hamiltonian perspective, the sum over twisted sectors, already at small torus size, projects in the m = 0 limit onto a definite superselection sector of the ℝ 4 theory. In the massless limit, we recover the exact value of the gaugino condensate |〈 λλ 〉| = 16 π 2 Λ 3 , and demonstrate how a spurious U(1) symmetry eliminates all $$ \mathcal{CP} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>CP</mml:mi> </mml:math> -violating effects. Our results are directly testable in lattice simulations, and our method extends naturally to non-supersymmetric gauge theories.

Journal of High Energy PhysicsVol. 2025(10)
University of Toronto (CA), Durham University (GB)
University of Toronto, Natural Sciences and Engineering Research Council of Canada, Science and Technology Facilities Council
Openalex Percentile: Top 11%
Particle physics theoretical and experimental studies
1.87
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