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Light-Front QCD(1+1) Coupled to Chiral Adjoint Fermions
High Energy Physics - Theory · Submitted 18 Dec 1995
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find exact expressions for the degenerate vacuum states and the analog of the \theta vacuum.
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The abstract, sentence by sentence
We consider SU(N) gauge theory in 1+1 dimensions coupled to chiral fermions in the adjoint representation of the gauge group. With all fields in the adjoint representation the gauge group is actually SU(N)/Z_N, which possesses nontrivial topology. In particular, there are N distinct topological sectors and the physical vacuum state has a structure analogous to a \theta vacuum. We show how this feature is realized in light-front quantization for the case N=2, using discretization as an infrared regulator. In the discretized form of the theory the nontrivial vacuum structure is associated with the zero momentum mode of the gauge field A^+. We find exact expressions for the degenerate vacuum states and the analog of the \theta vacuum. The model also possess a condensate which we calculate. We discuss the difference between this chiral light-front theory and the theories that have previously been considered in the equal-time approach.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider SU(N) gauge theory in 1+1 dimensions coupled to chiral fermions in the adjoint representation of the gauge group. | background 0.54 | 0.40 | 0.04 | asserted 0.94 |
| s1 | With all fields in the adjoint representation the gauge group is actually SU(N)/Z_N, which possesses nontrivial topology. | background 0.83 | 0.16 | 0.07 | asserted 1.00 |
| s2 | In particular, there are N distinct topological sectors and the physical vacuum state has a structure analogous to a \theta vacuum. | background 0.63 | 0.18 | 0.15 | asserted 1.00 |
| s3 | We show how this feature is realized in light-front quantization for the case N=2, using discretization as an infrared regulator. | method 0.75 | 0.93 | 0.10 | asserted 1.00 |
| s4 | In the discretized form of the theory the nontrivial vacuum structure is associated with the zero momentum mode of the gauge field A^+. | result 0.80 | 0.72 | 0.11 | asserted 1.00 |
| s5 | We find exact expressions for the degenerate vacuum states and the analog of the \theta vacuum. | result 0.98 | 0.97 | 0.33 | asserted 1.00 |
| s6 | The model also possess a condensate which we calculate. | result 0.94 | 0.95 | 0.08 | asserted 0.99 |
| s7 | We discuss the difference between this chiral light-front theory and the theories that have previously been considered in the equal-time approach. | contribution 0.65 | 0.51 | 0.07 | asserted 0.57 |
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The paper
Original abstract
We consider SU(N) gauge theory in 1+1 dimensions coupled to chiral fermions in the adjoint representation of the gauge group. With all fields in the adjoint representation the gauge group is actually SU(N)/Z_N, which possesses nontrivial topology. In particular, there are N distinct topological sectors and the physical vacuum state has a structure analogous to a \theta vacuum. We show how this feature is realized in light-front quantization for the case N=2, using discretization as an infrared regulator. In the discretized form of the theory the nontrivial vacuum structure is associated with the zero momentum mode of the gauge field A^+. We find exact expressions for the degenerate vacuum states and the analog of the \theta vacuum. The model also possess a condensate which we calculate. We discuss the difference between this chiral light-front theory and the theories that have previously been considered in the equal-time approach.
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