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Gribov ambiguity and non-trivial vacuum structure of gauge theories on a cylinder
High Energy Physics - Theory · Submitted 5 Dec 1992
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show by explicit construction that a proper treatment of the Gribov ambiguity leads to a highly non-trivial structure of all physical states in these quantum field theory models.
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The abstract, sentence by sentence
Using the hamiltonian framework, we analyze the Gribov problem for U(N) and SU(N) gauge theories on a cylinder (= (1+1) dimensional spacetime with compact space S^1). The space of gauge orbits is found to be an orbifold. We show by explicit construction that a proper treatment of the Gribov ambiguity leads to a highly non-trivial structure of all physical states in these quantum field theory models. The especially interesting example of massless QCD is discussed in more detail: There, some of the special static gauge transformations which are responsible for the Gribov ambiguity also lead to a spectral flow, and this implies a chiral condensate in all physical states. We also show that the latter is closely related to the Schwinger term and the chiral anomaly.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Using the hamiltonian framework, we analyze the Gribov problem for U(N) and SU(N) gauge theories on a cylinder (= (1+1) dimensional spacetime with compact space S^1). | contribution 0.79 | 0.94 | 0.05 | asserted 0.93 |
| s1 | The space of gauge orbits is found to be an orbifold. | result 1.00 | 0.94 | 0.11 | asserted 1.00 |
| s2 | We show by explicit construction that a proper treatment of the Gribov ambiguity leads to a highly non-trivial structure of all physical states in these quantum field theory models. | result 0.93 | 0.96 | 0.77 | asserted 1.00 |
| s3 | The especially interesting example of massless QCD is discussed in more detail: There, some of the special static gauge transformations which are responsible for the Gribov ambiguity also lead to a spectral flow, and this implies a chiral condensate in all physical states. | result 0.88 | 0.86 | 0.17 | asserted 0.99 |
| s4 | We also show that the latter is closely related to the Schwinger term and the chiral anomaly. | interpretation 0.50 | 0.87 | 0.08 | asserted 1.00 |
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Original abstract
Using the hamiltonian framework, we analyze the Gribov problem for U(N) and SU(N) gauge theories on a cylinder (= (1+1) dimensional spacetime with compact space S^1). The space of gauge orbits is found to be an orbifold. We show by explicit construction that a proper treatment of the Gribov ambiguity leads to a highly non-trivial structure of all physical states in these quantum field theory models. The especially interesting example of massless QCD is discussed in more detail: There, some of the special static gauge transformations which are responsible for the Gribov ambiguity also lead to a spectral flow, and this implies a chiral condensate in all physical states. We also show that the latter is closely related to the Schwinger term and the chiral anomaly.
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2 arXiv papers cite this in 3 sentences
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Uses its method or tool 1 paper
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Our approach follows the Hamiltonian framework developed by Langmann and Semenoff [ref] , in which gauge redundancies are eliminated by explicitly solving the Gauss law constraint prior to quantization.
From 2D Yang-Mills to Calogero-Sutherland via a colored particle · Introduction · 1.00
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