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In gauge theory, especially in non-abelian gauge theories, global problems at gauge fixing are often encountered. Gauge fixing means choosing a representative from each gauge orbit. The space of representatives is a submanifold and represents the gauge fixing condition. Ideally, every gauge orbit will intersect this submanifold once and only once. Unfortunately, this is often impossible globally for non-abelian gauge theories because of topological obstructions and the best that can be done is make this condition true locally. A gauge fixing submanifold may not intersect a gauge orbit at all or it may intersect it more than once. This is called a Gribov ambiguity (named after Vladimir Gribov). Gribov ambiguities lead to a nonperturbative failure of the BRST symmetry, among other things. A way to resolve the problem of Gribov ambiguity is to restrict the relevant functional integrals to a single Gribov region whose boundary is called a Gribov horizon. See also the original paper of Gribov,〔V. N. Gribov. Quantization of non-abelian gauge theories. Nuclear Physics B139 (1978), p.1-19〕 Heinzl's paper with a quantum-mechanical toy example,〔T. Heinzl. Hamiltonian Approach to the Gribov Problem. Nuclear Physics B (Proc.Suppl) 54A (1997) 194-197, arXiv:hep-th/9609055,〕 and the second slide of Kondo's presentation.〔http://www.icra.it/MG/mg12/talks/sqg5_kondo.pdf〕 ==References== 〔 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Gribov ambiguity」の詳細全文を読む スポンサード リンク
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