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The condensate in commutative and noncommutative theories Dmitri Bykov Moscow State University
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Overview of dimension two condensates in gluodynamics and Contribute to OPEs, for example, The gluon condensate may be sensitive to various topological defects such as Dirac strings and monopoles. [F.V.Gubarev, L.Stodolsky, V.I.Zakharov, 2001]
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Curci-Ferrari gauge: BRST-invariant on-shell [K.-I. Kondo, 2001] Landau-type -gauges: [D.B., A.A.Slavnov, 2005]
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Gauge theory on a noncommutative plane Weyl ordering Product of operators Moyal product of symbols [Review: M.Douglas, N.Nekrasov, 2001]
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Noncommutative gauge theory as a matrix model is a field with values in the Lie algebra Action: The shift leads us to conventional gauge theory with action
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Gauge transformations in the matrix model language (homogeneous!) Thus, we have a gauge-invariant (non-local) operator
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In the conventional gauge theory language this operator is [A.A.Slavnov, 2004] an (infinite) constant operator with zero v.e.v.: operator with the desired condensate as its v.e.v. Is the condensate gauge-invariant?
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Important question arises: ? This is not always true ! Counterexample – the partial isometry operator
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Back to our case Under a «quantum» gauge transformation the variation of the condensate is non-zero: Here is fixed! [R.N.Baranov, D.B., A.A.Slavnov, 2006]
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1. The operator is still gauge-invariant, if one considers Ward identities. 2. The volume-averaged operator decouples from Green’s functions
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Result: The condensate is invariant under a limited set of gauge transformations. Thank you for attention.
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