Abstract:Massive vector fields can be described in a gauge invariant way with the introduction of compensating fields. In the unitary gauge one recovers the original formulation. Although this gauging mechanism can be extended to noncommutative spaces in a straightforward way, non trivial aspects show up when we consider the Seiberg-Witten map. As we show here, only a particular class of its solutions leads to an action that admits the unitary gauge fixing.
“…We also note that the MCS coupling constant g 2 and the Chern-Simons parameter µ have both appeared as inverse couplings when compared with (20). We can now fix the gauge invariance in (24), for instance by choosing the unitary gauge Λ = 0, to recover the self-dual model given in (20). We thus conclude that the U (1) invariant MCS theory is dual to the U(1) invariant Stückelberg formulation of self-dual model.…”
Section: Equivalence Of the Mcs Theory And The Sd Modelmentioning
confidence: 73%
“…In [24] the SW map for the NC Stückelberg-Proca theory has been obtained by requiring that in the unitary gauge it gives the Proca theory. Using the same criterion, the SW map for the NC Stückelberg-SD model is found to bê…”
Section: The Ncsd Model With a Compensatingmentioning
We consider the Maxwell-Chern-Simons theory in noncommutative three dimensional space-time.We show that the Seiberg-Witten map is ambiguous due to the dimensional coupling constant. To get the dual theory we start from a master action obtained by promoting the global shift invariance to a local one. We also obtain the mapping between the observables of the two equivalent theories.We show that the equivalence between the Maxwell-Chern-Simons theory and the self-dual model in commutative space-time does not survive in the non-commutative setting.
“…We also note that the MCS coupling constant g 2 and the Chern-Simons parameter µ have both appeared as inverse couplings when compared with (20). We can now fix the gauge invariance in (24), for instance by choosing the unitary gauge Λ = 0, to recover the self-dual model given in (20). We thus conclude that the U (1) invariant MCS theory is dual to the U(1) invariant Stückelberg formulation of self-dual model.…”
Section: Equivalence Of the Mcs Theory And The Sd Modelmentioning
confidence: 73%
“…In [24] the SW map for the NC Stückelberg-Proca theory has been obtained by requiring that in the unitary gauge it gives the Proca theory. Using the same criterion, the SW map for the NC Stückelberg-SD model is found to bê…”
Section: The Ncsd Model With a Compensatingmentioning
We consider the Maxwell-Chern-Simons theory in noncommutative three dimensional space-time.We show that the Seiberg-Witten map is ambiguous due to the dimensional coupling constant. To get the dual theory we start from a master action obtained by promoting the global shift invariance to a local one. We also obtain the mapping between the observables of the two equivalent theories.We show that the equivalence between the Maxwell-Chern-Simons theory and the self-dual model in commutative space-time does not survive in the non-commutative setting.
“…In [13] the SW map for the NC Stückelberg-Proca theory has been obtained by requiring that in the unitary gauge it gives the Proca theory. Using the same criterion, the SW map for the NC Stückelberg-SD model is found to bê …”
Applying a master action technique we obtain the dual of the noncommutative Maxwell-ChernSimons theory. The equivalence between the Maxwell-Chern-Simons theory and the self-dual model in commutative space-time does not survive in the non-commutative setting. We also point out an ambiguity in the Seiberg-Witten map.
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