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Mass for Plasma Photons from Gauge Symmetry Breaking, Europhys. Lett. 75 189, hep-th/0601166. 5 M. Gasperini, Anomalous electromagnetic effects in the mixing of photons with a neutral vector (1991)

by J T Mendonça, P Castelo Ferreira
Venue:Photon - Graviphoton Mixing In A Dielectric Medium, Phys. Lett. B237
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Ue(1) × Ug(1) actions in 2+1-dimensions: Full vectorial electric and magnetic

by P. Castelo Ferreira
"... It is considered a dimensional reduction of Ue(1) × Ug(1) 3 + 1-dimensional electromagnetism to 2 + 1-dimensions. It is shown that all the six electric and magnetic field vectorial components are present in the reduced theory and that they can be described in terms of vector gauge fields. The quant ..."
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It is considered a dimensional reduction of Ue(1) × Ug(1) 3 + 1-dimensional electromagnetism to 2 + 1-dimensions. It is shown that all the six electric and magnetic field vectorial components are present in the reduced theory and that they can be described in terms of vector gauge fields. The quantum structure is maintained in the absence of boundary effects. In the case where boundary effects are present a cross Chern-Simons term between both gauge fields is present such that the quantum structure of the reduced theory changes. The dimensional reduced action is invariant under parity (P) and time-inversion (T). PACS: 03.50.De, 12.20.m, 41.20.q, 13.40.f Keywords: Electromagnetism, Two Dimensions, pseudo-photon
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...on can be implemented such that the scalar fields are charged under the gauge groups, in such case it is necessary to consider gauge covariant derivatives such that the action remains gauge invariant =-=[17,18]-=-. We do not develop this topic here. We also remark that the middle terms in equation (7) could be integrated by parts, however this would hold boundary terms that are not gauge invariant. 3 Field Def...

A Pseudo-Photon in Non-Trivial Background

by P. Castelo Ferreira
"... We show that in the presence of external fields for which either ˙ B ext = 0 or ∇ × E ext = 0 it is not possible to derive the classical Maxwell equations from an action with only one gauge field. We suggest that one possible solution is to consider a second physical pseudo-vector gauge field C. ..."
Abstract - Cited by 4 (4 self) - Add to MetaCart
We show that in the presence of external fields for which either ˙ B ext = 0 or ∇ × E ext = 0 it is not possible to derive the classical Maxwell equations from an action with only one gauge field. We suggest that one possible solution is to consider a second physical pseudo-vector gauge field C. The action for this theory is originally motivated by the inclusion of magnetic monopoles. These particles play no role in this work and our argument is only based in, that the violation of the Bianchi identities, cannot be accounted at the action level with only the standard gauge field. We give a particular example for a periodic rotating external magnetic field. Our construction holds that at classical level both the vector and pseudo-vector gauge fields A and C are regular. We compare pseudo-photon with paraphoton (graviphoton) theories concluding that, besides the mechanisms of gauge symmetry already studied by the authors, the Bianchi identities violation are a crucial difference between both theories. We also show that the effects in PVLAS experiment due to the inclusion of pseudo-photons cannot be distinguished from the usual classical induced electric and magnetic fields due to the standard Maxwell equations. Therefore, although this kind of optical experiments cannot test the existence of pseudo-photons, they do not exclude its existence. PACS: 03.50.De, 12.20.m,11.15.-q
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...es of freedom [7,9]. Although this seems simply a technicality it has very striking consequences in relation to the Bianchi identities and on mechanisms of gauge symmetry breaking and mass generation =-=[10,11]-=-. The most easy way to explain this difference between both theories is to note that the map between both theories presented in [10] is generally non-regular, i.e. a pseudo-vector regular field config...

September 2006 A Pseudo-Photon in Non-Trivial Background Fields

by P. Castelo Ferreira, J. Tito Mendonça , 2006
"... We show that in the presence of external fields for which either ˙ B ext = 0 or ∇ × E ext = 0 it is not possible to derive the classical Maxwell equations from an action with only one gauge field. We suggest that one possible solution is to consider a second physical pseudo-vector gauge field C. ..."
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We show that in the presence of external fields for which either ˙ B ext = 0 or ∇ × E ext = 0 it is not possible to derive the classical Maxwell equations from an action with only one gauge field. We suggest that one possible solution is to consider a second physical pseudo-vector gauge field C. The action for this theory is originally motivated by the inclusion of magnetic monopoles. These particles play no role in this work and our argument is only based in, that the violation of the Bianchi identities, cannot be accounted at the action level with only the standard gauge field. We give a particular example for a periodic rotating external magnetic field. Our construction holds that at classical level both the vector and pseudo-vector gauge fields A and C are regular. We compare pseudo-photon with paraphoton (graviphoton) theories concluding that, besides the mechanisms of gauge symmetry already studied by the authors, the Bianchi identities violation are a crucial difference between both theories. We also show that the effects in PVLAS experiment due to the inclusion of pseudo-photons cannot be distinguished from the usual classical induced electric and magnetic fields due to the standard Maxwell equations. Therefore, although this kind of optical experiments cannot test the existence of pseudo-photons, they do not exclude its existence. PACS:?03.50.De,?03.70.+k,?11.15.-q
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...es of freedom [7,9]. Although this seems simply a technicality it has very striking consequences in relation to the Bianchi identities and on mechanisms of gauge symmetry breaking and mass generation =-=[10,11]-=-. The most easy way to explain this difference between both theories is to note that the map between both theories presented in [10] is generally non-regular, i.e. a pseudo-vector regular field config...

July 2007, hep-th/0601171 Generalized Proca Equations and Vacuum Current from Breaking of Ue(1) × Ug(1) Gauge Symmetry

by P. Castelo Ferreira, J. T. Mendonça , 2007
"... We study a Ue(1) × Ug(1) Electric-Magnetic theory with minimal coupling between both gauge fields A (photon) and C (pseudo-photon). We consider two possible mechanism of symmetry breaking that generate generalized Proca masses for the gauge field A. By considering a vacuumexpectation-value (vev) fo ..."
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We study a Ue(1) × Ug(1) Electric-Magnetic theory with minimal coupling between both gauge fields A (photon) and C (pseudo-photon). We consider two possible mechanism of symmetry breaking that generate generalized Proca masses for the gauge field A. By considering a vacuumexpectation-value (vev) for the C field in the full Ue(1) ×Ug(1) theory we obtain both a mass term and a vacuum current. By considering the broken electric theory Ue(1) we obtain as a solution for the C field a remaining free field c such that, upon be given a vev, renders a mass term for the photon field A. The interpretation for the vev is given in terms of constant currents and homology cycles of the underlying space manifold. The number of degrees of freedom, before and after gauge symmetry breaking, are discussed. As a particular case of this construction the authors have already shown that this mechanism reproduces the Schwinger-Anderson mechanism such that upon gauge symmetry breaking due to non trivial vacuum generates mass for the standard photon (plasmon). We show that, although generally, Lorentz symmetry may be broken in the pseudophoton sector due to its vev, the effective theory for the standard photon still preserves Lorentz invariance.
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...his is an important remark, although we are reproducing well known effective results (in particular the SchwingerAnderson [7,8] mechanism can be described by the construction studied here as shown in =-=[18]-=-), we must stress that our approach is new and that the physical interpretation is distinct, the effective mass (and vacuum current when present) are due to the pseudo-photon vev. 22 Generalized Proc...

Explicit Actions for Electromagnetism with Two Gauge Fields with Only one Electric and one Magnetic Physical Fields

by unknown authors , 2006
"... We extend the work of Mello et al. based in Cabbibo and Ferrari concerning the description of electromagnetism with two gauge fields from a variational principle, i.e. an action. We provide a systematic independent derivation of the allowed actions which have only one magnetic and one electric physi ..."
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We extend the work of Mello et al. based in Cabbibo and Ferrari concerning the description of electromagnetism with two gauge fields from a variational principle, i.e. an action. We provide a systematic independent derivation of the allowed actions which have only one magnetic and one electric physical fields and are invariant under the discrete symmetries P and T. We conclude that neither the Lagrangian, nor the Hamiltonian, are invariant under the electromagnetic duality rotations. This agrees with the weak-strong coupling mixing characteristic of the duality due to the Dirac quantization condition providing a natural way to differentiate dual theories related by the duality rotations (the energy is not invariant). Also the standard electromagnetic duality rotations considered in this work violate both P and T by inducing Hopf terms (theta terms) for each sector and a mixed Maxwell term. The canonical structure of the theory is briefly addressed and the magnetic gauge sector is interpreted as a ghost sector.
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...tric description of the theory. Also compatible with this last mechanism we can give a vacuum-expectation-value to the C field that renders an effective Proca mass to the standard photon, the A field =-=[18,19]-=-. 1 This argument is not completely closed once there are ways of implementing duality rotations that preserve P and T symmetries [13,14]. 12 Electromagnetic Duality The study of theories with two ga...

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