“…SLF can be successfully applied to large classes of models beyond QED [20], including SM weak interactions [11]. We consider it as a promising alternative to the gauge theory plus BRST setting, that does not explicitly use indefinite metric at intermediate steps.…”
Section: Discussionmentioning
confidence: 99%
“…(This conflict with the terminology of the Higgs mechanism does not enjoy the attention that it deserves.) The absence of SSB does not mean that there is no Higgs particle in SLF -only it is not the driving agent, but its presence is a necessity for the self-consistency of the theory [20]. It is presently not clear whether the notion of local symmetries in terms of locally conserved observable currents, as known from Lagrangian quantization with spin s < 1, extends to non-Abelian currents in SLF.…”
Section: Discussionmentioning
confidence: 99%
“…Because it entails the possibility of "measurement of charges at a distance", it is well-known to be in conflict with locality of charged fields [1,9]. We show how a new approach to QED advocated in [15,19,20,13] that avoids indefinite metric and ghosts, can achieve Gauss' Law. We explain why this is not at variance with recent results in [5].Dedicated to Detlev Buchholz on the occasion of his 75th birthday…”
mentioning
confidence: 99%
“…In an emergent approach [15,19,20,13], a perturbative construction of QED is proposed that avoids indefinite metric from the outset. It exploits the fact that the cohomological problem…”
The quantum Gauss Law as an interacting field equation is a prominent feature of QED with eminent impact on its algebraic and superselection structure and the properties of its charged particles. Because it entails the possibility of "measurement of charges at a distance", it is well-known to be in conflict with locality of charged fields [1,9]. We show how a new approach to QED advocated in [15,19,20,13] that avoids indefinite metric and ghosts, can achieve Gauss' Law. We explain why this is not at variance with recent results in [5].Dedicated to Detlev Buchholz on the occasion of his 75th birthday
“…SLF can be successfully applied to large classes of models beyond QED [20], including SM weak interactions [11]. We consider it as a promising alternative to the gauge theory plus BRST setting, that does not explicitly use indefinite metric at intermediate steps.…”
Section: Discussionmentioning
confidence: 99%
“…(This conflict with the terminology of the Higgs mechanism does not enjoy the attention that it deserves.) The absence of SSB does not mean that there is no Higgs particle in SLF -only it is not the driving agent, but its presence is a necessity for the self-consistency of the theory [20]. It is presently not clear whether the notion of local symmetries in terms of locally conserved observable currents, as known from Lagrangian quantization with spin s < 1, extends to non-Abelian currents in SLF.…”
Section: Discussionmentioning
confidence: 99%
“…Because it entails the possibility of "measurement of charges at a distance", it is well-known to be in conflict with locality of charged fields [1,9]. We show how a new approach to QED advocated in [15,19,20,13] that avoids indefinite metric and ghosts, can achieve Gauss' Law. We explain why this is not at variance with recent results in [5].Dedicated to Detlev Buchholz on the occasion of his 75th birthday…”
mentioning
confidence: 99%
“…In an emergent approach [15,19,20,13], a perturbative construction of QED is proposed that avoids indefinite metric from the outset. It exploits the fact that the cohomological problem…”
The quantum Gauss Law as an interacting field equation is a prominent feature of QED with eminent impact on its algebraic and superselection structure and the properties of its charged particles. Because it entails the possibility of "measurement of charges at a distance", it is well-known to be in conflict with locality of charged fields [1,9]. We show how a new approach to QED advocated in [15,19,20,13] that avoids indefinite metric and ghosts, can achieve Gauss' Law. We explain why this is not at variance with recent results in [5].Dedicated to Detlev Buchholz on the occasion of his 75th birthday
“…A good candidate SEM for unbounded helicity particles now also exists in SL field theory [24]. The Velo-Zwanziger instability [25] is exorcised [26]. The prohibition for covariant spinorial field types (A, B) to represent massless Wigner particles of helicity r, unless r = B − A, argued in Section 5.9 of [19], has been made void.…”
Modular localization and the theory of string-localized fields have revolutionized several key aspects of quantum field theory. They reinforce the contention that local symmetry emerges directly from quantum theory, but global gauge invariance remains in general an unwarranted assumption to be examined case by case. Armed with those modern tools, we reconsider here the classical Okubo–Marshak argument on the non-existence of a “strong CP problem” in quantum chromodynamics.
A non-perturbative and exactly solvable quantum field theoretical model for a “dressed Dirac field” is presented, that exhibits all the kinematical features of QED: an appropriate delocalization of the charged field as a prerequisite for the global Gauss Law, superselected photon clouds (asymptotic expectation values of the Maxwell field), infraparticle nature of charged particles that cannot be separated from their photon clouds, broken Lorentz symmetry. The model serves as an intermediate leg on a new roadmap towards full QED, formulated as an off-shell theory, i.e., including a perturbative construction of its interacting charged fields. It also fills a gap in recent discussions of the “Infrared Triangle”, and points the way towards a new scattering theory for theories with massless particles of helicity ≥ 1, in which infraparticles can be described at the level of charged fields, rather than just states.
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