Abstract:Recent insights into the conceptual structure of localization in QFT ("modular localization") led to clarifications of old unsolved problems. The oldest one is the Einstein-Jordan conundrum which led Jordan in 1925 to the discovery of quantum field theory. This comparison of fluctuations in subsystems of heat bath systems (Einstein) with those resulting from the restriction of the QFT vacuum state to an open subvolume (Jordan) leads to a perfect analogy; the globally pure vacuum state becomes upon local restri… Show more
“…A gauge theoretic formulation for s > 1 interactions does not seem to be known. On the other hand the higher spin analogs of the linear relation between stringlocal free fields and their pointlike partners in the same localization class are rather straightforward; instead of a single scalar stringlike Stückelberg field one obtains a linear relation involving a family of intrinsic tensor Stückelberg fields for all spins up to s−1 [12]. These are the prerequisites for an extension to higher spin interactions.…”
“…This new concept is not only important for the ongoing research in QFT[11], but it also permits to understand old problems in a new light[12] 13. Based on the standard idea that a click in a counter localizes a particle in the counter (with rapidly decreasing vacuum polarization caused tails).…”
Wigner's famous 1939 classification of positive energy representations, combined with the more recent modular localization principle, has led to a significant conceptual and computational extension of renormalized perturbation theory to interactions involving fields of higher spin. Traditionally the clash between pointlike localization and the the Hilbert space was resolved by passing to a Krein space setting which resulted in the wellknown BRST gauge formulation. Recently it turned out that maintaining a Hilbert space formulation for interacting higher spin fields requires a weakening of localization from point-to string-like fields for which the d=s+1 short distance scaling dimension for integer spins is reduced to d=1 and and renormalizable couplings in the sense of power-counting exist for any spin.This new setting leads to a significant conceptual change of the relation of massless couplings with their massless counterpart. Whereas e.g. the renormalizable interactions of s=1 massive vectormesons with s<1 matter falls within the standard field-particle setting, their zero mass limits lead to much less understood phenomena as "infraparticles" and gluon/quark confinement. It is not surprising that such drastic conceptual changes in the area of gauge theories also lead to a radical change concerning the Higgs issue.
“…A gauge theoretic formulation for s > 1 interactions does not seem to be known. On the other hand the higher spin analogs of the linear relation between stringlocal free fields and their pointlike partners in the same localization class are rather straightforward; instead of a single scalar stringlike Stückelberg field one obtains a linear relation involving a family of intrinsic tensor Stückelberg fields for all spins up to s−1 [12]. These are the prerequisites for an extension to higher spin interactions.…”
“…This new concept is not only important for the ongoing research in QFT[11], but it also permits to understand old problems in a new light[12] 13. Based on the standard idea that a click in a counter localizes a particle in the counter (with rapidly decreasing vacuum polarization caused tails).…”
Wigner's famous 1939 classification of positive energy representations, combined with the more recent modular localization principle, has led to a significant conceptual and computational extension of renormalized perturbation theory to interactions involving fields of higher spin. Traditionally the clash between pointlike localization and the the Hilbert space was resolved by passing to a Krein space setting which resulted in the wellknown BRST gauge formulation. Recently it turned out that maintaining a Hilbert space formulation for interacting higher spin fields requires a weakening of localization from point-to string-like fields for which the d=s+1 short distance scaling dimension for integer spins is reduced to d=1 and and renormalizable couplings in the sense of power-counting exist for any spin.This new setting leads to a significant conceptual change of the relation of massless couplings with their massless counterpart. Whereas e.g. the renormalizable interactions of s=1 massive vectormesons with s<1 matter falls within the standard field-particle setting, their zero mass limits lead to much less understood phenomena as "infraparticles" and gluon/quark confinement. It is not surprising that such drastic conceptual changes in the area of gauge theories also lead to a radical change concerning the Higgs issue.
“…The important role of the S-matrix for modular localization in wedges has triggered attempts to reconstruct a full causal QFT from its "on-shell footprint" in form of its S-matrix [77,78]. These ideas are presently too weak for constructions in higher dimensions.…”
Section: A Critical Perspective Based On Modular Localizationmentioning
“…14 Maybe all these problems can be resolved in the wider context of algebraic quantum field theory by means of the promising idea of modular localization [111]. 1.1.6 Approaches to quantum field theory Figure 1.4 on p. 26 suggests that a large number of particles can be created in a high-energy proton-proton collision.…”
Section: On the Measurement Problemmentioning
confidence: 99%
“…Whereas mainstream physics clearly goes with the successful pragmatic approach, the supposed necessity to choose between "no (mathematical) rigor" and "no (practical) relevance" is much harder for philosophers, as they should insist on both (so should physicists). The powerful concept of modular localization, which is based on the Tomita-Takesaki modular theory of operator algebras, has a promising potential for achieving the big goal of bringing the algebraic and pragmatic approaches together, thus even revealing the reasons for the success of the pragmatic approach and at the same time leading to a deeper understanding of the quantization of gauge theories and to a demystification of the Higgs mechanism (for an overview, see [111]). Moreover, the ensemble aspect and statistical mechanics type of probability follow naturally from modular localization, although in a more radical way compared to how we here implement these features by an irreversible contribution to time evolution on a finite space.…”
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