Quantum Field Theory

A special issue of Universe (ISSN 2218-1997). This special issue belongs to the section "Foundations of Quantum Mechanics and Quantum Gravity".

Deadline for manuscript submissions: closed (28 February 2023) | Viewed by 35945

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Theoretical High Energy Physics, University of Heidelberg, Heidelberg, Germany
Interests: quantum field theory; pure Yang-Mills theory and the foundations of quantum mechanics
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Special Issue Information

Dear Colleagues,

Quantum field theory is a convincing framework to address a variety of subatomic processes, high-energy particle reactions, and the effective physics of condensed matter systems. In particular, quantum gauge theory has acquired a prominent status. This Special Issue aims to present the latest development in local quantum field theory, perturbatively and nonperturbatively and largely analytically describing systems of variable spacetime dimension D = d + 1 and signature as well as field content. Examples are nonperturbative and analytical approaches to gauge theory (semiclassical approaximation, nonperturbative a priori estimates) and conformal field theory in d = 1, 2, 3 as well as approaches to quantum field theory that exploit a weak–strong coupling duality. We also welcome submissions discussing resummation schemes of small-coupling expansions, operator product expansions, numerical approaches such as lattice gauge theory, quantum field theoretic investigations on strongly curved spacetime backgrounds and at finite temperature, and the various approaches to quantum gravity.

Dr. Ralf Hofmann
Guest Editor

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Published Papers (12 papers)

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Editorial

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7 pages, 231 KiB  
Editorial
Quantum Field Theory
by Ralf Hofmann
Universe 2024, 10(1), 14; https://doi.org/10.3390/universe10010014 - 28 Dec 2023
Viewed by 2745
Abstract
This Special Issue on quantum field theory presents work covering a wide and topical range of subjects mainly within the area of interacting 4D quantum field theories subject to certain backgrounds [...] Full article
(This article belongs to the Special Issue Quantum Field Theory)

Research

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6 pages, 256 KiB  
Communication
Yang–Mills Instantons in the Dual-Superconductor Vacuum Can Become Confining
by Dmitry Antonov
Universe 2023, 9(6), 257; https://doi.org/10.3390/universe9060257 - 29 May 2023
Cited by 1 | Viewed by 981
Abstract
As known, the realistic, exponential, fall-off of the rate of production of light mesons in the chromo-electric field of a quark–antiquark string, as a function of the meson mass, can be obtained from the Schwinger-formula Gaussian fall-off within a phenomenological approach which assumes [...] Read more.
As known, the realistic, exponential, fall-off of the rate of production of light mesons in the chromo-electric field of a quark–antiquark string, as a function of the meson mass, can be obtained from the Schwinger-formula Gaussian fall-off within a phenomenological approach which assumes a certain distribution of the string tension. This approach gets a clear meaning in the London limit of the dual superconductor, where the logarithmic increase of the chromo-electric field towards the core of the string leads precisely to the change of the Gaussian fall-off to the exponential one, thus allowing for an identification of the phenomenological distribution of the string tension. In this paper, we demonstrate that, for this distribution of the string tension, the distribution of large-size Yang–Mills instantons, which are interacting with the confining monopole background, becomes O(1/ρ3), where ρ is the size of an instanton. Since such a distribution of large-size instantons is known to yield confinement, we conclude that, in the London limit of the dual-superconductor vacuum, instantons can form a confining medium, and we evaluate their contribution to the total string tension. Full article
(This article belongs to the Special Issue Quantum Field Theory)
24 pages, 492 KiB  
Article
Bosonic Casimir Effect in an Aether-like Lorentz-Violating Scenario with Higher Order Derivatives
by Robson A. Dantas, Herondy F. Santana Mota and Eugênio R. Bezerra de Mello
Universe 2023, 9(5), 241; https://doi.org/10.3390/universe9050241 - 20 May 2023
Cited by 7 | Viewed by 1057
Abstract
In this paper, we investigate the bosonic Casimir effect in a Lorentz-violating symmetry scenario. The theoretical model adopted consists of a real massive scalar quantum field confined in a region between two large parallel plates, having its dynamics governed by a modified Klein–Gordon [...] Read more.
In this paper, we investigate the bosonic Casimir effect in a Lorentz-violating symmetry scenario. The theoretical model adopted consists of a real massive scalar quantum field confined in a region between two large parallel plates, having its dynamics governed by a modified Klein–Gordon equation that presents a Lorentz symmetry-breaking term. In this context, we admit that the quantum field obeys specific boundary conditions on the plates. The Lorentz-violating symmetry is implemented by the presence of an arbitrary constant space-like vector in a CPT-even aether-like approach, considering a direct coupling between this vector with the derivative of the field in higher order. The modification of the Klein–Gordon equation produces important corrections on the Casimir energy and pressure. Thus, we show that these corrections strongly depend on the order of the higher derivative term and the specific direction of the constant vector, as well as the boundary conditions considered. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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6 pages, 244 KiB  
Communication
On the Temperature Dependence of the String-Breaking Distance in QCD
by Dmitry Antonov
Universe 2023, 9(2), 97; https://doi.org/10.3390/universe9020097 - 13 Feb 2023
Cited by 2 | Viewed by 1280
Abstract
The temperature dependence of the QCD string-breaking distance is evaluated in terms of the string tension and the rate of production of light mesons in the chromo-electric field of a flux tube. As a function of the meson mass, the mentioned rate can [...] Read more.
The temperature dependence of the QCD string-breaking distance is evaluated in terms of the string tension and the rate of production of light mesons in the chromo-electric field of a flux tube. As a function of the meson mass, the mentioned rate can be falling off either as a Gaussian, as suggested by the Schwinger formula, or as an exponential, which is the case in the London limit of the dual superconductor. We find an excellent agreement of the so-evaluated temperature dependence of the string-breaking distance with the respective lattice data, for the case of the meson-production rate corresponding to the London limit. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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11 pages, 352 KiB  
Article
From Soft Dirac Monopoles to the Dirac Equation
by Manfried Faber
Universe 2022, 8(8), 387; https://doi.org/10.3390/universe8080387 - 22 Jul 2022
Cited by 3 | Viewed by 1465
Abstract
In the model of topological particles we have four types of topologically stable dual Dirac monopoles with soft cores and finite mass. We discuss the steps for getting a Dirac equation for these particles. We show for the free and the interacting case [...] Read more.
In the model of topological particles we have four types of topologically stable dual Dirac monopoles with soft cores and finite mass. We discuss the steps for getting a Dirac equation for these particles. We show for the free and the interacting case that we arrive at the Dirac equation in the limit, where the soft solitons approach singular dual Dirac monopoles. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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9 pages, 280 KiB  
Article
On Emergent Particles and Stable Neutral Plasma Balls in SU(2) Yang-Mills Thermodynamics
by Ralf Hofmann and Thierry Grandou
Universe 2022, 8(2), 117; https://doi.org/10.3390/universe8020117 - 12 Feb 2022
Cited by 5 | Viewed by 4649
Abstract
For a pure SU(2) Yang–Mills theory in 4D, we revisit the spatial (3D), ball-like region of radius r0 in its bulk subject to the pressureless, deconfining phase at T0=1.32Tc, where Tc denotes the critical temperature [...] Read more.
For a pure SU(2) Yang–Mills theory in 4D, we revisit the spatial (3D), ball-like region of radius r0 in its bulk subject to the pressureless, deconfining phase at T0=1.32Tc, where Tc denotes the critical temperature for the onset of the deconfining–preconfining phase transition. Such a region possesses finite energy density and represents the self-intersection of a figure-eight shaped center-vortex loop if a BPS monopole of core radius ∼r052.4, isolated from its antimonopole by repulsion externally invoked through a transient shift of (anti)caloron holonomy (pair creation), is trapped therein. The entire soliton (vortex line plus region of self-intersection of mass m0 containing the monopole) can be considered an excitation of the pressureless and energyless ground state of the confining phase. Correcting an earlier estimate of r0, we show that the vortex-loop self-intersection region associates to the central part of a(n) (anti)caloron and that this region carries one unit of electric U(1) charge via the (electric-magnetic dually interpreted) charge of the monopole. The monopole core quantum vibrates at a thermodynamically determined frequency ω0 and is unresolved. For a deconfining-phase plasma oscillation about the zero-pressure background at T=T0, we compute the lowest frequency Ω0 within a neutral and homogeneous spatial ball (no trapped monopole) in dependence of its radius R0. For R0=r0 a comparison of Ω0 with ω0 reveals that the neutral plasma oscillates much slower than the same plasma driven by the oscillation of a monopole core. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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7 pages, 494 KiB  
Article
Implications of Quantum Gravity for Dark Matter Searches with Atom Interferometers
by Xavier Calmet and Nathaniel Sherrill
Universe 2022, 8(2), 103; https://doi.org/10.3390/universe8020103 - 5 Feb 2022
Cited by 4 | Viewed by 1690
Abstract
In this brief paper, we show that atom interferometer experiments such as MAGIS, AION and AEDGE do not only have the potential to probe very light dark matter models, but will also probe quantum gravity. We show that the linear coupling of a [...] Read more.
In this brief paper, we show that atom interferometer experiments such as MAGIS, AION and AEDGE do not only have the potential to probe very light dark matter models, but will also probe quantum gravity. We show that the linear coupling of a singlet scalar dark matter particle to electrons or photons is already ruled out by our current understanding of quantum gravity coupled to data from torsion pendulum experiments. On the other hand, the quadratic coupling of scalar dark matter to electrons and photons has a large viable parameter space which will be probed by these atom interferometers. Implications for searches of quantum gravity are discussed. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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10 pages, 291 KiB  
Article
Dual Superconductor Model of Confinement: Quantum-String Representation of the 4D Yang–Mills Theory on a Torus and the Correlation Length away from the London Limit
by Dmitry Antonov
Universe 2022, 8(1), 7; https://doi.org/10.3390/universe8010007 - 24 Dec 2021
Cited by 2 | Viewed by 2258
Abstract
This paper is devoted to the dual superconductor model of confinement in the 4D Yang–Mills theory. In the first part, we consider the latter theory compactified on a torus, and use the dual superconductor model in order to obtain the Polchinski–Strominger term in [...] Read more.
This paper is devoted to the dual superconductor model of confinement in the 4D Yang–Mills theory. In the first part, we consider the latter theory compactified on a torus, and use the dual superconductor model in order to obtain the Polchinski–Strominger term in the string representation of a Wilson loop. For a certain realistic critical value of the product of circumferences of the compactification circles, which is expressed in terms of the gluon condensate and the vacuum correlation length, the coupling of the Polchinski–Strominger term turns out to be such that the string conformal anomaly cancels out, making the string representation fully quantum. In the second part, we use the analogy between the London limit of the dual superconductor and the low-energy limit of the 4D compact QED, to obtain the partition function of the dual superconductor model away from the London limit. There, we find a decrease of the vacuum correlation length, and derive the corresponding potential of monopole currents. Full article
(This article belongs to the Special Issue Quantum Field Theory)
16 pages, 322 KiB  
Article
The Black Hole Firewall Transformation and Realism in Quantum Mechanics
by Gerard ’t Hooft
Universe 2021, 7(8), 298; https://doi.org/10.3390/universe7080298 - 13 Aug 2021
Cited by 12 | Viewed by 9917
Abstract
A procedure to derive a unitary evolution law for a quantised black hole has been proposed by the author. The proposal requires that one starts off with the entire Penrose diagram for the eternal black hole as the background metric, after which one [...] Read more.
A procedure to derive a unitary evolution law for a quantised black hole has been proposed by the author. The proposal requires that one starts off with the entire Penrose diagram for the eternal black hole as the background metric, after which one has to invoke the antipodal identification in order to see how the two asymptotic domains of this metric both refer to the same outside world. In this paper, we focus on the need to include time reversal in applying this identification. This forces us to postulate the existence of an ‘anti-vacuum’ state in our world, which is the state where energy density reaches a maximal value. We find that this squares well with the deterministic interpretation of quantum mechanics, according to which quantum Hilbert space is to be regarded as the ‘vector representation’ of a real world. One has to understand how to deal with gravity in such considerations. The non-perturbative component of the gravitational force seems to involve cut-and-paste procedures as dynamical features of space and time, of which the re-arrangement of space-time into two connected domains in the Penrose diagram is a primary example. Thus, we attempt to obtain new insights in the nature of particle interactions at the Planck scale, as well as quantum mechanics itself. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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31 pages, 527 KiB  
Article
Firewall from Effective Field Theory
by Pei-Ming Ho and Yuki Yokokura
Universe 2021, 7(7), 241; https://doi.org/10.3390/universe7070241 - 13 Jul 2021
Cited by 17 | Viewed by 2481
Abstract
For an effective field theory in the background of an evaporating black hole with spherical symmetry, we consider non-renormalizable interactions and their relevance to physical effects. The background geometry is determined by the semi-classical Einstein equation for an uneventful horizon where the vacuum [...] Read more.
For an effective field theory in the background of an evaporating black hole with spherical symmetry, we consider non-renormalizable interactions and their relevance to physical effects. The background geometry is determined by the semi-classical Einstein equation for an uneventful horizon where the vacuum energy–momentum tensor is small for freely falling observers. Surprisingly, after Hawking radiation appears, the transition amplitude from the Unruh vacuum to certain multi-particle states grows exponentially with time for a class of higher-derivative operators after the collapsing matter enters the near-horizon region, despite the absence of large curvature invariants. Within the scrambling time, the uneventful horizon transitions towards a firewall, and eventually the effective field theory breaks down. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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Review

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24 pages, 449 KiB  
Review
QCD Effective Locality: A Theoretical and Phenomenological Review
by Herbert M. Fried, Yves Gabellini, Thierry Grandou and Peter H. Tsang
Universe 2021, 7(12), 481; https://doi.org/10.3390/universe7120481 - 7 Dec 2021
Cited by 2 | Viewed by 2188
Abstract
About ten years ago, the use of standard functional manipulations was demonstrated to imply an unexpected property satisfied by the fermionic Green’s functions of QCD and dubbed Effective Locality. This feature of QCD is non-perturbative, as it results from a full gauge [...] Read more.
About ten years ago, the use of standard functional manipulations was demonstrated to imply an unexpected property satisfied by the fermionic Green’s functions of QCD and dubbed Effective Locality. This feature of QCD is non-perturbative, as it results from a full gauge invariant integration of the gluonic degrees of freedom. In this review article, a few salient theoretical aspects and phenomenological applications of this property are summarized. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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34 pages, 457 KiB  
Review
Real Clifford Algebras and Their Spinors for Relativistic Fermions
by Stefan Floerchinger
Universe 2021, 7(6), 168; https://doi.org/10.3390/universe7060168 - 28 May 2021
Cited by 6 | Viewed by 2516
Abstract
Real Clifford algebras for arbitrary numbers of space and time dimensions as well as their representations in terms of spinors are reviewed and discussed. The Clifford algebras are classified in terms of isomorphic matrix algebras of real, complex or quaternionic type. Spinors are [...] Read more.
Real Clifford algebras for arbitrary numbers of space and time dimensions as well as their representations in terms of spinors are reviewed and discussed. The Clifford algebras are classified in terms of isomorphic matrix algebras of real, complex or quaternionic type. Spinors are defined as elements of minimal or quasi-minimal left ideals within the Clifford algebra and as representations of the pin and spin groups. Two types of Dirac adjoint spinors are introduced carefully. The relationship between mathematical structures and applications to describe relativistic fermions is emphasized throughout. Full article
(This article belongs to the Special Issue Quantum Field Theory)
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