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Related papers: Amending the Vafa-Witten Theorem

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We consider the canonical quantization of an ordinary fluid. The resulting long-distance effective field theory is derivatively coupled, and therefore strongly coupled in the UV. The system however exhibits a number of peculiarities,…

High Energy Physics - Theory · Physics 2011-06-23 Solomon Endlich , Alberto Nicolis , Riccardo Rattazzi , Junpu Wang

In theories of Einstein gravity coupled with a dilaton and a two-form, a soft theorem for the two-form, known as the Kalb-Ramond B-field, has so far been missing. In this work we fill the gap, and in turn formulate a unified soft theorem…

High Energy Physics - Theory · Physics 2017-10-25 Paolo Di Vecchia , Raffaele Marotta , Matin Mojaza

We consider a confining Yang-Mills theory without Goldstone Bosons which could describe the bosonic sector of the weak interactions. This model can be gauge invariantly regularized on a lattice. A strong coupling analysis of the low lying…

High Energy Physics - Lattice · Physics 2009-10-22 A. Galli

In strongly magnetized backgrounds, electrically charged vector bosons can condense. When considering the rho-meson sector of QCD, this results in the existence of a superconducting state with Abrikosov vortices. As a next order effect,…

High Energy Physics - Phenomenology · Physics 2012-01-05 Jos Van Doorsselaere

We derive cosmological soft theorems for solids coupled to gravity. To this end, we first derive all cosmological adiabatic modes for solids, which display the interesting novelty of non-vanishing anisotropic stresses on large scales. Then,…

High Energy Physics - Theory · Physics 2019-06-12 Enrico Pajer , Sadra Jazayeri , Drian van der Woude

We consider diquark condensation in finite density lattice SU(2). We first present an extension of Vafa-Witten result, on spontaneous breaking of vector-like global symmetries, that allows us to formulate a no-go theorem for diquark…

High Energy Physics - Lattice · Physics 2009-10-31 R. Aloisio , V. Azcoiti , G. Di Carlo , A. Galante , A. F. Grillo

The massive Schwinger model in bosonic representation is quantized on the light front using the Dirac--Bergmann method. The non-perturbative theta- vacuum in terms of coherent states of the gauge-field zero mode is derived and found to…

High Energy Physics - Theory · Physics 2009-10-31 Lubomir Martinovic , James P. Vary

We adapt the Goldstone theorem to study spontaneous symmetry breaking in relativistic theo- ries at finite charge density. It is customary to treat systems at finite density via non-relativistic Hamiltonians. Here we highlight the…

High Energy Physics - Theory · Physics 2013-01-10 Alberto Nicolis , Federico Piazza

We argue that the Standard Model is accompanied by a new pseudo-scalar degree of freedom, $\eta_{\rm w}$-meson, which cancels the topological susceptibility of the electroweak vacuum and gets its mass from this effect. The prediction is…

High Energy Physics - Theory · Physics 2025-06-12 Gia Dvali , Archil Kobakhidze , Otari Sakhelashvili

Following previous work we further explore the possibility that the chirally broken phase of gauge theories admits an infrared fixed point interpretation. The slope of the $\beta$ function, $\beta'_*$, is found to vanish at the infrared…

High Energy Physics - Phenomenology · Physics 2025-08-26 Roman Zwicky

Large families of confining holographic QFTs, described by Einstein-Dilaton gravity, are considered on constant-curvature manifolds in the presence of a $\theta$-angle. The space of ground states of such theories is explored as a function…

High Energy Physics - Theory · Physics 2026-04-23 Ahmad Ghodsi , Elias Kiritsis , Francesco Nitti

On a null-plane (light-front), all effects of spontaneous chiral symmetry breaking are contained in the three Hamiltonians (dynamical Poincar\'e generators), while the vacuum state is a chiral invariant. This property is used to give a…

Nuclear Theory · Physics 2015-06-12 Silas R. Beane

According to a commonly held view of spontaneously broken symmetry in gauge theories, troublesome Nambu-Goldstone bosons are effectively eliminated by turning into longitudinal modes of a massive vector meson. This note shows that this is…

High Energy Physics - Theory · Physics 2015-06-18 G. S. Guralnik , C. R. Hagen

It is well-known that the square principle $\square_\lambda$ entails the existence of a non-reflecting stationary subset of $\lambda^+$, whereas the weak square principle $\square^*_\lambda$ does not. Here we show that if…

Logic · Mathematics 2017-11-17 Gunter Fuchs , Assaf Rinot

It is shown that the evaluation of the expectation value (EV) of topological charge density over $\theta$-vacuum is reduced to investigation of the Chern-Simons term EV. An equation for this quantity is established and solved. EV of the…

High Energy Physics - Theory · Physics 2007-05-23 A. M. Kotzinian , O. Yu. Shevchenko , A. N. Sissakian

We consider self-magnetization of charged and neutral vector bosons bearing a magnetic moment in a gas and in vacuum. For charged vector bosons (W bosons) a divergence of the magnetization in both the medium and the electroweak vacuum…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. Perez Rojas , E. Rodriguez Querts

We construct an approximate scheme based on the concept of the spontaneous symmetry breakdown, satisfying the Goldstone theorem, for finite volume Bose-Einstein condensed gases in both zero and finite temperature cases. In this paper, we…

Strongly Correlated Electrons · Physics 2009-11-11 Hiroaki Enomoto , Masahiko Okumura , Yoshiya Yamanaka

We describe a class of relativistic models incorporating finite density of matter in which spontaneous breakdown of continuous symmetries leads to a lesser number of Nambu-Goldstone bosons than that required by the Goldstone theorem. This…

High Energy Physics - Phenomenology · Physics 2011-07-19 V. A. Miransky , I. A. Shovkovy

Positivity bounds coming from consistency of UV scattering amplitudes are in general insufficient to prove the weak gravity conjecture for theories beyond Einstein-Maxwell. Additional ingredients about the UV may be necessary to exclude…

High Energy Physics - Theory · Physics 2020-11-20 Gregory J. Loges , Toshifumi Noumi , Gary Shiu

It is known that in order for a supersymmetric gauge theory to be dynamically broken a necessary but not sufficient condition is that the Witten index $(-1)^F=n_b^0-n_f^0$ is zero. In the case the Witten index is zero it is in general hard…

High Energy Physics - Phenomenology · Physics 2019-03-19 Renata Jora