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Related papers: Kaon Condensation and Goldstone's Theorem

200 papers

In non-relativistic systems, when there is spontaneous symmetry breaking, the number of Nambu-Goldstone bosons ($n_{NG}$) are not necessarily equal to the number of broken generators ($n_{BG}$). Here we use the method of operators for…

High Energy Physics - Theory · Physics 2017-08-01 Ivan Arraut

At the TeV scale, heavy quarks, for example the 4th generation quarks of the Standard Model with four generations, can form condensates which dynamically break the electroweak symmetry. A dense quark system may form other types of…

High Energy Physics - Phenomenology · Physics 2017-08-23 Chi Xiong

A new formulation is presented to treat thermal and quantum fluctuations around the kaon condensate on the basis of chiral symmetry; separating the zero-mode from the beginning and using the path-integral method, we can formulate the…

Nuclear Theory · Physics 2009-10-31 Toshitaka Tatsumi , Masatomi Yasuhira

We show that QCD Dirac spectra well below Lambda_{QCD}, both at zero and at nonzero chemical potential, can be obtained from a chiral Lagrangian. At nonzero chemical potential Goldstone bosons with nonzero baryon number condense beyond a…

High Energy Physics - Theory · Physics 2017-08-23 D. Toublan , J. J. M. Verbaarschot

We formulate the equivalence between the longitudinal weak-boson and the Goldstone boson as a criterion for sensitively probing the electroweak symmetry breaking mechanism and develop a precise power counting rule for chiral Lagrangian…

High Energy Physics - Phenomenology · Physics 2008-02-03 Hong-Jian He , Yu-Ping Kuang , C. -P. Yuan

In the limit of vanishing up, down and strange quark masses, QCD exhibits a chiral symmetry. This symmetry is broken spontaneously to its vector subgroup, giving rise to Goldstone bosons. These acquire a small mass through the explicit…

High Energy Physics - Phenomenology · Physics 2024-12-31 Ulf-G. Meißner

We present recent results in three-flavor chiral perturbation theory at finite isospin $\mu_I$ and strangeness $\mu_s$ chemical potentials at zero temperature. The phase diagram to ${\cal O}(p^2)$ in the $\mu_I$--$\mu_S$ plane is mapped out…

High Energy Physics - Phenomenology · Physics 2025-02-11 Jens O. Andersen , Martin Kjøllesdal Johnsrud , Qing Yu , Hua Zhou

The propagation of low-momentum baryons through QCD matter at low isospin density is studied using chiral perturbation theory. When the isospin chemical potential exceeds a critical value, the dispersion relation for the lowest nucleon mode…

High Energy Physics - Phenomenology · Physics 2009-11-07 Michael C. Birse , Thomas D. Cohen , Judith A. McGovern

As the number of fermion fields is increased, gauge theories are expected to undergo a transition from a QCD-like phase, characterised by confinement and chiral symmetry breaking, to a conformal phase, where the theory becomes…

High Energy Physics - Phenomenology · Physics 2022-10-14 Luigi Del Debbio , Roman Zwicky

We study the thermodynamic properties of matter at vanishing temperature for non-extreme values of the isospin chemical potential and of the strange quark chemical potential. From the leading order pressure obtained by maximizing the static…

High Energy Physics - Phenomenology · Physics 2016-04-06 Stefano Carignano , Andrea Mammarella , Massimo Mannarelli

An overview is presented of the talks in the working group on Goldstone Bosons. Topics touched on are CP-violation in the Kaon system, rare Kaon decays, $\pi\pi$-scattering, $\phi$-meson decays, scalar mesons, form-factors and…

High Energy Physics - Phenomenology · Physics 2017-08-23 Johan Bijnens , Ada Farilla , Rory Miskimen

The phenomenon of spontaneous symmetry breaking is well known. It is known to be accompanied with the appearance of the `Goldstone boson'. In this paper we construct the canonical coordinates of the Goldstone boson, for quantum spin systems…

Mathematical Physics · Physics 2009-10-31 T. Michoel , A. Verbeure

We study pion and kaon condensation using three-flavor chiral perturbation theory at finite isospin and strangeness quark chemical potentials {\mu}I and {\mu}S . The phase diagram consists of a vacuum phase and three distinct Bose condensed…

High Energy Physics - Phenomenology · Physics 2022-06-10 Jens O. Andersen , Martin Kjøllesdal Johnsrud

Kaon condensation may play an important role in the structure of hadronic matter at densities greater than that of nuclear matter, as exist in the interior of neutron stars. We present the results of the first lattice QCD investigation of…

High Energy Physics - Lattice · Physics 2008-11-26 William Detmold , Kostas Orginos , Martin J. Savage , Andre Walker-Loud

A mechanism of spontaneous conformal symmetry breaking based on field condensates in the Standard Model of strong and electroweak interactions is suggested. It is shown that an existence of the top quark condensate can supersede the tachyon…

High Energy Physics - Phenomenology · Physics 2013-01-17 V. N. Pervushin , A. B. Arbuzov , R. G. Nazmitdinov , A. E. Pavlov , A. F. Zakharov

Bose condensation is central to our understanding of quantum phases of matter. Here we review Bose condensation in topologically ordered phases (also called topological symmetry breaking), where the condensing bosons have non-trivial mutual…

Strongly Correlated Electrons · Physics 2018-05-23 F. J. Burnell

We study QCD-like theories with pseudoreal fermions at finite baryon density. Such theories include two-color QCD with quarks in the fundamental representation of the color group as well as any-color QCD with quarks in the adjoint color…

High Energy Physics - Phenomenology · Physics 2009-10-31 J. B. Kogut , M. A. Stephanov , D. Toublan , J. J. M. Verbaarschot , A. Zhitnitsky

We consider nonrelativistic superfluids where the global U(1)-symmetry is spontaneously broken. At sufficiently long wavelengths, the relevant degree of freedom is the massless Goldstone mode and we construct an effective low energy theory…

Condensed Matter · Physics 2007-05-23 Jens O. Andersen

We have simulated two-colour four-flavour QCD at non-zero chemical potential $\mu$ for quark number. Simulations were performed on $8^4$ and $12^3 \times 24$ lattices. Clear evidence was seen for the formation of a colourless diquark…

High Energy Physics - Lattice · Physics 2014-11-17 J. B. Kogut , D. K. Sinclair , S. J. Hands , S. E. Morrison

We study the Higgs condensation $H={\bar t}t$ mechanism in the Top-mode Standard Model at the next-to-leading order in 1/Nc. The calculation includes the effects of the Goldstone fields, but not the effects of the transverse components of…

High Energy Physics - Phenomenology · Physics 2009-10-28 G. Cvetic , N. D. Vlachos