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Related papers: Holographic Penta and Hepta Quark State in Confini…

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With the construction of the Witten-Sakai-Sugimoto model in the D0-D4 background, we systematically investigate the holographic baryon spectrum in the case of three flavors. The background geometry in this model is holographically dual to…

High Energy Physics - Theory · Physics 2018-06-06 Wenhe Cai , Si-wen Li

If the Theta^+(1540) is interpreted as a bound state of a $\bar s$ quark and two (ud) diquarks in a relative P-wave, then it is very likely that there exist pentaquark states with a heavy antiquark, $\bar b$ or $\bar c$, and two ``light''…

High Energy Physics - Phenomenology · Physics 2010-04-05 Iain W. Stewart , Margaret E. Wessling , Mark B. Wise

We study $\textrm{AdS}_2\times S^4 \times S^2 \times \Sigma_2$ solutions in type IIB string theory arising from D1 -- D3 -- NS5 brane intersections. These backgrounds enjoy sixteen supercharges and the corresponding internal geometry is…

High Energy Physics - Theory · Physics 2020-01-22 Giuseppe Dibitetto , Yolanda Lozano , Nicolò Petri , Anayeli Ramirez

I call attention to the possibility that QCD bound states (hadrons) could be derived using rigorous Hamiltonian, perturbative methods. Solving Gauss' law for $A^0$ with a non-vanishing boundary condition at spatial infinity gives an…

High Energy Physics - Phenomenology · Physics 2015-06-22 Paul Hoyer

We construct a new NS5-brane solution in AdS_4 x CP^3 with S^2 x S^3 topology. This solution belongs to the general class of non-Einstein N_{11} metrics to which T^{1,1} belongs, and carries a non-vanishing D0-brane charge. In eleven…

High Energy Physics - Theory · Physics 2015-06-15 Yolanda Lozano , Andrea Prinsloo

We analyze the phases of the Sakai-Sugimoto model at finite temperature and baryon chemical potential. Baryonic matter is represented either by 4-branes in the 8-branes or by strings stretched from the 8-branes to the horizon. We find the…

High Energy Physics - Theory · Physics 2009-03-04 Oren Bergman , Gilad Lifschytz , Matthew Lippert

The classical quenched quark models with three constituent quarks provide a good description for the baryon spatial ground states, but fail to reproduce the spectrum of baryon excited states. More and more evidences suggest that unquenched…

Nuclear Theory · Physics 2016-06-22 Jia-Jun Wu , B. S. Zou

The strange-anticharmed Pentaquark is a $uud\bar{c}s$ or $udd\bar{c}s$ five-quark baryon that is expected to be either a narrow resonance, or possibly even stable against strong and electromagnetic decay. We describe this hyperon here, its…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. A. Moinester , D. Ashery , L. G. Landsberg , H. J. Lipkin

In this work, we analyze a class of Yang-Mills models containing adjoint Higgs fields, with SU(N) symmetry spontaneously broken down to Z(N), showing they contain center vortices, Y-junctions formed by them, and junctions where different…

High Energy Physics - Theory · Physics 2013-03-14 L. E. Oxman

The correspondence between theories in anti-de Sitter space and conformal field theories in physical space-time leads to an analytic, semiclassical model for strongly-coupled QCD which has scale invariance at short distances and color…

High Energy Physics - Phenomenology · Physics 2014-08-27 Stanley J. Brodsky , Guy de Teramond , Robert Shrock

The complex nonperturbative color-confining dynamics of QCD is well captured in a semiclassical effective theory based on superconformal quantum mechanics and its extension to the light-front. I describe here how this new approach to hadron…

High Energy Physics - Theory · Physics 2016-03-23 Guy F. de Teramond

A D5 brane winding around a stack of D3 branes can be used as a model of persistent current in a thin superconducting ring, with the number N of D3s corresponding to the number of transverse channels in the ring. We consider, in the large N…

High Energy Physics - Theory · Physics 2015-06-11 Sergei Khlebnikov

We study the charmed and bottomed doubly strange baryons within the heavy-quark-light-diquark framework. The two strange quarks are assumed to lie in $S$ wave and thus their total spin is 1. We calculate the mass spectra of the $S$ and $P$…

High Energy Physics - Phenomenology · Physics 2017-08-02 Wei Wang , Rui-Lin Zhu

It is not understood whether scale-separated AdS vacua in string theory admit a holographic dual. A well-known class of such vacua is provided by the DGKT solutions of massive type IIA string theory, where scale separation arises from large…

High Energy Physics - Theory · Physics 2026-01-22 Fien Apers

An AdS_4 brane embedded in AdS_5 exhibits the novel feature that a four-dimensional graviton is localized near the brane, but the majority of the infinite bulk away from the brane where the warp factor diverges does not see four-dimensional…

High Energy Physics - Theory · Physics 2009-11-07 Raphael Bousso , Lisa Randall

In this paper, we study properties of baryons by using a holographic dual of QCD on the basis of the D4/D8-brane configuration, where baryons are described by a soliton. We first determine the asymptotic behavior of the soliton solution,…

High Energy Physics - Theory · Physics 2010-03-04 Koji Hashimoto , Tadakatsu Sakai , Shigeki Sugimoto

We consider the cosmology of a pair of domain walls bounding a five-dimensional bulk space-time with negative cosmological constant, in which the distance between the branes is not fixed in time. Although there are strong arguments to…

High Energy Physics - Theory · Physics 2009-09-15 Justin Khoury , Paul J. Steinhardt , Daniel Waldram

Early studies proposed a connection between cuprate superconductivity and fractionalized spin liquid states. But the low temperature phase diagram is dominated by states without fractionalization, with a competition between…

Strongly Correlated Electrons · Physics 2025-05-23 Maine Christos , Zhu-Xi Luo , Henry Shackleton , Ya-Hui Zhang , Mathias Scheurer , Subir Sachdev

We present a coupled channel unitary approach to obtain states dynamically generated from the meson baryon interaction with hidden charm, using constraints of heavy quark spin symmetry. We use as basis of states, $\bar D B$, $\bar D^* B$…

High Energy Physics - Phenomenology · Physics 2013-09-18 C. W. Xiao , J. Nieves , E. Oset

The penta-quark(5Q) Theta^+(1540) is studied in anisotropic lattice QCD with renormalized anisotropy a_s/a_t=4 for a high-precision measurement. Both the positive and the negative parity 5Q baryons are studied using a non-NK type…

High Energy Physics - Lattice · Physics 2009-11-10 N. Ishii , T. Doi , H. Iida , M. Oka , F. Okiharu , H. Suganuma