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Related papers: Comment on "Hybridized Tetraquarks"

200 papers

Recently we formulated covariant equations describing the tetraquark in terms of an admixture of two-body states $D\bar D$ (diquark-antidiquark), $MM$ (meson-meson), and three-body-like states where two of the quarks are spectators while…

High Energy Physics - Phenomenology · Physics 2024-04-22 B. Blankleider , A. N. Kvinikhidze

Additional broader I=0 states in the KN channel near $\Theta^+$(1540) are expected in many models, making the absence of any signature in the K$^+$-deuteron scattering data even more puzzling. In an ideal "three-body" picture the $\Theta$…

High Energy Physics - Phenomenology · Physics 2009-11-10 Shmuel Nussinov

We introduce the semiring of values $\Gamma$ with respect to the tropical operations associated to an algebroid curve. As a set, $\Gamma$ determines and is determined by the well known semigroup of values $S$ and we prove that $\Gamma$ is…

Algebraic Geometry · Mathematics 2018-02-22 Emilio Carvalho , Marcelo Escudeiro Hernandes

Let $\Gamma$ be a finitely presented group and $G$ a linear algebraic group over $\mathbb{R}$. A representation $\rho:\Gamma\rightarrow G(\mathbb{R})$ can be seen as an $\mathbb{R}$-point of the representation variety $\mathfrak{R}(\Gamma,…

Algebraic Geometry · Mathematics 2015-09-10 Louis-Clément Lefèvre

We prove a $\Gamma$-convergence result for space dependent weak membrane energies, that is for 'truncated quadratic potentials', that are quadratic below some threshold (depending on the pair of points that we are considering) and constant…

Analysis of PDEs · Mathematics 2018-01-10 Leonard Kreutz

Assuming X(3872) is a $qc \bar q \bar c$ tetraquark and using its mass as input, we perform a schematic study of the masses of possible heavy tetraquarks using the color-magnetic interaction with the flavor symmetry breaking corrections.

High Energy Physics - Phenomenology · Physics 2008-11-26 Ying Cui , Xiao-Lin Chen , Wei-Zhen Deng , Shi-Lin Zhu

We derive covariant equations describing the tetraquark in terms of an admixture of two-body states $D\bar D$ (diquark-antidiquark), $MM$ (meson-meson), and three-body-like states $q\bar q (T_{q\bar q})$, $q q (T_{\bar q\bar q})$, and $\bar…

High Energy Physics - Phenomenology · Physics 2023-05-24 A. N. Kvinikhidze , B. Blankleider

Doubled $\alpha'$-geometry is the simplest higher-derivative gravitational theory with exact global duality symmetry. We use the double metric formulation of this theory to compute on-shell three-point functions to all orders in $\alpha'$.…

High Energy Physics - Theory · Physics 2016-06-08 Usman Naseer , Barton Zwiebach

We present first results on the axial and pseudoscalar $\Delta$ form factors. The analysis is carried out in the quenched approximation where statistical errors are small and the lattice set-up can be investigated relatively quickly. We…

High Energy Physics - Lattice · Physics 2011-03-22 Constantia Alexandrou , Eric B. Gregory , Tomasz Korzec , Giannis Koutsou , John Negele , Toru Sato , Antonios Tsapalis

The masses of the excited heavy tetraquarks with hidden charm are calculated within the relativistic diquark-antidiquark picture. The dynamics of the light quark in a heavy-light diquark is treated completely relativistically. The diquark…

High Energy Physics - Phenomenology · Physics 2008-12-18 D. Ebert , R. N. Faustov , V. O. Galkin

The relationship between the refractive index decrement, $\delta$, and the real part of the atomic form factor, $f^\prime$, is used to derive a simple polynomial functional form for $\delta(E)$ far from the K-edge of the element. The…

Classical Physics · Physics 2023-06-29 Saransh Singh , K. Aditya Mohan

We propose a new interpretation of the neutral and charged X, Z exotic hadron resonances. Hybridized-tetraquarks are neither purely compact tetraquark states nor bound or loosely bound molecules. The latter would require a negative or zero…

High Energy Physics - Phenomenology · Physics 2016-05-18 A. Esposito , A. Pilloni , A. D. Polosa

Consider a partial flag variety $X$ which is not a grassmaninan. Consider also its cohomology ring ${\rm H}^*(X,\ZZ)$ endowed with the base formed by the Poincar\'e dual classes of the Schubert varieties. In \cite{Richmond:recursion}, E.…

Algebraic Geometry · Mathematics 2008-12-12 Nicolas Ressayre

If connecting properties of a multiquark hadron with those exhibited by its constituents, QCD sum rules inferred along the routes of traditional wisdom necessarily involve contributions not related at all to and thus not presenting…

High Energy Physics - Phenomenology · Physics 2022-06-16 Wolfgang Lucha , Dmitri Melikhov , Hagop Sazdjian

It is shown that some formulae describing optical rotatory dispersion of $\alpha$-quartz with the aid of two Drude's terms reduce to the combined formula containing one Drude's and one Chandrasekhar's term. Comparison of various formulae…

Materials Science · Physics 2007-05-23 V. Vysin , I. Vysin

Let $\Gamma$ be a countable group and $(X, \Gamma)$ a compact topological dynamical system. We study the question of the existence of an intermediate $C^*$-subalgebra $\mathcal{A}$ $$C^{*}_{r}(\Gamma)<\mathcal{A}<C(X)\rtimes_r\Gamma,$$…

Operator Algebras · Mathematics 2024-04-16 Tattwamasi Amrutam , Eli Glasner , Yair Glasner

We present new linear relations among the masses of S-wave tetraquarks with either one flavour ($QQ \bar Q \bar Q$) or two ($QQ\bar q \bar q$). Because the relations are sensitive to the hidden-colour, spin, and spatial degrees of freedom,…

High Energy Physics - Phenomenology · Physics 2023-12-01 Muhammad Naeem Anwar , Timothy J. Burns

We prove an approximation result showing how operators of the type $-\Delta -\gamma \delta (x-\Gamma)$ in $L^2(\mathbb{R}^2)$, where $\Gamma$ is a graph, can be modeled in the strong resolvent sense by point-interaction Hamiltonians with an…

Mathematical Physics · Physics 2020-01-28 P. Exner , K. Nemcova

We propose a formula constructed out of elementary functions that captures many of the detailed features of the transverse resistivity $\rho_{xy}$ for the integer quantum Hall effect. It is merely a phenomenological formula in the sense…

Mesoscale and Nanoscale Physics · Physics 2024-03-01 André LeClair

Partial dynamical systems (X,alpha) arise naturally when dealing with commutative C*-dynamical system (A,delta). We associate with every pair (X,alpha), or (A,delta), a covariance C*-algebra C*(X,alpha)=C*(A,delta) which agrees with a…

Operator Algebras · Mathematics 2007-05-23 B. K. Kwasniewski