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Related papers: X (3872) as a Universal and Composite State

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The $X(3872)$ could be a shallow $D\bar D^*$ bound state, a compact four-quark state, or a partially composite particle, i.e. a superposition of the two. We will review how these hypotheses could be tested experimentally, examining…

High Energy Physics - Phenomenology · Physics 2025-06-11 Angelo Esposito , Alfredo Glioti , Davide Germani , Antonio D. Polosa

From a study of the lineshape of the $X(3872)$, the LHCb collaboration measures a sizeable negative effective range. This cannot be reconciled with a shallow $D\bar{D}^*$ bound state hypothesis. Based on Weinberg's compositeness criterion,…

High Energy Physics - Phenomenology · Physics 2022-02-23 Angelo Esposito , Luciano Maiani , Alessandro Pilloni , Antonio D. Polosa , Veronica Riquer

The $X(3872)$ resonance has been conjectured to be a $J^{PC} = 1^{++}$ charm meson-antimeson two-body molecule. Meanwhile, there is no experimental evidence for larger, few-body compounds of multiple charm meson-antimeson pairs which would…

High Energy Physics - Phenomenology · Physics 2021-03-05 Lorenzo Contessi , Johannes Kirscher , Manuel Pavon Valderrama

The compositeness $X$ is defined as the probability to observe the composite structure such as the hadronic molecule component in a bound state. One of the model-independent approaches to calculate $X$ is the weak-binding relation. However,…

High Energy Physics - Phenomenology · Physics 2022-11-30 Tomona Kinugawa , Tetsuo Hyodo

We present in this talk a series of new results on the nature of a bound state or resonance based on the calculation of the expectation values of the number operators of the free particles in the state of interest. In this way, a new…

High Energy Physics - Phenomenology · Physics 2017-11-30 J. A. Oller

The unusual properties of the X(3872) have led to speculation that it is a weakly bound state of mesons, chiefly $D^0\bar D^{0*}$. Tests of this hypothesis are investigated and it is proposed that measuring the $3\pi J/\psi$, $\gamma…

High Energy Physics - Phenomenology · Physics 2008-11-26 Eric S. Swanson

The concept of a superposition is a revolutionary novelty introduced by Quantum Mechanics. If a system may be in any one of two pure states x and y, we must consider that it may also be in any one of many superpositions of x and y. An…

Quantum Physics · Physics 2008-04-07 Daniel Lehmann

Because of the controversial X(3872) meson's very close proximity to the $D^0\bar{D}^{*0}$ threshold, this charmonium-like resonance is often considered a meson-meson molecule. However, a molecular wave function must be essentially of a…

High Energy Physics - Phenomenology · Physics 2012-11-06 S. Coito , G. Rupp , E. van Beveren

The momentum space zero-range model is used to investigate universal properties of three interacting particles confined to two dimensions. The pertinent equations are first formulated for a system of two identical and one distinct particle…

Quantum Gases · Physics 2011-10-04 F. F. Bellotti , T. Frederico , M. T. Yamashita , D. V. Fedorov , A. S. Jensen , N. T. Zinner

The concept of a modular value of an observable of a pre- and post-selected quantum system is introduced. It is similar in form and in some cases has a close connection to the weak value of an observable, but instead of describing an…

Quantum Physics · Physics 2011-05-17 Yaron Kedem , Lev Vaidman

The compositeness of weakly bound states is discussed using the effective field theory from the viewpoint of the low-energy universality. We introduce a model with coupling of the single-channel scattering to the bare state, and study the…

High Energy Physics - Phenomenology · Physics 2024-09-26 Tomona Kinugawa , Tetsuo Hyodo

In order to understand the structure of the X(3872), the $c \bar c$ charmonium core state coupling to the $D^0 \bar D^{\ast 0}$ and $D^+ D^{\ast -}$ molecular states are studied. The strengths of the couplings between the charmonium state…

High Energy Physics - Phenomenology · Physics 2014-05-07 Makoto Takizawa , Sachiko Takeuchi

The state of a quantum system, consisting of two distinct subsystems, is called separable if it can be prepared by two distant experimenters who receive instructions from a common source, via classical communication channels. A necessary…

Quantum Physics · Physics 2009-10-30 Asher Peres

The near-threshold exotic hadrons such as $T_{cc}$ and $X(3872)$ are naively considered as the hadronic molecular state from the viewpoint of the low-energy universality. However, it is also known that the elementary dominant state is not…

High Energy Physics - Phenomenology · Physics 2023-08-21 Tomona Kinugawa , Tetsuo Hyodo

The existing analyses on the X(3872) lineshape are consistent with the hypothesis that it is a compact particle composed of four quarks. This conclusion follows from fitting available data with a Flatte' distribution derived from an…

High Energy Physics - Phenomenology · Physics 2026-05-13 A. Carducci , G. Cianti , P. D'Annibali , D. Germani , A. D. Polosa

The composite nature of a shallow bound state is studied by using the weak-binding relation, which connects the compositeness of the bound state with observables. We first show that the previous weak-binding relation cannot be applied to…

High Energy Physics - Phenomenology · Physics 2022-07-21 Tomona Kinugawa , Tetsuo Hyodo

We search a simplest and minimal way to determine whether a given quantum system is entangled or separable. For this end, we propose binary correlation measurements in which restricted knowledge of only zero or non-zero correlations is…

Quantum Physics · Physics 2021-06-29 Toru Ohira

The motion of a composite system made of N particles is examined in a space with a canonical noncommutative algebra of coordinates. It is found that the coordinates of the center-of-mass position satisfy noncommutative algebra with…

General Relativity and Quantum Cosmology · Physics 2015-06-19 Kh. P. Gnatenko

A solvable coordinate-space model is employed to study the $c\bar{c}$ component of the X(3872) wave function, by coupling a confined $^3P_1$ $c\bar{c}$ state to the almost unbound $S$-wave $D^0\bar{D}^{*0}$ channel via the $^3P_0$…

High Energy Physics - Phenomenology · Physics 2015-06-12 Susana Coito , George Rupp , Eef van Beveren

Using the relation proposed by Weinberg in 1972, combining quantum and cosmological parameters, we prove that the self gravitational potential energy of any fundamental particle is a quantum, with physical properties independent of the mass…

General Physics · Physics 2012-01-17 Antonio Alfonso-Faus
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