4.7 Article

X(3872)'s excitation and its connection with production at hadron colliders

Journal

PHYSICAL REVIEW D
Volume 106, Issue 9, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.106.094004

Keywords

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Funding

  1. Ministerio Espanol de Ciencia e Innovacion [P18-FR-5057]
  2. Junta de Andalucia
  3. Operativo FEDER Andalucia [PAIDI FQM-205]
  4. [PID2019-107844GB-C22]
  5. [UHU-1264517]

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The LHCb collaboration has found that the production rate of X(3872) decreases as final state particle multiplicity increases in proton-proton collisions. The ALICE experiment at CERN has observed that the number of deuterons produced increases with multiplicity. Researchers have used a diffusion Monte Carlo method to analyze the structure of X(3872) and found that it resembles a light-meson-heavy-meson molecule. They have also computed the mass of the first color excited cc over bar qq over bar tetraquark state and found it to be around 4.0 GeV, a region where many new exotic candidates have been collected.
The LHCb collaboration has found that the production rate of X(3872) in proton-proton collisions decreases as final state particle multiplicity increases. Moreover, the ALICE experiment at CERN has observed that the number of deuterons produced increases with multiplicity, a behavior that is qualitatively different from that of the X(3872). These experimental findings may point to a compact structure for the X(3872) or, at least, that its hadronization could proceed through a charm-anticharm core. We have recently used a diffusion Monte Carlo method to solve the 4-body Schrodinger equation that describes the X(3872) as a cc over bar qq over bar tetraquark system with quantum numbers IG(JPC) = 0+(1++) and 1-(1++). According to our structural analysis, the quark-(anti)quark correlations resemble light-meson-heavy-meson molecules of type omega J=psi and rho J=psi, rather than the most extended D over bar D* interpretation. It was argued that this fact may be the key to make compatible the molecular features of the X(3872) with its production observables. The same formalism allows us to compute the first color excited cc over bar qq over bar tetraquark state with either IG(JPC) = 0+(1++) or 1-(1++). A bound-state is found in each channel, their masses are around 4.0 GeV which is an energy region where many new exotic candidates have been collected by the Particle Data Group. Concerning their structural properties, these states cluster in a compact diquark-antidiquark arrangement which matches perfectly with a so-called Born-Oppenheimer tetraquark configuration. The promptly production rates of these states in proton-proton, proton-nucleus and nucleus-nucleus collisions should fall off equal to or even faster than those of the X(3872).

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