LCSR analysis of compact pentaquarks yields μ_u/μ_d = -2 for all currents and μ_c = 0 for one current, with numerical moments of order 1-3 μ_N that differ in flavor decomposition from molecular calculations.
Aaij, et al., Evidence for a new structure in theJ/ψpandJ/ψ¯psystems inB0 s →J/ψp¯pdecays, Phys
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Hadron ratios for J/Ψ, Ψ(2S) and X(3872) are linked to the separation and dissociation of in-medium c cbar pairs through Fermi Golden rule overlaps between in-vacuum and in-medium wave functions.
Fully heavy pentaquark fragmentation functions PQ5Q1.0 are completed for charm and bottom flavors and used to compute NLL/NLO+ semi-inclusive production rates at future colliders.
This review summarizes the historical motivation, detector design, experimental techniques, and major physics results of the LHCb experiment at the LHC.
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Analytic electromagnetic signatures of compact pentaquark structure: A multi-current QCD light-cone sum rules analysis of the $P_{\psi s}^{\Lambda}$ states
LCSR analysis of compact pentaquarks yields μ_u/μ_d = -2 for all currents and μ_c = 0 for one current, with numerical moments of order 1-3 μ_N that differ in flavor decomposition from molecular calculations.
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Hadronisation of in-medium $c\bar c$ pairs to the exotic $X(3872)$
Hadron ratios for J/Ψ, Ψ(2S) and X(3872) are linked to the separation and dissociation of in-medium c cbar pairs through Fermi Golden rule overlaps between in-vacuum and in-medium wave functions.
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Fully Heavy Pentaquarks with JETHAD: A High-Energy Viewpoint
Fully heavy pentaquark fragmentation functions PQ5Q1.0 are completed for charm and bottom flavors and used to compute NLL/NLO+ semi-inclusive production rates at future colliders.
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The LHCb Experiment
This review summarizes the historical motivation, detector design, experimental techniques, and major physics results of the LHCb experiment at the LHC.