Production of the X(3870) at the Upsilon(4S) by the Coalescence of Charm Mesons
arXiv:hep-ph/0402177 · doi:10.1103/PhysRevD.69.114012
Abstract
If the recently-discovered charmonium state X(3870) is a loosely-bound molecule of the charm mesons D^0 and \bar D^{*0} or \bar D^0 and D^{*0}, it can be produced in e^+ e^- annihilation at the Υ(4S) resonance by the coalescence of charm mesons produced in the decays of B^+ and B^- mesons. Remarkably, in the case of 2-body decays of the B mesons, the leading contribution to the coalescence probability depends only on hadron masses and on the width and branching fractions of the B meson. As the binding energy E_b of the molecule goes to zero, the coalescence probability scales as E_b^{1/2} log(E_b). Unfortunately, the coalescence probability is also suppressed by two powers of the ratio of the width to the mass of the B meson, and is therefore many orders of magnitude too small to be observed in current experiments at the B factories.
10 pages, revtex4, 1 figure
References in corpus (10)
- Observation of a narrow charmonium-like state in exclusive B+ -> K+ pi+pi- J/psi decays
- Observation of a New Narrow Charmonium State in Exclusive B+-->K+ pi+pi- J/psi Decays
- The D*0 D0bar threshold resonance
- Charmonium Options for the X(3872)
- Charmonium levels near threshold and the narrow state $X(3872) \to π^{+}π^{-}\jpsi$
- Low-energy Universality and the New Charmonium Resonance at 3870 MeV
- Interference and binding effects in decays of possible molecular component of X(3872)
- Molecular States of Heavy Quark Mesons
- On the hidden charm state at 3872 MeV
- The upper limit of the e+e- partial width of X(3872)
Cited by in corpus (35)
- The hidden-charm pentaquark and tetraquark states
- Non-Standard Heavy Mesons and Baryons, an Experimental Review
- The New Heavy Mesons: A Status Report
- Observation of a resonance-like structure in the pi^+- psi' mass distribution in exclusive B-->K pi^+- psi' decays
- QCD and strongly coupled gauge theories: challenges and perspectives
- Nuclear effective field theory: status and perspectives
- Observation of a near-threshold omega-J/psi mass enhancement in exclusive B-->K omega J/psi decays
- Observation of a charged (DD*bar)- mass peak in e+e- --> pi+ (DD*bar)- at Ecm=4.26 GeV
- Pion Interactions in the X(3872)
- Bounds on the width, mass difference and other properties of X(3872) --> pi+pi-J/psi decays
- Weak decays of heavy hadrons into dynamically generated resonances
- A New Hadron Spectroscopy
- Heavy quark spin selection rule and the properties of the X(3872)
- Exclusive Production of the X(3872) in B Meson Decay
- Production of the X(3872) in B Meson Decay by the Coalescence of Charm Mesons
- Factorization in the Production and Decay of the X(3872)
- On the scattering of D and D* mesons off the X(3872)
- A Phenomenological analysis on isospin-violating decay of
- Testing the molecular nature of and in semileptonic and decays
- Weakly-bound Hadronic Molecule near a 3-body Threshold
- AdS-QCD quark-antiquark potential, meson spectrum and tetraquarks
- X(3872) and the bound state problem of () in a chiral quark model
- Operator Product Expansion in the Production and Decay of the X(3872)
- Inclusive Production of the X(3872)
- Hadronic Atom as a Key to Revealing the Mystery
- Search for X(3872) in gamma gamma Fusion and ISR at CLEO
- Strategies for an accurate determination of the X(3872) energy from QCD lattice simulations
- Scalar and Vector 4Q Systems in Anisotropic Lattice QCD
- Lowest-lying Tetra-Quark Hadrons in Anisotropic Lattice QCD
- Search for the decay
- Dipion invariant mass spectrum in
- Search for X(3872) in gamma gamma Fusion and ISR at CLEO
- New Particles from Belle
- Schottky Anomaly and Hadronic Spectrum
- On the origin of the narrow peak and the isospin symmetry breaking of the (3872)