2003/09/27 by M.B. Voloshin, M. B. Voloshin · 269 citations
Chemistry · Physics and Astronomy · #Advanced Chemical Physics Studies #Atomic and Molecular Physics #Atomic physics #Chemistry #Coherence (philosophical gambling strategy) #Component (thermodynamics) #Crystallography #Hadron #Interference (communication) #Molecular Spectroscopy and Structure #Particle physics #Physics #Quantum mechanics #Resonance (particle physics) #Spectral line #Telecommunications #X(3872) #hep-ph
paper · pdf · doi:10.1016/j.physletb.2003.11.014
published in Physics Letters B 579(3-4), 316-320 (Elsevier BV) · 7 pages, 1 figure
arxiv created 2003/09/27 · openalex publication_date 2003/12/04 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
It is pointed out that the internal structure of the narrow resonance X(3872) at the D0D̄∗0 threshold can be studied in some detail by measuring the rate and the spectra in the decays X(3872)→D0D̄0π0 and X(3872)→D0D̄0γ. In particular, if this resonance contains a dominant “molecular” component DD∗̄±D̄D∗, this component can be revealed and studied by a distinct pattern of interference between the underlying decays of D∗0 and D̄∗0 whose coherence is ensured by fixed (but yet unknown) C parity of the X(3872).