Resonant substructure in K sup minus. pi. sup +. pi. sup +. pi. sup minus decays of D sup 0 mesons
We determine the resonant substructure of {ital D}{sup 0}{r arrow}{ital K}{sup {minus}}{pi}{sup +}{pi}{sup +}{pi}{sup {minus}} decays using a five-dimensional maximum-likelihood technique to extract the relative fractions and phases of the amplitudes contributing to this final state. We find that tw...
Gespeichert in:
Veröffentlicht in: | Physical review letters 1990-05, Vol.64:22 |
---|---|
Hauptverfasser: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | We determine the resonant substructure of {ital D}{sup 0}{r arrow}{ital K}{sup {minus}}{pi}{sup +}{pi}{sup +}{pi}{sup {minus}} decays using a five-dimensional maximum-likelihood technique to extract the relative fractions and phases of the amplitudes contributing to this final state. We find that two-body decay modes account for at least 76% of all decays. We obtain branching ratios for several decay modes including {ital B}({ital D}{sup 0}{r arrow}{ital K}{sup {minus}}{ital a}{sub 1}{sup +}) =(9.0{plus minus}0.9{plus minus}1.7)%, {ital B}({ital D}{sup 0}{r arrow}{ital {bar K}} {sup *0}{rho}{sup 0})=(1.9{plus minus}0.3{plus minus}0.7)%, and {ital B}({ital D}{sup 0}{r arrow}{ital K}{sub 1}(1270){sup {minus}}{pi}{sup +}) =(1.8{plus minus}0.5 {plus minus}0.8)%. For the decay mode {ital D}{sup 0}{r arrow}{ital {bar K}} {sup *0}{rho}{sup 0}, the {ital {bar K}} {sup *0} and {rho}{sup 0} are found to be polarized with their spins oriented in the direction of their motion as seen from the {ital D}{sup 0} frame. |
---|---|
ISSN: | 0031-9007 1079-7114 |
DOI: | 10.1103/PhysRevLett.64.2615 |