| dc.contributor.author | Ammar, Raymond G. | |
| dc.contributor.author | Ball, S. | |
| dc.contributor.author | Baringer, Philip S. | |
| dc.contributor.author | Coppage, Don | |
| dc.contributor.author | Copty, N. | |
| dc.contributor.author | Davis, Robin E. P. | |
| dc.contributor.author | Hancock, N. | |
| dc.contributor.author | Kelly, M. | |
| dc.contributor.author | Kwak, Nowhan | |
| dc.contributor.author | Lam, H. | |
| dc.date.accessioned | 2007-04-14T10:05:00Z | |
| dc.date.available | 2007-04-14T10:05:00Z | |
| dc.date.issued | 1993-09 | |
| dc.identifier.citation | SELEN, M, SADOFF, AJ, et al. Measurement of the D -> pipi branching fractions. PHYSICAL REVIEW LETTERS. September 1993. 71(13) : 1973-1977 | |
| dc.identifier.uri | http://hdl.handle.net/1808/1475 | |
| dc.description.abstract | Using data from CLEO II at the Cornell Electron Storage Ring we provide a new measurement of the branching fraction for D0 --> pi+pi-, and we present the first measurements of D0 --> pi0pi0 and of D+ --> pi+pi0, which is due to an isospin changing DELTAI = 3/2 transition. From these data we extract the ratio of isospin amplitudes \A2/A0\, and the cosine of the relative phase delta = delta2 - delta0 between these amplitudes, for D --> pipi decays. Unlike the situation in kaon decay where A2 is strongly suppressed, we find \A2/A0\ = 0.72 +/- 0.13 +/- 0.11 and cos delta = 0.14 +/- 0.13 +/- 0.09. | |
| dc.language.iso | en_US | |
| dc.publisher | AMERICAN PHYSICAL SOC | |
| dc.title | Measurement of the D -> pipi branching fractions | |
| dc.type | Article | |
| dc.identifier.doi | 10.1103/PhysRevLett.71.1973 | |
| dc.rights.accessrights | openAccess | |
