Determination of the Parity of the Neutral Pion via the Four-Electron Decay
| dc.creator | Abouzaid, E. | |
| dc.creator | Arenton, M. | |
| dc.creator | Barker, A. R. | |
| dc.creator | Bellantoni, L. | |
| dc.creator | Blucher, E. | |
| dc.creator | Bock, G. J. | |
| dc.creator | Cheu, E. | |
| dc.creator | Coleman, R. | |
| dc.creator | Corcoran, M. D. | |
| dc.creator | Cox, B. | |
| dc.creator | Erwin, A. R. | |
| dc.creator | Escobar, C. O. | |
| dc.creator | Glazov, A. | |
| dc.creator | Golossanov, A. | |
| dc.creator | Gomes, R. A. | |
| dc.creator | Gouffon, P. | |
| dc.creator | Hsiung, Y. B. | |
| dc.creator | Jensen, D. A. | |
| dc.creator | Kessler, R. | |
| dc.creator | Kotera, K. | |
| dc.creator | Ledovskoy, A. | |
| dc.creator | McBride, P. L. | |
| dc.creator | Monnier, E. | |
| dc.creator | Nguyen, H. | |
| dc.creator | Niclasen, R. | |
| dc.creator | Phillips II, D. G. | |
| dc.creator | Ramberg, E. J. | |
| dc.creator | Ray, R. E. | |
| dc.creator | Ronquest, M. | |
| dc.creator | Santos, E. | |
| dc.creator | Slater, W. | |
| dc.creator | Smith, D. | |
| dc.creator | Solomey, N. | |
| dc.creator | Swallow, E. C. | |
| dc.creator | Toale, P. A. | |
| dc.creator | Tschirhart, R. | |
| dc.creator | Wah, Y. W. | |
| dc.creator | Wang, J. | |
| dc.creator | White, H. B. | |
| dc.creator | Whitmore, J. | |
| dc.creator | Wilking, M. J. | |
| dc.creator | Winstein, B. | |
| dc.creator | Winston, R. | |
| dc.creator | Worcester, E. T. | |
| dc.creator | Yamanaka, T. | |
| dc.creator | Zimmerman, E. D. | |
| dc.creator | Zukanovich, R. F. | |
| dc.date | 2008-02-14 | |
| dc.date | 2008-05-11 | |
| dc.date.accessioned | 2026-07-07T13:04:34Z | |
| dc.date.available | 2026-07-07T13:04:34Z | |
| dc.description | We present a new determination of the parity of the neutral pion via the double Dalitz decay pi^0 -> e+ e- e+ e-. Our sample, which consists of 30511 candidate decays, was collected from K_L -> pi0 pi0 pi0 decays in flight at the KTeV-E799 experiment at Fermi National Accelerator Laboratory. We confirm the negative pi^0 parity, and place a limit on scalar contributions to the pi^0 -> e+ e- e+ e- decay amplitude of less than 3.3% assuming CPT conservation. The pi^0 gamma* gamma* form factor is well described by a momentum-dependent model with a slope parameter fit to the final state phase space distribution. Additionally, we have measured the branching ratio of this mode to be B(pi^0 -> e+ e- e+ e-) = (3.26 +- 0.18) x 10^(-5). | |
| dc.description | 5 pages, 4 figures. Typographical error in radiative branching ratio (Eq. 6) corrected | |
| dc.identifier | https://arxiv.org/abs/0802.2064 | |
| dc.identifier | http://arxiv.org/abs/0802.2064 | |
| dc.identifier | Phys.Rev.Lett.100:182001,2008 | |
| dc.identifier | doi:10.1103/PhysRevLett.100.182001 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/227208 | |
| dc.subject | High Energy Physics - Experiment | |
| dc.title | Determination of the Parity of the Neutral Pion via the Four-Electron Decay | |
| dc.type | text |