The branching fraction of the tau(-)-> 3h(-)2h(+)nu(tau) decay (h=pi,K) is measured with the BABAR detector to be (8.56 +/- 0.05 +/- 0.42)x10(-4), where the first error is statistical and the second systematic. The observed structure of this decay is significantly different from the phase space prediction, with the rho resonance playing a strong role. The decay tau(-)-> f(1)(1285)pi(-)nu(tau), with the f(1)(1285) meson decaying to four charged pions, is observed and the branching fraction is measured to be (3.9 +/- 0.7 +/- 0.5)x10(-4).

Study of the tau(-)-> 3h(-)2h(+)nu(tau) decay RID A-8798-2012 RID C-2728-2008 RID C-5223-2009 RID C-5719-2008 RID D-1055-2009 RID A-2675-2009

LUSIANI, Alberto;
2005

Abstract

The branching fraction of the tau(-)-> 3h(-)2h(+)nu(tau) decay (h=pi,K) is measured with the BABAR detector to be (8.56 +/- 0.05 +/- 0.42)x10(-4), where the first error is statistical and the second systematic. The observed structure of this decay is significantly different from the phase space prediction, with the rho resonance playing a strong role. The decay tau(-)-> f(1)(1285)pi(-)nu(tau), with the f(1)(1285) meson decaying to four charged pions, is observed and the branching fraction is measured to be (3.9 +/- 0.7 +/- 0.5)x10(-4).
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Utilizza questo identificativo per citare o creare un link a questo documento: http://hdl.handle.net/11384/4660
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