The FINUDA experiment performed a systematic study of the charged mesonic weak decay channel of $p$-shell $\Lambda$-hypernuclei. Negatively charged pion spectra from mesonic decay were measured with magnetic analysis for the first time for ${^{7}_{\Lambda}Li}$, ${^{9}_{\Lambda}Be}$, ${^{11}_{\Lambda}B}$ and ${^{15}_{\Lambda}N}$. The shape of the $\pi^{-}$ spectra was interpreted through a comparison with pion distorted wave calculations that take into account the structure of both hypernucleus and daughter nucleus. Branching ratios $\Gamma_{\pi^{-}}/\Gamma_{tot}$ were derived from the measured spectra and converted to $\pi^{-}$ decay rates $\Gamma_{\pi^{-}}$ by means of known or extrapolated total decay widths $\Gamma_{tot}$ of $p$-shell $\Lambda$-hypernuclei. Based on these measurements, the spin-parity assignment $1/2^+$ for ${^{7}_{\Lambda}Li}$ and $5/2^+$ for ${^{11}_{\Lambda}B}$ ground-state are confirmed and a spin-parity $3/2^+$ for ${^{15}_{\Lambda}N}$ ground-state is assigned for the first time.

New results on Mesonic Weak Decay of p-shell Lambda-Hypernuclei

BOTTA, Elena;BRESSANI, Tullio;BUFALINO, STEFANIA;BUSSO, Luigi;DE MORI, FRANCESCA;MARCELLO, Simonetta;
2009-01-01

Abstract

The FINUDA experiment performed a systematic study of the charged mesonic weak decay channel of $p$-shell $\Lambda$-hypernuclei. Negatively charged pion spectra from mesonic decay were measured with magnetic analysis for the first time for ${^{7}_{\Lambda}Li}$, ${^{9}_{\Lambda}Be}$, ${^{11}_{\Lambda}B}$ and ${^{15}_{\Lambda}N}$. The shape of the $\pi^{-}$ spectra was interpreted through a comparison with pion distorted wave calculations that take into account the structure of both hypernucleus and daughter nucleus. Branching ratios $\Gamma_{\pi^{-}}/\Gamma_{tot}$ were derived from the measured spectra and converted to $\pi^{-}$ decay rates $\Gamma_{\pi^{-}}$ by means of known or extrapolated total decay widths $\Gamma_{tot}$ of $p$-shell $\Lambda$-hypernuclei. Based on these measurements, the spin-parity assignment $1/2^+$ for ${^{7}_{\Lambda}Li}$ and $5/2^+$ for ${^{11}_{\Lambda}B}$ ground-state are confirmed and a spin-parity $3/2^+$ for ${^{15}_{\Lambda}N}$ ground-state is assigned for the first time.
2009
681
139
146
http://arxiv.org/abs/0905.0623
M. Agnello; A. Andronenkov; G. Beer; L. Benussi; M. Bertani; H.C. Bhang; G. Bonomi; E. Botta; M. Bregant; T. Bressani; S. Bufalino; L. Busso; D. Calvo; P. Camerini; B. Dalena; F. De Mori; G.D' Erasmo; F.L. Fabbri; A. Feliciello; A. Filippi; E.M. Fiore; A. Fontana; H. Fujioka; P. Genova; P. Gianotti; N. Grion; O. Hartmann; B. Kang; V. Lenti; V. Lucherini; S. Marcello; T. Maruta; N. Mirfakhrai; P. Montagna; O. Morra; T. Nagae; D. Nakajima; H. Outa; E. Pace; M. Palomba; A. Pantaleo; A. Panzarasa; V. Paticchio; S. Piano; F. Pompili; R. Rui; A. Sanchez Lorente; M. Sekimoto; G. Simonetti; A. Toyoda; R. Wheadon; A. Zenoni; A. Gal
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/100189
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