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The weak decay of helium hypernuclei

Technical Report ·
DOI:https://doi.org/10.2172/6831977· OSTI ID:6831977

A [Lambda] hyperon replaces a neutron in a nucleus to form a hypernucleus via the [sup A]X(K[sup [minus]], [pi][sup [minus]]) [sub [Lambda]][sup A]X reaction at 750 MeV/c (Brookhaven Experiment 788). The free [Lambda] decay rates [Gamma]([Lambda] [yields] p[pi][sup [minus]]) and [Gamma]([Lambda] [yields] n[pi][sup 0]) are diminished due to Pauli blocking; but a non-mesonic decay mode, nucleon stimulated decay N[Lambda] [yields] Nn, is present and is detected via the energetic decay nucleon(s) ([approx] 400MeV/c). Measurements of the various hypernuclear decay rates [Gamma]([Lambda] [yields] p[pi][sup [minus]]), [Gamma]([Lambda] [yields] n[pi][sup 0]) and [Gamma]([Lambda]n [yields] nn) provides insight into the strong modification of the weak interaction such as the baryon-baryon [Delta]I =[1/2] rule. The hypernuclear state is isolated by momentum analysis of (K[sup [minus]], [pi][sup [minus]]) target reaction. Out-of-beam large volume scintillation detectors and tracking chambers axe used to make particle identification of the hypernuclear decay products by time-of-flight, dE/dx, and range. The kinetic energy of the decay neutrons are measured by time of flight using the large volume 100 element neutron detector system. The hypernuclear lifetime is directly measured using precision scintillator counters and tracking chambers. Measurements of the various decay rates as well as the total lifetime are discussed for [sub [Lambda]][sup 4]He.

Research Organization:
Carnegie-Mellon Univ., Pittsburgh, PA (United States)
Sponsoring Organization:
DOE; USDOE, Washington, DC (United States)
DOE Contract Number:
FG02-87ER40315
OSTI ID:
6831977
Report Number(s):
DOE/ER/40315-196; ON: DE93003650
Country of Publication:
United States
Language:
English