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INDC(IND)-35G - IAEA Nuclear Data Services

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- 4 -<br />

ANGULAR DISTRIBUTION OF POLAR LIGHT CHARGED PARTICLES IN<br />

THERMAL NEUTRON-<strong>IND</strong>UCBD FISSION OP 235<br />

M.M. ahanna, A.K. Sinha and G.K.. Mehta<br />

Indian Institute of Technology, Kanpur-208016,<strong>IND</strong>IA<br />

D.M. Nadfcarnl<br />

Bhabha Atomic Research Centre, Bombay-400085, <strong>IND</strong>IA*<br />

The angular distribution of polar ligfc* cLar^ed particles<br />

(LCPs) em it tad In thermal neutron-induced fission of 2"u has been<br />

measured. The method of detection of polar LCPs consists of using<br />

a pair of lonlzation chamber with a multi-hole collimator as a<br />

common cathode. The ionizatlon chambers detect the fission<br />

fragments related to polar and equatorial LGPs, the LCPs being<br />

detected by a semiconductor AB-£ telescope. The collimator<br />

arrangement thus separates tha polar and equatorial events. Using<br />

different collimation for polar LCP region of angular distribution*<br />

the yields of polar protons, tritons and alpha particles were<br />

measured. Using Mote Carlo simulation far the detection system*<br />

o(0J fcr the angular distribution of polar protons, tritons and<br />

alpha particles were determined (refer to table).<br />

Table<br />

The width of the angular distribution of polar LCPs.<br />

LCPs a(&)<br />

Alpha particle (28.0±7.0)°<br />

Proton (13.0+6.0)°<br />

Triton (25.0+15.0)°<br />

The errors Indicated in the table are statistical only. The<br />

angular distribution of polar protons was found to be narrow<br />

compared to a wide angular distribution of polar tritons and alpha<br />

particles as indicated in the table.

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