Positron Annihilation in Neutron-Irradiated p -Type Silicon
L. J. Cheng, C.K. Yeh, S. I. Ma, C. S. Su
Abstract
L. J. Cheng, C.K. Yeh, S. I. Ma, C. S. Su
Abstract
Effects of neutron irradiation and subsequent thermal annealing on positron-lifetime spectra in $p$-type silicon have been studied. In unirradiated samples, two annihilation rates (4.13 \ifmmode\times\else\texttimes\fi{} ${10}^{9}$ ${\mathrm{sec}}^{\ensuremath{-}1}$ with an intensity of 98% and 7.14 \ifmmode\times\else\texttimes\fi{} ${10}^{8}$ ${\mathrm{sec}}^{\ensuremath{-}1}$ with an intensity of 2%) are observed. The annihilation rate of the dominant component becomes smaller upon irradiation. The effect saturates at high integrated neutron flux, \ensuremath{\sim} 1 \ifmmode\times\else\texttimes\fi{} ${10}^{17}$ n/${\mathrm{cm}}^{2}$, and disappears completely upon thermal annealing at 400-500 \ifmmode^\circ\else\textdegree\fi{}C. The annealing behavior is dependent on the integrated neutron flux. These results show that some neutron-induced defects act as positron traps at room temperature. Our study also gives evidence that high-order vacancy defects are formed during annealing near 300 \ifmmode^\circ\else\textdegree\fi{}C. The mean electron density of the positron-sensitive defects (positron traps) is estimated from the saturation value of the annihilation rate to be about 35% less than that in the perfect crystal. The diffusion coefficient and the mobility of thermalized positrons in silicon are estimated to be about 0.16 ${\mathrm{cm}}^{2}$/sec and 6.4 ${\mathrm{cm}}^{2}$/sec V, respectively.
OpenAlex reports 27 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
Effects of neutron irradiation and subsequent thermal annealing on positron-lifetime spectra in $p$-type silicon have been studied. In unirradiated samples, two annihilation rates (4.13 \ifmmode\times\else\texttimes\fi{} ${10}^{9}$ ${\mathrm{sec}}^{\ensuremath{-}1}$ with an intensity of 98% and 7.14 \ifmmode\times\else\texttimes\fi{} ${10}^{8}$ ${\mathrm{sec}}^{\ensuremath{-}1}$ with an intensity of 2%) are observed. The annihilation rate of the dominant component becomes smaller upon irradiation. The effect saturates at high integrated neutron flux, \ensuremath{\sim} 1 \ifmmode\times\else\texttimes\fi{} ${10}^{17}$ n/${\mathrm{cm}}^{2}$, and disappears completely upon thermal annealing at 400-500 \ifmmode^\circ\else\textdegree\fi{}C. The annealing behavior is dependent on the integrated neutron flux. These results show that some neutron-induced defects act as positron traps at room temperature. Our study also gives evidence that high-order vacancy defects are formed during annealing near 300 \ifmmode^\circ\else\textdegree\fi{}C. The mean electron density of the positron-sensitive defects (positron traps) is estimated from the saturation value of the annihilation rate to be about 35% less than that in the perfect crystal. The diffusion coefficient and the mobility of thermalized positrons in silicon are estimated to be about 0.16 ${\mathrm{cm}}^{2}$/sec and 6.4 ${\mathrm{cm}}^{2}$/sec V, respectively.
Key concepts: Annihilation, Physics, Neutron, Annealing (glass), Positron, Neutron temperature, Nuclear physics, Atomic physics