1986
DOI: 10.1071/ph860497
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Numerical Simulation of Positron Diffusion in the Heavy Noble Gases Ar, Kr and Xe

Abstract: Numerical simulation has been carried out of positron annihilation and diffusion under the influence of an external temperature and electric field in heavy noble gases. The electric field was varied over the range 0-200 V cm -1 amagat -1 (1 amagat ... 2.687 xl 0 19 atoms cm -3), whereas the temperature was varied from 300 to 3000 K. It is observed that the decay constant ZeIT increases with increasing atomic mass of the interacting gases He, Ne, Ar, Kr and Xe, while the diffusion coefficient decreases except i… Show more

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(6 citation statements)
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“…When the magnetic field is applied to the gas assembly the value of Ec increases: (EdKr '" 40 V cm-1 and (Ec}xe '" 60 V cm-1 at B = 10 kG, whereas at B = 50 kG, Ec is ",70 V cm-1 for Kr and ",80 V cm-1 for Xe. The magnetic field has more effect in Kr than in Xe because Kr is a lighter gas (see Singh and Grover 1986). The theoretical and experimental annihilation rates by different workers are presented in Table 1.…”
Section: Resultsmentioning
confidence: 99%
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“…When the magnetic field is applied to the gas assembly the value of Ec increases: (EdKr '" 40 V cm-1 and (Ec}xe '" 60 V cm-1 at B = 10 kG, whereas at B = 50 kG, Ec is ",70 V cm-1 for Kr and ",80 V cm-1 for Xe. The magnetic field has more effect in Kr than in Xe because Kr is a lighter gas (see Singh and Grover 1986). The theoretical and experimental annihilation rates by different workers are presented in Table 1.…”
Section: Resultsmentioning
confidence: 99%
“…a , and we assume that Fo(v,t) =F(v)e-A,t. Using this assumption in equation (1) and after integrating over velocity, we get a linear integro-differential equation (see Singh and Grover 1987), the solution of which yields the equilibrium positron velocity distribution y(v). After calculating y(v), we obtain the annihilation rate…”
Section: Methods Of Studymentioning
confidence: 99%
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