1968
DOI: 10.1016/s0065-2199(08)60185-2
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Positrons and Positronium in Gases

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Cited by 110 publications
(33 citation statements)
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“…It is found empirically that the value of Z eff at very low energies is proportional to the dipole polarizability α of the hydrogen atom (Osmon, 1965) [36] and can be represented by α 1.25 . The annihilation of positrons with electrons results in two photons at a rate λ, Fraser (1968) [37]: [19], D: Green and Gribakin (2013) [35]. In the above equation ρ is the density in grams per cubic centimeter and M A is the atomic mass.…”
Section: Z Effmentioning
confidence: 99%
“…It is found empirically that the value of Z eff at very low energies is proportional to the dipole polarizability α of the hydrogen atom (Osmon, 1965) [36] and can be represented by α 1.25 . The annihilation of positrons with electrons results in two photons at a rate λ, Fraser (1968) [37]: [19], D: Green and Gribakin (2013) [35]. In the above equation ρ is the density in grams per cubic centimeter and M A is the atomic mass.…”
Section: Z Effmentioning
confidence: 99%
“…Besides reproducing the low-energy elastic cross section, this model potential approach also does a reasonable job of reproducing Z eff (v). The annihilation parameter is computed from the scattering wave function using [4,25,26] …”
Section: Collision Modelmentioning
confidence: 99%
“…One parameter is the positronium fraction, i.e., the number of positrons surviving in the form of free positronium. Another parameter is the annihilation parameter, Z eff (v), which can be defined in terms of the spin-averaged annihilation cross section, σ ann (v), by the identity [4],…”
Section: Introductionmentioning
confidence: 99%
“…The annihilation parameter Z eff is computed from the scattering wave function using the identity [23][24][25],…”
Section: G Positron Annihilationmentioning
confidence: 99%