POSITRON-ANNIHILATION IN LIQUID-HELIUM AND LIQUID ARGON UNDER AN ELECTRIC-FIELD

Citation
I. Pepe et al., POSITRON-ANNIHILATION IN LIQUID-HELIUM AND LIQUID ARGON UNDER AN ELECTRIC-FIELD, Journal of physics. B, Atomic molecular and optical physics, 28(16), 1995, pp. 3643-3659
Citations number
30
Categorie Soggetti
Physics, Atomic, Molecular & Chemical",Optics
ISSN journal
09534075
Volume
28
Issue
16
Year of publication
1995
Pages
3643 - 3659
Database
ISI
SICI code
0953-4075(1995)28:16<3643:PILALA>2.0.ZU;2-L
Abstract
We have made new measurements of the lifetimes at 4.29 K and 2.92 K in He I, and at 2.14 K and 1.67 K in He II, without and with an electric field. At 4.19 K we have a new value of the lifetime, 2.01 +/- 0.002 ns, leading to a Z(eff) of 3.53 at zero field. In contrast to earlier reports, Z(eff) decreases very slightly as the temperature is lowered and the density increases. The orthopositronium lifetime at 4.19 K is 98.1 +/- 0.2 ns, at zero field, independent of field up to 18 kV cm(-1 ). At 4.19 K the free positron decay rate falls exponentially with inc reasing field to a value 5% below its zero-field value, the drop-off r ate being 0.36 +/- 0.04 cm amagat V-1. From 28 through 50 V cm(-1) ama gat(-1) the decay rate of the free component rises slowly as expected because of the increasing positronium fraction over the same range of electric field. In liquid argon there is positronium enhancement begin ning at or below 3 V cm(-1) amagat(-1), which contrasts with 160 V cm( -1) amagat(-1) for argon gas. At least two lifetimes make up the long triplet component, suggesting different degrees of thermalization, or different states of positronium within the liquid. The effect of the e lectric field is to enhance the longer-lived, or more thermal componen t, in strong contrast with the findings of Charlton et al for the gas. The argon results suggest positron behaviour similar to that of elect rons in the liquid phase, namely, such particles move in a conduction band subject to small effective scattering and diffusion cross section s. An analytic model in which the scattering length is an adjustable p arameter yields the onset of positronium enhancement just below 3 V cm (-1) amagat(-1) when a(s) = -0.043 a(0), corresponding to an elastic s cattering and diffusion cross section of 0.034 pi a(0)(2). Consequence s for positron thermalization are discussed. A model of positronium lo sing energy slowly in the liquid without bubble formation is suggested .