Slow Positron Group

Group Leader: HYODO, Toshio

The poitron is the anti-particle of the electron. The Slow Positron Facility of the Photon Factory provides a high intensity, pulsed slow positron beam. The beam is used for researches in solid state physics and atomic and molelcular physics.

[Major Research Projects]

Total-reflection high-energy positron diffraction (TRHEPD)

For positrons with their positive charge, it is straightforward to obtain information only for the atomic arrangement on the topmost surface. That is, positrons incident on a surface at a glancing angle below a critical angle are totally reflected at the first atomic layer and do not enter the crystal at all. By using this characteristic of positron beams, diffraction patterns reflecting the atomic positions at the topmost surface can be obtained by directing positrons with a given energy at a certain grazing angle to the crystal surface. The diffraction patterns can then be used to determine the atomic positions at the topmost surface. This forms the essence of the TRHEPD method.

Positron and electron diffraction patterns obtained for glancing angles of 1.3° and 2.1°.

Experiment using positronium negative ion Ps-

Photodetachment of Ps-
(by Nagashima Lab. in TUS)

A positron may be bound with an electron to form a positronium atom, a boud state like an hydrogen atom. It is also possible to form a positronium negative ion (Ps-) by binding one more electron. Ps- ions are emitted from a tungsten surface when it is bombarded with a slow positron beam. Its formation efficiency increases drastically when alkali metals such as Na and Cs is deposited on the surface. This station is for the formation of pulse Ps- by bombarding such a surface with a slow positron pulse and the applications. Recently an experiment of photodetachment of Ps- (dissociation into Ps and an electron by an irradiation of a laser beam) was successfully conducted.

Ps-TOF (positron time-of-flight) measurement

Ps-TOF is a measurement of the energy of positronium emitted from a solid surface. The incident positrons hit the sample target and the ortho-Ps atoms emitted from the surface annihilate in flight. The annihilation gamma-rays are viewed by detector through lead slits and the time of the detection with reference to the positron injection time is recorded. The width and the frequency of the incident positron pulse are 1ns-10ns (variable) and 50 Hz, respectively.

R&D Study of Positron Beamlines and apparatus


HYODO, ToshioProf.Positron science
WADA, KenAssistant Prof.Positron science
MOCHIZUKI, IzumiResearcherPositron science


Slow Positron Facility

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