TY - JOUR
T1 - Intense positron beam at KEK
AU - Kurihara, Toshikazu
AU - Yagishita, Akira
AU - Enomoto, Atsushi
AU - Kobayashi, Hitoshi
AU - Shidara, Tetsuo
AU - Shirakawa, Akihiro
AU - Nakahara, Kazuo
AU - Saitou, Haruo
AU - Inoue, Kouji
AU - Nagashima, Yasuyuki
AU - Hyodo, Toshio
AU - Nagai, Yasuyoshi
AU - Hasegawa, Masayuki
AU - Inoue, Yoshi
AU - Kogure, Yoshiaki
AU - Doyama, Masao
PY - 2000/8
Y1 - 2000/8
N2 - A positron beam is a useful probe for investigating the electronic states in solids, especially concerning the surface states. The advantage of utilizing positron beams is in their simpler interactions with matter, owing to the absence of any exchange forces, in contrast to the case of low-energy electrons. However, such studies as low-energy positron diffraction, positron microscopy and positronium (Ps) spectroscopy, which require high intensity slow-positron beams, are very limited due to the poor intensity obtained from a conventional radioactive-isotope-based positron source. In conventional laboratories, the slow-positron intensity is restricted to 106 e+/s due to the strength of the available radioactive source. An accelerator based slow-positron source is a good candidate for increasing the slow-positron intensity. One of the results using a high intensity pulsed positron beam is presented as a study of the origins of a Ps emitted from SiO2. We also describe the two-dimensional angular correlation of annihilation radiation (2D-ACAR) measurement system with slow-positron beams and a positron microscope.
AB - A positron beam is a useful probe for investigating the electronic states in solids, especially concerning the surface states. The advantage of utilizing positron beams is in their simpler interactions with matter, owing to the absence of any exchange forces, in contrast to the case of low-energy electrons. However, such studies as low-energy positron diffraction, positron microscopy and positronium (Ps) spectroscopy, which require high intensity slow-positron beams, are very limited due to the poor intensity obtained from a conventional radioactive-isotope-based positron source. In conventional laboratories, the slow-positron intensity is restricted to 106 e+/s due to the strength of the available radioactive source. An accelerator based slow-positron source is a good candidate for increasing the slow-positron intensity. One of the results using a high intensity pulsed positron beam is presented as a study of the origins of a Ps emitted from SiO2. We also describe the two-dimensional angular correlation of annihilation radiation (2D-ACAR) measurement system with slow-positron beams and a positron microscope.
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U2 - 10.1016/S0168-583X(00)00074-4
DO - 10.1016/S0168-583X(00)00074-4
M3 - Article
AN - SCOPUS:0034247020
SN - 0168-583X
VL - 171
SP - 164
EP - 171
JO - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
JF - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
IS - 1
ER -