Experiment of positron generation using a crystal target at the KEK electron/positron linac

Abstract

We have performed an experiment of positron generation using a crystal target at an electron/positron linac at KEK. The target consists of a tungsten crystal to emit photons and an amorphous tungsten for pair creation, whose thicknesses are 0.5 and 2.0 radiation length, respectively. When the 〈1 1 1〉 crystal axis is oriented parallel to the 3 GeV incident electron beam, the positron yield is enhanced by 40% compared to values for the disoriented crystal. No effect of injecting intense ultra-short electron bunches on the crystalline structure is observed. The crystal orientation dependence of the positron yield as well as the enhancement factor can be explained by a simulation assuming a coherent bremsstrahlung process of the electron in the crystal.

Original language	English
Pages (from-to)	104-111
Number of pages	8
Journal	Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
Volume	173
Issue number	1
DOIs	https://doi.org/10.1016/S0168-583X(00)00195-6
Publication status	Published - 1 Jan 2001

ASJC Scopus subject areas

Nuclear and High Energy Physics
Instrumentation

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10.1016/S0168-583X(00)00195-6

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Inoue, M., Takenaka, S., Yoshida, K., Endo, I., Iinuma, M., Takahashi, T., Bogdanov, A. V., Kolchuzkin, A. M., Potylitsin, A. P., Vnukov, I. E., Okuno, H., Anami, S., Enomoto, A., Furukawa, K., Kamitani, T., Ogawa, Y., & Ohsawa, S. (2001). Experiment of positron generation using a crystal target at the KEK electron/positron linac. Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms, 173(1), 104-111. https://doi.org/10.1016/S0168-583X(00)00195-6

Experiment of positron generation using a crystal target at the KEK electron/positron linac. / Inoue, M.; Takenaka, S.; Yoshida, K.; Endo, I.; Iinuma, M.; Takahashi, T.; Bogdanov, Alexey Victorovich; Kolchuzkin, A. M.; Potylitsin, A. P.; Vnukov, I. E.; Okuno, H.; Anami, S.; Enomoto, A.; Furukawa, K.; Kamitani, T.; Ogawa, Y.; Ohsawa, S.

In: Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms, Vol. 173, No. 1, 01.01.2001, p. 104-111.

Research output: Contribution to journal › Article › peer-review

Inoue, M, Takenaka, S, Yoshida, K, Endo, I, Iinuma, M, Takahashi, T, Bogdanov, AV, Kolchuzkin, AM, Potylitsin, AP, Vnukov, IE, Okuno, H, Anami, S, Enomoto, A, Furukawa, K, Kamitani, T, Ogawa, Y & Ohsawa, S 2001, 'Experiment of positron generation using a crystal target at the KEK electron/positron linac', Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms, vol. 173, no. 1, pp. 104-111. https://doi.org/10.1016/S0168-583X(00)00195-6

Inoue, M. ; Takenaka, S. ; Yoshida, K. ; Endo, I. ; Iinuma, M. ; Takahashi, T. ; Bogdanov, Alexey Victorovich ; Kolchuzkin, A. M. ; Potylitsin, A. P. ; Vnukov, I. E. ; Okuno, H. ; Anami, S. ; Enomoto, A. ; Furukawa, K. ; Kamitani, T. ; Ogawa, Y. ; Ohsawa, S. / Experiment of positron generation using a crystal target at the KEK electron/positron linac. In: Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms. 2001 ; Vol. 173, No. 1. pp. 104-111.

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abstract = "We have performed an experiment of positron generation using a crystal target at an electron/positron linac at KEK. The target consists of a tungsten crystal to emit photons and an amorphous tungsten for pair creation, whose thicknesses are 0.5 and 2.0 radiation length, respectively. When the 〈1 1 1〉 crystal axis is oriented parallel to the 3 GeV incident electron beam, the positron yield is enhanced by 40% compared to values for the disoriented crystal. No effect of injecting intense ultra-short electron bunches on the crystalline structure is observed. The crystal orientation dependence of the positron yield as well as the enhancement factor can be explained by a simulation assuming a coherent bremsstrahlung process of the electron in the crystal.",

author = "M. Inoue and S. Takenaka and K. Yoshida and I. Endo and M. Iinuma and T. Takahashi and Bogdanov, {Alexey Victorovich} and Kolchuzkin, {A. M.} and Potylitsin, {A. P.} and Vnukov, {I. E.} and H. Okuno and S. Anami and A. Enomoto and K. Furukawa and T. Kamitani and Y. Ogawa and S. Ohsawa",

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AU - Inoue, M.

AU - Takenaka, S.

AU - Yoshida, K.

AU - Endo, I.

AU - Iinuma, M.

AU - Takahashi, T.

AU - Bogdanov, Alexey Victorovich

AU - Kolchuzkin, A. M.

AU - Potylitsin, A. P.

AU - Vnukov, I. E.

AU - Okuno, H.

AU - Anami, S.

AU - Enomoto, A.

AU - Furukawa, K.

AU - Kamitani, T.

AU - Ogawa, Y.

AU - Ohsawa, S.

PY - 2001/1/1

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N2 - We have performed an experiment of positron generation using a crystal target at an electron/positron linac at KEK. The target consists of a tungsten crystal to emit photons and an amorphous tungsten for pair creation, whose thicknesses are 0.5 and 2.0 radiation length, respectively. When the 〈1 1 1〉 crystal axis is oriented parallel to the 3 GeV incident electron beam, the positron yield is enhanced by 40% compared to values for the disoriented crystal. No effect of injecting intense ultra-short electron bunches on the crystalline structure is observed. The crystal orientation dependence of the positron yield as well as the enhancement factor can be explained by a simulation assuming a coherent bremsstrahlung process of the electron in the crystal.

AB - We have performed an experiment of positron generation using a crystal target at an electron/positron linac at KEK. The target consists of a tungsten crystal to emit photons and an amorphous tungsten for pair creation, whose thicknesses are 0.5 and 2.0 radiation length, respectively. When the 〈1 1 1〉 crystal axis is oriented parallel to the 3 GeV incident electron beam, the positron yield is enhanced by 40% compared to values for the disoriented crystal. No effect of injecting intense ultra-short electron bunches on the crystalline structure is observed. The crystal orientation dependence of the positron yield as well as the enhancement factor can be explained by a simulation assuming a coherent bremsstrahlung process of the electron in the crystal.

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