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Phys. Rev. E 67, 016502 (2003) [8 pages]

Measurement of positron production efficiency from a tungsten monocrystalline target using 4- and 8-GeV electrons

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T. Suwada*, S. Anami, R. Chehab, A. Enomoto, K. Furukawa, K. Kakihara, T. Kamitani, Y. Ogawa, S. Ohsawa, and T. Oogoe
Accelerator Laboratory, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan

H. Okuno
Institute of Particle and Nuclear Studies, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan

T. Fujita, K. Umemori, and K. Yoshida
Hiroshima Synchrotron Radiation Center, Hiroshima University, 2-313 Kagamiyama, Higashi-Hiroshima 739-8526, Japan

R. Hamatsu and K. Sasahara
Department of Physics, Tokyo Metropolitan University, 1-1 Minami-Ohsawa, Hachioji, Tokyo 192-0397, Japan

V. Ababiy, A. P. Potylitsyn, and I. E. Vnukov
Nuclear Physics Institute, Tomsk Polytechnic University, 634050, P.O. Box 25, Tomsk, Russia

Received 28 May 2001; revised 7 November 2002; published 16 January 2003

Intense positron sources are being widely investigated for the next-generation linear colliders and B factories. A new method utilizing an axially oriented crystal as a positron-production target is one of the bright schemes, since it provides a powerful photon source through channeling and coherent bremsstrahlung processes when high-energy electrons penetrate the target. A series of positron-production experiments with tungsten crystals hit by 4- and 8-GeV single-bunch electron beams were carried out at the KEKB 8-GeV injector linac. Three tungsten crystals with different thicknesses (2.2, 5.3, and 9.0 mm) and those combined with amorphous tungsten plates were tested on a precise goniometer. The positron-production yields were measured with a magnetic spectrometer in the positron momentum (Pe+) range from 5 to 20MeV/c. The angle of the 111 crystal axis with respect to the electron-beam direction was controlled by measuring the relative intensities of the produced positrons as a function of the rotational angle of the goniometer. The results show that the enhancements of the positron yield from crystal targets compared to amorphous targets of the same thickness at Pe+=20MeV/c are from 1.5 to 3.7 and from 1.8 to 5.1, depending upon the target thickness for 4- and 8-GeV electrons, respectively.

© 2003 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.67.016502
DOI:
10.1103/PhysRevE.67.016502
PACS:
41.75.Fr, 41.75.Ht, 61.80.Fe, 61.85.+p

*Electronic address: tsuyoshi.suwada@kek.jp

Also at LAL, IN2P3-CNRS, Université de Paris–Sud, Bât. 200, B.P. 34, 91898 Orsay, France.