TY - JOUR
T1 - Superconducting solenoidal spectrometer for a balloon-borne experiment
AU - Ajima, Y.
AU - Anraku, K.
AU - Haga, T.
AU - Higashi, Y.
AU - Honda, H.
AU - Imori, M.
AU - Inaba, S.
AU - Kimura, N.
AU - Kobayashi, M.
AU - Makida, Y.
AU - Matsui, N.
AU - Matsumoto, H.
AU - Matsunaga, H.
AU - Motoki, M.
AU - Nozaki, M.
AU - Nishihara, Y.
AU - Nishimura, J.
AU - Orito, S.
AU - Otoba, M.
AU - Saeki, T.
AU - Sanuki, T.
AU - Sasaki, M.
AU - Shimamura, K.
AU - Suzuki, J.
AU - Suzuki, K.
AU - Takimi, N.
AU - Tanaka, K.
AU - Tsunoda, T.
AU - Ueda, I.
AU - Yajima, T.
AU - Yamagami, T.
AU - Yamamoto, A.
AU - Yamaoka, H.
AU - Yoshida, T.
AU - Yoshimura, K.
PY - 2000/3/21
Y1 - 2000/3/21
N2 - The BESS detector is a new type of balloon-borne spectrometer which utilizes various technologies recently developed for collider experiments. The principal scientific objectives include a measurement of cosmic-ray antiproton spectrum, search for anti-nuclei in cosmic radiation, and precise measurements of cosmic-ray primaries. A thin superconducting solenoidal coil produces a uniform magnetic field of 1 T. Cylindrical drift chambers are located inside and outside the coil and perform continuous tracking. The momentum resolution is 0.5% at 1 GeV/c. i.e., the maximum detectable rigidity is 200 GV. Scintillation counter hodoscopes, placed above and below the solenoid, provide timing and dE/dx measurements and trigger generation. The timing resolution is 80 ps/counter. This cylindrical configuration achieves a large geometrical acceptance of 0.35 m2 sr which is essential to detect rare cosmic-ray particles. In order to cope with high trigger rate and large data size, intelligent trigger circuits and a fast and parallel data acquision system are also developed. In 1993, the first scientific flight of the BESS apparatus was carried out and the first mass-measured antiprotons were detected at energies below 500 MeV.
AB - The BESS detector is a new type of balloon-borne spectrometer which utilizes various technologies recently developed for collider experiments. The principal scientific objectives include a measurement of cosmic-ray antiproton spectrum, search for anti-nuclei in cosmic radiation, and precise measurements of cosmic-ray primaries. A thin superconducting solenoidal coil produces a uniform magnetic field of 1 T. Cylindrical drift chambers are located inside and outside the coil and perform continuous tracking. The momentum resolution is 0.5% at 1 GeV/c. i.e., the maximum detectable rigidity is 200 GV. Scintillation counter hodoscopes, placed above and below the solenoid, provide timing and dE/dx measurements and trigger generation. The timing resolution is 80 ps/counter. This cylindrical configuration achieves a large geometrical acceptance of 0.35 m2 sr which is essential to detect rare cosmic-ray particles. In order to cope with high trigger rate and large data size, intelligent trigger circuits and a fast and parallel data acquision system are also developed. In 1993, the first scientific flight of the BESS apparatus was carried out and the first mass-measured antiprotons were detected at energies below 500 MeV.
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U2 - 10.1016/S0168-9002(99)01010-4
DO - 10.1016/S0168-9002(99)01010-4
M3 - Article
AN - SCOPUS:0034696454
SN - 0168-9002
VL - 443
SP - 71
EP - 100
JO - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
JF - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
IS - 1
ER -