Cargando…
The energy spectrum of cosmic-ray electrons from 10 to 100 GeV observed with a highly granulated imaging calorimeter
Cosmic-ray electrons (and positrons) have been observed in the energy range from 12 to ~100 GeV with a new balloon-borne payload, the Balloon-borne Electron Telescope with Scintillating Fibers (BETS). This is the first publication of the absolute energy spectrum of electrons measured with a highly g...
Autores principales: | , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2001
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1086/322274 http://cds.cern.ch/record/559297 |
_version_ | 1780899043420930048 |
---|---|
author | Torii, S Tamura, T Tateyama, N Yoshida, K Nishimura, J Yamagami, T Murakami, H Kobayashi, T Komori, Y Kasahara, K Yuda, T |
author_facet | Torii, S Tamura, T Tateyama, N Yoshida, K Nishimura, J Yamagami, T Murakami, H Kobayashi, T Komori, Y Kasahara, K Yuda, T |
author_sort | Torii, S |
collection | CERN |
description | Cosmic-ray electrons (and positrons) have been observed in the energy range from 12 to ~100 GeV with a new balloon-borne payload, the Balloon-borne Electron Telescope with Scintillating Fibers (BETS). This is the first publication of the absolute energy spectrum of electrons measured with a highly granulated fiber calorimeter. The calorimeter makes it possible to select electrons against the background protons by detailed observation of both the longitudinal and the lateral shower development. The performance of the detector was calibrated by the CERN-SPS accelerator beams: electrons from 5 to 100 GeV, protons from 60 to 250 GeV. The balloon observations were carried out twice, in 1997 and 1998, at the Sanriku Balloon Center (Institute of Space and Astronautical Science) in Japan. The observation time was ~13 hr in all at an altitude above 34 km. A total of 1349 electron candidates were collected, and the 628 events with energies above 12.5 GeV, well above the geomagnetic rigidity cutoff of ~10 GV, have been used to compose a differential absolute energy spectrum at the top of the atmosphere. The energy spectrum is described by a power-law index of 3.00+or-0.09, and the absolute differential intensity at 10 GeV is 0.199+or-0.015 m/sup -2/ s/sup -1 / sr/sup -1/ GeV/sup -1/. The overall shape of the energy spectrum in 10-100 GeV can be explained by a diffusion model, in which the authors assume an energy-dependent diffusion coefficient ( varies as E/sup 0.3/) for an injection spectrum, E/sup -2.4/. (31 refs). |
id | cern-559297 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2001 |
record_format | invenio |
spelling | cern-5592972019-09-30T06:29:59Zdoi:10.1086/322274http://cds.cern.ch/record/559297engTorii, STamura, TTateyama, NYoshida, KNishimura, JYamagami, TMurakami, HKobayashi, TKomori, YKasahara, KYuda, TThe energy spectrum of cosmic-ray electrons from 10 to 100 GeV observed with a highly granulated imaging calorimeterAstrophysics and AstronomyCosmic-ray electrons (and positrons) have been observed in the energy range from 12 to ~100 GeV with a new balloon-borne payload, the Balloon-borne Electron Telescope with Scintillating Fibers (BETS). This is the first publication of the absolute energy spectrum of electrons measured with a highly granulated fiber calorimeter. The calorimeter makes it possible to select electrons against the background protons by detailed observation of both the longitudinal and the lateral shower development. The performance of the detector was calibrated by the CERN-SPS accelerator beams: electrons from 5 to 100 GeV, protons from 60 to 250 GeV. The balloon observations were carried out twice, in 1997 and 1998, at the Sanriku Balloon Center (Institute of Space and Astronautical Science) in Japan. The observation time was ~13 hr in all at an altitude above 34 km. A total of 1349 electron candidates were collected, and the 628 events with energies above 12.5 GeV, well above the geomagnetic rigidity cutoff of ~10 GV, have been used to compose a differential absolute energy spectrum at the top of the atmosphere. The energy spectrum is described by a power-law index of 3.00+or-0.09, and the absolute differential intensity at 10 GeV is 0.199+or-0.015 m/sup -2/ s/sup -1 / sr/sup -1/ GeV/sup -1/. The overall shape of the energy spectrum in 10-100 GeV can be explained by a diffusion model, in which the authors assume an energy-dependent diffusion coefficient ( varies as E/sup 0.3/) for an injection spectrum, E/sup -2.4/. (31 refs).oai:cds.cern.ch:5592972001 |
spellingShingle | Astrophysics and Astronomy Torii, S Tamura, T Tateyama, N Yoshida, K Nishimura, J Yamagami, T Murakami, H Kobayashi, T Komori, Y Kasahara, K Yuda, T The energy spectrum of cosmic-ray electrons from 10 to 100 GeV observed with a highly granulated imaging calorimeter |
title | The energy spectrum of cosmic-ray electrons from 10 to 100 GeV observed with a highly granulated imaging calorimeter |
title_full | The energy spectrum of cosmic-ray electrons from 10 to 100 GeV observed with a highly granulated imaging calorimeter |
title_fullStr | The energy spectrum of cosmic-ray electrons from 10 to 100 GeV observed with a highly granulated imaging calorimeter |
title_full_unstemmed | The energy spectrum of cosmic-ray electrons from 10 to 100 GeV observed with a highly granulated imaging calorimeter |
title_short | The energy spectrum of cosmic-ray electrons from 10 to 100 GeV observed with a highly granulated imaging calorimeter |
title_sort | energy spectrum of cosmic-ray electrons from 10 to 100 gev observed with a highly granulated imaging calorimeter |
topic | Astrophysics and Astronomy |
url | https://dx.doi.org/10.1086/322274 http://cds.cern.ch/record/559297 |
work_keys_str_mv | AT toriis theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT tamurat theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT tateyaman theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT yoshidak theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT nishimuraj theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT yamagamit theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT murakamih theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT kobayashit theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT komoriy theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT kasaharak theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT yudat theenergyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT toriis energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT tamurat energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT tateyaman energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT yoshidak energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT nishimuraj energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT yamagamit energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT murakamih energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT kobayashit energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT komoriy energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT kasaharak energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter AT yudat energyspectrumofcosmicrayelectronsfrom10to100gevobservedwithahighlygranulatedimagingcalorimeter |