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Title: Overview of the SPring-8 Diagnostics Beamlines

Abstract

We present an overview of the two SPring-8 diagnostics beamlines, the beamline I (dipole magnet source) and II (insertion device source). At the beamline I, synchrotron radiation (SR) in both the X-ray and the visible bands is exploited for characterizations of the electron beam. At the beamline II, by observing the spectral, spatial, and temporal characteristics of X-ray SR of the insertion device (ID), new techniques for accelerator diagnostics are investigated. Irradiation experiments with the ID to develop accelerator components such as photon absorbers, and production of intensive 10 MeV {gamma}-rays by backward Compton scattering of external far infrared (FIR) laser photons are being prepared at the beamline II.

Authors:
; ; ; ; ; ; ; ; ; ;  [1];  [2]
  1. Japan Synchrotron Radiation Research Institute, SPring-8, Sayo, Hyogo, 679-5198 (Japan)
  2. Center of Advanced Metrology, Chubu University, Kasugai, Aichi, 487-8501 (Japan)
Publication Date:
OSTI Identifier:
21410261
Resource Type:
Journal Article
Journal Name:
AIP Conference Proceedings
Additional Journal Information:
Journal Volume: 1234; Journal Issue: 1; Conference: SRI 2009: 10. international conference on radiation instrumentation, Melbourne (Australia), 27 Sep - 2 Oct 2009; Other Information: DOI: 10.1063/1.3463223; (c) 2010 American Institute of Physics; Journal ID: ISSN 0094-243X
Country of Publication:
United States
Language:
English
Subject:
43 PARTICLE ACCELERATORS; ACCELERATORS; COMPTON EFFECT; DIPOLES; ELECTRON BEAMS; GAMMA RADIATION; LASER RADIATION; MAGNETS; MEV RANGE; MONOCHROMATORS; PHOTONS; SPRING-8 STORAGE RING; SYNCHROTRON RADIATION; X RADIATION; BASIC INTERACTIONS; BEAMS; BOSONS; BREMSSTRAHLUNG; ELASTIC SCATTERING; ELECTROMAGNETIC INTERACTIONS; ELECTROMAGNETIC RADIATION; ELEMENTARY PARTICLES; ENERGY RANGE; EQUIPMENT; INTERACTIONS; IONIZING RADIATIONS; LEPTON BEAMS; MASSLESS PARTICLES; MULTIPOLES; PARTICLE BEAMS; RADIATION SOURCES; RADIATIONS; SCATTERING; STORAGE RINGS; SYNCHROTRON RADIATION SOURCES

Citation Formats

Takano, S, Masaki, M, Tamura, K, Mochihashi, A, Nakamura, T, Suzuki, S, Oishi, M, Shoji, M, Taniuchi, Y, Okayasu, Y, Ohkuma, H, and Okajima, S. Overview of the SPring-8 Diagnostics Beamlines. United States: N. p., 2010. Web. doi:10.1063/1.3463223.
Takano, S, Masaki, M, Tamura, K, Mochihashi, A, Nakamura, T, Suzuki, S, Oishi, M, Shoji, M, Taniuchi, Y, Okayasu, Y, Ohkuma, H, & Okajima, S. Overview of the SPring-8 Diagnostics Beamlines. United States. https://doi.org/10.1063/1.3463223
Takano, S, Masaki, M, Tamura, K, Mochihashi, A, Nakamura, T, Suzuki, S, Oishi, M, Shoji, M, Taniuchi, Y, Okayasu, Y, Ohkuma, H, and Okajima, S. 2010. "Overview of the SPring-8 Diagnostics Beamlines". United States. https://doi.org/10.1063/1.3463223.
@article{osti_21410261,
title = {Overview of the SPring-8 Diagnostics Beamlines},
author = {Takano, S and Masaki, M and Tamura, K and Mochihashi, A and Nakamura, T and Suzuki, S and Oishi, M and Shoji, M and Taniuchi, Y and Okayasu, Y and Ohkuma, H and Okajima, S},
abstractNote = {We present an overview of the two SPring-8 diagnostics beamlines, the beamline I (dipole magnet source) and II (insertion device source). At the beamline I, synchrotron radiation (SR) in both the X-ray and the visible bands is exploited for characterizations of the electron beam. At the beamline II, by observing the spectral, spatial, and temporal characteristics of X-ray SR of the insertion device (ID), new techniques for accelerator diagnostics are investigated. Irradiation experiments with the ID to develop accelerator components such as photon absorbers, and production of intensive 10 MeV {gamma}-rays by backward Compton scattering of external far infrared (FIR) laser photons are being prepared at the beamline II.},
doi = {10.1063/1.3463223},
url = {https://www.osti.gov/biblio/21410261}, journal = {AIP Conference Proceedings},
issn = {0094-243X},
number = 1,
volume = 1234,
place = {United States},
year = {Wed Jun 23 00:00:00 EDT 2010},
month = {Wed Jun 23 00:00:00 EDT 2010}
}