The Lbl 1-2 Gev Synchrotron Radiation Source
نویسنده
چکیده
The design of the 1-2 GeV Synchrotron Radiation Source to be built at the Lawrence Berkeley Laboratory is described. The goal of this facility is to provide very high brightness photon beams in the ultraviolet and soft X -ray regions. The photon energy nnge to be served is from 0.5 eV to 10 keY, with the brightest beams available in the I eV I keY interval. For time-resolved experiments, beam pulses of a few tens of picoseconds will be available. Emphasis will be on the use of undulators and wigglers to produce high quality, intense beams. Initially, four of the former and one of the latter devices will be installed, with six long straight sections left open for future installations. In addition, provision is being made for 48 beam lines from bending magnets. The storage ring is optimized for operation at 1.5 GeV, with a maximum energy of 1.9 GeV. The injection system includes a 1.5 GeV booster synchrotron for full energy injection at the nominal operating energy of the storage ring. Filling time for the maximum storage ring intensity of 400 mA is about. 2 minutes, and beam lifetime will be about 6 hours. Attention has been given to the extraordinary requirements for beam stability, and to the need to independently control photon beam alignment. Typical rms beam size in insertion regions is 20 1 um horizontal, and 38 ]!m vertical. The ",:lnner in which this design achieves very high spectral brightness from undulators and wigglers, while maintaining a modest value for the beam current, will be described. Primarily, this requires that. the design of the lattice, the arrangement of bending magnets, focusing quadrupoles and straight sections, be done with this in mind.
منابع مشابه
Lattice Design of Beijing Light Source
In this paper the preliminary design of magnet lattice of Beijing Light Source(BLS) is described. Beijing Light Source is a new generation light source with the energy of 2.2GeV2.5GeV. By choosing the FBA(five bend achromat) and TBA (triplet bend achromat) structure very low nature horizontal emittance is reached with using superconducting dipole magnets. Having made some harmonic correction th...
متن کاملSynchrotron Radiation Facilities in the Usa *
With the successful commissioning and achievement of significant milestones at both the 7-GeV Advanced Photon Source (APS) at Argonne National Laboratory and the 1.5-GeV Advanced Light Source (ALS) at Lawrence Berkeley National Laboratory, synchrotron radiation research capability in the United States holds the promise of many important discoveries in the decade to come. An overview of current ...
متن کاملطراحی الکترومغناطیسهای حلقه انبارش طرح چشمه نور ایران
Iranian Light Source Facility (ILSF) is a new 3 GeV synchrotron radiation laboratory in the Middle East. The ILSF storage ring (SR) is based on a Five-Bend Achromat lattice, providing a beam emittance of 0.48 nm rad. The ring is consisting of 100 pure dipole, 320 quadrupole and 320 sextupole magnets. In this paper, we present some design features of the SR magnets and discuss their detailed ph...
متن کاملThe Beijing Electron-positron Collider and Its Second Phase Construction
The Beijing Electron-Positron Collider (BEPC) was constructed for both high energy physics and synchrotron radiation researches. As an e, e collider operating in the τ-charm region and the first synchrotron radiation source in China, the machine has been well operated more than 15 years since it was put into operation. As a collider, the peak luminosity of the BEPC has reached its design goal o...
متن کاملGrb 080916c: on the Radiation Origin of the Prompt Emission from Kev/mev to Gev
Fermi observations of high-energy gamma-ray emission from GRB 080916C shows that its spectrum is consistent with the Band function from MeV to tens of GeV. Assuming one single emission mechanism dominates in the whole energy range, we show that this spectrum is consistent with synchrotron origin by shockaccelerated electrons. The simple electron inverse-Compton model and the hadronic model are ...
متن کامل