ERL BASED ELECTRON-ION COLLIDER ERHIC. [electronic resource]
In this paper we describe eRHIC design based on the RHIC hadron rings and 10-to-20 GeV energy recovery electron linac. RHIC requires a very large tunability range for c.m. energies while maintaining very high luminosity up to 10³⁴ cm⁻² s⁻¹ per nucleon. The designs of this future polarized electron-h...
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Online Access |
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| Format: | Government Document Electronic eBook |
| Language: | English |
| Published: |
Washington, D.C. : Oak Ridge, Tenn. :
United States. Dept. of Energy. Office of Science ; distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy,
2005.
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| Subjects: |
MARC
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| 245 | 0 | 0 | |a ERL BASED ELECTRON-ION COLLIDER ERHIC. |h [electronic resource] |
| 260 | |a Washington, D.C. : |b United States. Dept. of Energy. Office of Science ; |a Oak Ridge, Tenn. : |b distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy, |c 2005. | ||
| 300 | |a 5 pages : |b digital, PDF file. | ||
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| 500 | |a Published through the Information Bridge: DOE Scientific and Technical Information. | ||
| 500 | |a 05/16/2005. | ||
| 500 | |a "bnl--73467-2005-cp" | ||
| 500 | |a "KB-0202011" | ||
| 500 | |a PAC 2005 PARTICLE ACCELERATOR CONFERENCE; KNOXVILLE, TN; 20050516 through 20050520. | ||
| 500 | |a ANDERSON,D.; LITVINENKO,V.N.; BEN-ZVI,I. | ||
| 520 | 3 | |a In this paper we describe eRHIC design based on the RHIC hadron rings and 10-to-20 GeV energy recovery electron linac. RHIC requires a very large tunability range for c.m. energies while maintaining very high luminosity up to 10³⁴ cm⁻² s⁻¹ per nucleon. The designs of this future polarized electron-hadron collider, eRHIC, based on a high current super-conducting energy-recovery linac (ERL) with energy of electrons up to 20 GeV, have a number of specific requirements on the ERL optics. Two of the most attractive features of this scheme are full spin transparency of the ERL at all operational energies and the capability to support up to four interaction points. We present two main layouts of the eRHIC, the expected beam and luminosity parameter, and discuss the potential limitation of its performance. Two of the most attractive features of this scheme are full spin transparency of the ERL at all operational energies and the capability to support up to four interaction points. We present two main layouts of the eRHIC, the expected beam and luminosity parameter, and discuss the potential limitation of its performance. | |
| 536 | |b DE-AC02-98CH10886. | ||
| 536 | |b AD-003. | ||
| 650 | 7 | |a Hadrons. |2 local. | |
| 650 | 7 | |a Design. |2 local. | |
| 650 | 7 | |a Spin. |2 local. | |
| 650 | 7 | |a Performance. |2 local. | |
| 650 | 7 | |a Luminosity. |2 local. | |
| 650 | 7 | |a Electrons. |2 local. | |
| 650 | 7 | |a Accelerators. |2 local. | |
| 650 | 7 | |a Optics. |2 local. | |
| 650 | 7 | |a Energy Recovery. |2 local. | |
| 650 | 7 | |a Linear Accelerators. |2 local. | |
| 650 | 7 | |a Particle Accelerators. |2 edbsc. | |
| 710 | 2 | |a Brookhaven National Laboratory. |4 res. | |
| 710 | 1 | |a United States. |b Department of Energy. |b Office of Science. |4 spn. | |
| 710 | 1 | |a United States. |b Department of Energy. |b Office of Scientific and Technical Information. |4 dst. | |
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