RuPAC2014 - List of Keywords (storage-ring)

Paper	Title	Other Keywords	Page
THPSC11	NSLS-II Booster Vacuum System	vacuum, booster, electron, radiation	342
	A.M. Semenov, V.V. Anashin, S.M. Gurov, V.A. Kiselev, A.A. Krasnov BINP SB RAS, Novosibirsk, Russia H.-C. Hseuh, T.V. Shaftan BNL, Upton, Long Island, New York, USA
	One of the last SR source third generation (NSLS-II) is constructed in Brookhaven National Laboratory in present time. To raise the operation effectiveness in continued mode with irradiation of maximum brightness injectors of these SR sources is operated continually on the energy up to energy of the main ring (linac or synchrotron booster). The injection on the full energy allows add electrons to early moved electrons in a storage ring rather than to regulate a magnet system. This operating mode is often named "Top-Up". NSLS-II consists of a linear accelerator on the electron energy up to 200 MeV, a synchrotron booster on the energy 3 GeV, a main storage ring. The status and review of vacuum system are written in this report.

THPSC14	Electron Emission and Trapping in Non-Uniform Fields of Magnet Structure and Insertion Devices at SR Source Siberia-2	electron, quadrupole, vacuum, wiggler	350
	V.I. Moiseev, V. Korchuganov, N.V. Smolyakov NRC, Moscow, Russia
	In vacuum chamber of SR source, scattered photons provide high intensity flows of photo emitted electrons along the magnetic fields lines. The unperturbed electrons reach the opposite walls. The relativistic bunches influence the trajectories of low energy electrons. These electrons can be trapped by non-uniform magnetic field. The low energy electron distributions change the operating settings of the storage ring. For Siberia-2 case, the low energy electron densities are evaluated both in quadrupole lenses and in superconducting wiggler on 7.5 T field. The qualitative description of the trapped electrons behavior was developed. In calculations, the analitical solution was obtained and used for estimations of the single impact of relativistic bunch.

THPSC26	Distributed Beam Loss Monitor Based on the Cherenkov Effect in Optical Fiber	electron, radiation, positron, linac	374
	Yu. Maltseva, F.E. Emanov, A.V. Petrenko, V.G. Prisekin BINP SB RAS, Novosibirsk, Russia F.E. Emanov NSU, Novosibirsk, Russia A.V. Petrenko CERN, Geneva, Switzerland
	A distributed beam loss monitor based on the Cherenkov effect in optical fiber has been implemented for the VEPP-5 electron and positron linacs and the 510 MeV damping ring at the Budker INP. The monitor operation is based on detection of the Cherenkov radiation generated in optical fiber by means of relativistic particles created in electromagnetic shower after highly relativistic beam particles (electrons or positrons) hit the vacuum pipe. The main advantage of the distributed monitor compared to local ones is that a long optical fiber section can be used instead of a large number of local beam loss monitors. In our experiments the Cherenkov light was detected by photomultiplier tube (PMT). Timing of PMT signal gives the location of the beam loss. In the experiment with 20 m long optical fiber we achieved 3 m spatial resolution. To improve spatial resolution optimization and selection process of optical fiber and PMT are needed and according to our theoretical estimations 0.5 m spatial resolution can be achieved. We also suggest similar techniques for detection of electron (or positron) losses due to Touschek effect in storage rings.

Paper

Title

Other Keywords

Page

THPSC11

NSLS-II Booster Vacuum System

vacuum, booster, electron, radiation

342

A.M. Semenov, V.V. Anashin, S.M. Gurov, V.A. Kiselev, A.A. Krasnov
BINP SB RAS, Novosibirsk, Russia
H.-C. Hseuh, T.V. Shaftan
BNL, Upton, Long Island, New York, USA

One of the last SR source third generation (NSLS-II) is constructed in Brookhaven National Laboratory in present time. To raise the operation effectiveness in continued mode with irradiation of maximum brightness injectors of these SR sources is operated continually on the energy up to energy of the main ring (linac or synchrotron booster). The injection on the full energy allows add electrons to early moved electrons in a storage ring rather than to regulate a magnet system. This operating mode is often named "Top-Up". NSLS-II consists of a linear accelerator on the electron energy up to 200 MeV, a synchrotron booster on the energy 3 GeV, a main storage ring. The status and review of vacuum system are written in this report.

THPSC14

Electron Emission and Trapping in Non-Uniform Fields of Magnet Structure and Insertion Devices at SR Source Siberia-2

electron, quadrupole, vacuum, wiggler

350

V.I. Moiseev, V. Korchuganov, N.V. Smolyakov
NRC, Moscow, Russia

In vacuum chamber of SR source, scattered photons provide high intensity flows of photo emitted electrons along the magnetic fields lines. The unperturbed electrons reach the opposite walls. The relativistic bunches influence the trajectories of low energy electrons. These electrons can be trapped by non-uniform magnetic field. The low energy electron distributions change the operating settings of the storage ring. For Siberia-2 case, the low energy electron densities are evaluated both in quadrupole lenses and in superconducting wiggler on 7.5 T field. The qualitative description of the trapped electrons behavior was developed. In calculations, the analitical solution was obtained and used for estimations of the single impact of relativistic bunch.

THPSC26

Distributed Beam Loss Monitor Based on the Cherenkov Effect in Optical Fiber

electron, radiation, positron, linac

374

Yu. Maltseva, F.E. Emanov, A.V. Petrenko, V.G. Prisekin
BINP SB RAS, Novosibirsk, Russia
F.E. Emanov
NSU, Novosibirsk, Russia
A.V. Petrenko
CERN, Geneva, Switzerland

A distributed beam loss monitor based on the Cherenkov effect in optical fiber has been implemented for the VEPP-5 electron and positron linacs and the 510 MeV damping ring at the Budker INP. The monitor operation is based on detection of the Cherenkov radiation generated in optical fiber by means of relativistic particles created in electromagnetic shower after highly relativistic beam particles (electrons or positrons) hit the vacuum pipe. The main advantage of the distributed monitor compared to local ones is that a long optical fiber section can be used instead of a large number of local beam loss monitors. In our experiments the Cherenkov light was detected by photomultiplier tube (PMT). Timing of PMT signal gives the location of the beam loss. In the experiment with 20 m long optical fiber we achieved 3 m spatial resolution. To improve spatial resolution optimization and selection process of optical fiber and PMT are needed and according to our theoretical estimations 0.5 m spatial resolution can be achieved. We also suggest similar techniques for detection of electron (or positron) losses due to Touschek effect in storage rings.