Paper |
Title |
Page |
TUPM2HA01 |
Commissioning COSY Cooler with Electron Beam at Novosibirsk |
79 |
|
- V.B. Reva, N. Alinovskiy, T.V. Bedareva, E.A. Bekhtenev, O.V. Belikov, V.N. Bocharov, V.V. Borodich, M.I. Bryzgunov, A.V. Bubley, V.A. Chekavinskiy, V.G. Cheskidov, B.A. Dovzhenko, A.I. Erokhin, M.G. Fedotov, A.D. Goncharov, K. Gorchakov, V.K. Gosteev, I.A. Gusev, A.A. Ivanov, G.V. Karpov, Y.I. Koisin, M.N. Kondaurov, V.R. Kozak, A.M. Kruchkov, A.D. Lisitsyn, I.A. Lopatkin, V.R. Mamkin, A.S. Medvedko, V.M. Panasyuk, V.V. Parkhomchuk, I.V. Poletaev, V.A. Polukhin, A.Yu. Protopopov, D.N. Pureskin, A.A. Putmakov, P.A. Selivanov, E.P. Semenov, D.V. Senkov, D.N. Skorobogatov, N.P. Zapiatkin
BINP SB RAS, Novosibirsk, Russia
|
|
|
The electron cooler of a 2 MEV for COSY storage ring FZJ is assembled in BINP. Results of experiments with high voltage, with electron beam, cascade transformer for distribution power along acceleration tube will be discussed in this report. The COSY cooler is designed on the classic scheme of low energy coolers like cooler CSRm, CSRe, LEIR that was produced in BINP before. The electron beam is transported inside the longitudinal magnetic field along whole trajectory from an electron gun to a collector. This optic scheme is stimulated by the wide range of the working energies 0.025–2 MeV. The electrostatic accelerator consists of 33 individual unify section. Each section contains two HV power supply (±30 kV) and power supply of the magnetic coils. The electrical power to each section is provided by the cascade transformer. The cascade transformer is the set of the transformers connected in series with isolating winding.
|
|
|
Slides TUPM2HA01 [3.228 MB]
|
|
|
WEPPO04 |
Collector for Electron Cooling Systems with Suppression of Reflected Electron Flux |
103 |
|
- M.I. Bryzgunov, A.V. Bubley, V.A. Chekavinskiy, I.A. Gusev, A.V. Ivanov, M.N. Kondaurov, V.M. Panasyuk, V.V. Parkhomchuk, D.N. Pureskin, A.A. Putmakov, V.B. Reva, D.V. Senkov, D.N. Skorobogatov
BINP SB RAS, Novosibirsk, Russia
|
|
|
Results of testing of the collector with Wien filter in the 2 MeV electron cooling system for COSY synchrotron are presented. Efficiency of a collector in high voltage electron cooling devices is important from the point of view of the load on high voltage power supply, radiation safety and vacuum conditions in the system. The collector for 2 MeV COSY cooler is supplemented with Wien filter which allows increase efficiency of the system by deflection secondary electron flux in crossed transverse electric and magnetic fields. Results of tests show that such solution provides efficiency of recuperation in the cooler up to 10-5. After tests some changes were made in the construction of the Wien filter to improve quality of the collector performance.
|
|
|
WEPPO07 |
Matching of Magnetic Field with Energy of Electrons in 2 MeV COSY Cooler |
110 |
|
- V.M. Panasyuk, M.I. Bryzgunov, A.V. Bubley, V.V. Parkhomchuk, V.B. Reva
BINP SB RAS, Novosibirsk, Russia
|
|
|
In the high energy electron cooler for COSY the beam energy range is wide (24 keV- 2 MeV). Typical guiding magnetic fields are 0.5 kG in accelerating tube, 1kG in transport channels and 2 kG in cooling solenoid and adjoining 45 degree toroids. As a result we have two sections with longitudinal gradient of field, three 90 degree bends and 45 degree toroid before solenoid entrance. In such circumstances the conditions of passage of electrons through the channel and theirs entrance into solenoid without heating are discussed. Also the results of using of correctors and pick-up system are considered.
|
|
|
WEPPO12 |
Compass for Measuring the Magnetic Lines Straightness at the Cooling Section in Vacuum |
121 |
|
- A.V. Bubley, M.I. Bryzgunov, V.G. Cheskidov, M.G. Fedotov, V.K. Gosteev, O.I. Meshkov, V.M. Panasyuk, V.V. Parkhomchuk, V.B. Reva
BINP SB RAS, Novosibirsk, Russia
- V. Kamerdzhiev, G. Langenberg
FZJ, Jülich, Germany
|
|
|
The 2 MeV cooler is under construction at COSY synchrotron. Due to high energy it is very strict requirement for the magnetic field homogeneity at the cooling solenoid. Since the magnetic field has to be adjusted during the accelerator operation, the measurement system is installed inside vacuum chamber. The design and features of this system are described in the article, as well as preliminary results are discussed.
|
|
|