Status of the S ource of P olarized I ons for the JINR accelerator complex

1. Status of the Source of Polarized Ions for the JINR accelerator complex V.V. Fimushkin, A.D. Kovalenko, L.V. Kutuzova, Yu.V. Prokofichev • Joint Institute for Nuclear Research, Dubna A.S. Belov • Institute for Nuclear Researchof Russian Academy of Sciences, Moscow V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

2. Studies of the structure of light nuclei including the deuteron and features of strong interactions using beams of polarized deuterons accelerated at the Synchrophasotron- weak-focusing 10 GeV proton synchrotron - have been started at the Laboratory of High Energies (LHE, JINR) since the middle of the80s Since 2003 these studies have been continued at the NUCLOTRON - a strong focusing superconducting 6AGeVheavy ion synchrotron that was put into operation in 1993 The basic problem of this machine in comparison with the Synchrophasotronis one-turn injection The NUCLOTRONinjection time is limited to about 8.36 µs whereas it was about 200µs for the old accelerator That's why the development of a newhigh intensity polarized ion source is considered as a very important high priority task V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

3. The NICA Collider Layout Colider 4T (CRing = 251.5 m) September 2009 Colider 2T- 534 (CRing = 534 m) July 2010 Collider 2T - 350 (CRing = 350 m) February 2010 The new flagship JINR project in high energy nuclear physics, NICA(Nuclotron-based Ion Collider fAcility), aimed at the study of phase transitions in strongly interacting nuclear matter at the highest possible baryon density, was put forward in 2006 V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

4. The NICAprogram consists of several subprojects • The one of them is the project NUCLOTRON-M, where the new polarized ion source is included in, because the existing 0.4 mA ↑D+ cryogenic source POLARIS cannot provide some of the key parameters necessary for the new facility • Physics with polarized light ion beamsis considered as an important part of the NICA collider programalso • The expected luminosity is planned at the level of (1030 -1031) cm-2·s -1 V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

5. D+ CRYOGENIC SOURCE POLARIS The source was used long time atthe Synchrophasotron since the beginnings of the 80th. An atomic beam forming process is required to pump a large mass of injected gas. There was no developed turbopump technology that time yet. It was decided to apply cryocondensation of deuterium molecules on cooled surfaces The source consists of two LHe cryostats: a pulsed atomic beam stage with two superconducting sextupole magnets, - the Penning plasma ionizer with high field SC solenoid The energy of the deuteron beam at the output of the source is about 3 keV, the current: 0.3-0.4 mA The vector and tensor polarizations are: Pz ~ +/-0.54, Pzz ~ +/- 0.76. V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

6. Further development of the polarization program at NUCLOTRON/NICA facilitysupposes the substantial increasing of pulsed intensity of source of the polarized light nuclei • The new project:SourceofPolarizedIonsproject (SPI-project) assumes the design and production of the universal high-intensity source of polarized deuterons & protons • As the first step the increase of intensity of the accelerated polarized D+ beam is supposed • The important fact is depolarization resonances are absent in the total energy range of the NUCLOTRON-M but only for the deuteron beam The main purpose of the SPI-project is to increase the intensity of the accelerated polarized beams at the JINR Accelerator Complex up to 1010 d/pulse V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

7. The SPI-project assumes thedevelopment of the source using charge-exchange ionizer. Nearly resonant charge-exchange reactions for production of polarized protons & deuterons are: H0 + D+ H+ + D 0 D0 + H+ D+ + H0 ~ 5 10-15 cm2 • The design output current of the SPIis up to 10 mA for D+ ( H+) • The D+polarization will be up to 90% of the maximal vector (±1) & tensor (+1,-2) polarization • The SPI-project is based in substantial part on the equipment which was supplied within the framework of the Agreement between JINR & IUCF(Bloomington, USA) The project is realized in close cooperation with INR of RAS (Moscow, Russia) V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

8. The SPI-project includes the following stages: • development of the high-intensity Source of Polarized Ions • complete tests of the SPI • modification of the linac pre-accelerator platform & power station • adaptation of the existing remote control system (console of linac) of the SPIunder the high voltage • mounting of the SPIand equipment at the pre-accelerator platform, • linac runs with polarized beams and polarization measurements at the linac output V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

9. The most labour-consuming and expensive work is development of theSource of Polarized Ionsbased on the equipment of Cooler Injector Polarized IOn Source (CIPIOS) developed at Indiana University Cyclotron Facility (IUCF, USA) in cooperation with the INR of RAS (Moscow) in 1999 Acknowledgements • The big work on transfer of the CIPIOS equipment from IUCF in Dubna has been done by V.P. Derenchuk Indiana University Cyclotron Facility, USA V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

10. Some CIPIOS parts delivered to LHEP-JINR from IUCF

11. CIPIOSincludes - source of the polarized atoms using the permanent sextupole magnets (B= 1.4 T)for focusing and electron spin separation - radio frequency transitions units of nuclear polarization - resonant charge-exchange ionizer (the polarized ion are formed at resonant charge-exchange of the polarized atoms and unpolarized ions in plasma) - specialspin orientation system at the output of CIPIOSin vertical position • Note: CIPIOS was intended for high-intensity negative polarized and unpolarized beams production V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

12. Cooler Injector Polarized Ion Source (CIPIOS)

13. V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

14. INR source of polarized protons • It is known that at INR the source of polarized protons with the charge-exchange plasma ionizer and the polarized atom storage in the ionization volume has been developed : Characteristics of polarized H+ (H-) ion beam of the INR source H+ Without polarized atom storage Intensity 6 mA Polarization 85% With polarized atom storage Intensity 11mA Polarization 80% H- Intensity 4 mA Polarization 90% V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

15. V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

16. V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

17. INR source with a storage cell Length 250 mm Internal diameter 15 mm Material Al • Density of polarized hydrogen atoms in an ionization region of a polarized ion source can be increased in comparison with free polarized atomic hydrogen beam by using of a storage cell • This was tested at INR: 11 mA H+ beam has been obtained with 80 % polarization V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

18. I, μA 1.0 2.0 3.0 4.0 5.0 6.0 T, ms Dynamics of polarized H+ ions from the ionizer with the storage cell in comparison with the H+ current obtained without the storage cell. The background H+ current is also shown. Solid line is from calculation. V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

19. Polarization of proton beam from the ionizer of ABS with storage cell vs time V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

20. The ionizer with storage ofpolarized atoms for the SPI allows - increase intensity of the polarized ion beam, - reduce emittance of the polarized beam - considerablyreduce H2+ion current which isdifficult to be separated from polarized D+ due to similar mass of the ions. V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

21. The NUCLOTRON feature is that single-turn injection is only possible and this machine accept only positive ions Therefore it is expedient to use the source of positive polarized deuterium ions Note:The highest intensity of the beam is reached forpositive polarized ion sources with charge-exchange plasma ionizer and the storage cell • SPI-sourceassumes to convert the charge-exchange ionizer of CIPIOS into the ionizer using storage of polarized deuterium atoms and production of positive polarizeddeuterons by resonance charge-exchange in the hydrogen plasma V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

22. Because the transferred equipment of the CIPIOS was not fully completed, the development and manufacturing of missing modules and parts of the new SPI was required. Mainly it concerns of the AtomicBeamSource(ABS) These are: • vacuum chamber of the ABS and sextupole magnets • dissociator • system of the atomicdeuterium (hydrogen) beamcooling at fast pulse valve of molecular deuterium (hydrogen)injectioninto the dissociator bulb • (H2, D2, O2) pulsed gas supply system • high-frequency pulse generator (pulse power up to5 kW, 50 MHz ) • modulator of the high-frequency generator (maximum voltage up to 4.5 kV and a pulse current upto 2 A) In addition acquisition of the missing equipment and devices for the source is also necessary V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

23. The designing and manufacture of ABS parts, optimization of the intensity of the atomicbeam, and functional tests of the RF cells of the nuclear polarization of deuterium (hydrogen)atoms will be performed at INR Special attention during the tests will be focused at the problems of the atomic deuteriumbeam formation process and study of the RF-transitions efficiency under nuclear polarization of the atomic deuterium beam V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

24. The RF-transitionunits will be checked and tuned with a sextupole electromagnet as an analyzing device V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

25. Thepurpose is to get atomic Dbeam with the pulse density of 2.5 ·1010 at/cm3 at the distanceof 150cm from the cooling channel outlet and the most probable velocity of 1.5 ·105 cm/s V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

26. Atomic Beam Source general view (INR test bench) Pulsed dissociator (INR-type), nozzle cooling to 70 K, set of permanent magnet sextupoles and electromagnet sextupole (CIPIOS), WF and SF RF transitions units. Expected intensity of polarized deuteron beam is 1.5 ·1017sec-1 (3 ms pulse),polarized hydrogen beam - 2·1017sec-1 V.Fimushkin, A.Belov , A.Kovalenko, L.Kutuzova, Yu. Prokofichev at PST&P2011

27. Pump, Turbo-V 3K-T, 2300 l/s H2 , 2400 l/s He - 2 item Pump, Turbo-V 2K-G, 1600 l/s N2 - 2 item Fore pump Dry scroll pump type TriScroll 600 Inverter, 30m³/h-2 item Cryocooler, Single Stage Cryodyne Refrigeration System, Model 350 will provide 40 watts of heat lift at 77K Pressure measurement system, MaxiGauge TPG256A controller for 6 gauges Total price of equipment ~ 190 K$ equipment is already purchased ABS will be purchased this year Power supply Sorensen SGI40X375C-1CAA (40V, 375A, 15kW) -ABS sextupole Power supply Sorensen DCS 8-350E (8V, 350A, 3 kW) Power supply Sorensen DCS 12-250E (12V, 250A, 3 kW)- ionizer solenoid Power supply Sorensen XG 8-200 (8V, 200A, 1.6 kW) Power supply Sorensen DCS20-150E (20V, 150A, 3 kW)- bending magnet of the ionizer ABS&IONIZER Power supply Sorensen XG 40-42 (40V, 42A, 1680 W) - ABS arc source Total price of equipment ~ 40 K$

28. 23.04.2011 (INR test bench)

29. Atomic Beam Source setup general view (from the right side) TOF MS ABS INR test bench

31. Cryocooler Single Stage Cryodyne Refrigeration System, Model 350

32. Some electronic devices of Atomic Beam Source High Voltage modulator of RF-generator (rear view) Pulse valve power supply High Voltage modulator of RF-generator(manufacturing process)

33. Status of the ABS development • The ABS parts have been assembled • Vacuum leaks have been eliminated • Vacuum tests have been performed • Residual vacuum pressure ~ 1 ·10-6 mbar has been obtained in all vacuum chambers of the ABS • Cryocooler CTI has been mounted on the dissociator chamber of the ABS • The cryocooler normal operation has been tested • The gaseous system of the ABS includes two pulsed gaseous valves (D2/H2 and O2) • The gaseous system is under tests at present

34. The work which is carried out at JINR includes • - assembly and tests of the charge-exchangeplasmaionizer, including the storage cell in the ionization volume • transportation ofhydrogen plasma with the flow of unpolarized protons up to 100 mA through the storagecell • - optimization of the ion-optical system up to 25 keV and transport of the high-current deuteron beam • - long-term tests of the SPIwith the storage cell in the ionizer - polarimetry of the accelerated beam at the output of linac It is necessary to developcontrol system components for primary analysis & data acquisition and for fiberoptic system of data transmission

35. NEW SOURCE OF POLARIZED IONS (DEUTERONS) H2 ↑D+ → D2→D→ D →→ D0+ H+D++ H0 D2

36. SPI front view ABS chamber ABS sextupole extraction chamber charge-exchange ionizer chamber ABS dissociator chamber arc plasma source chamber SPI supporting frame HV terminal

37. SPI side view Turbo-V 2K-G, 1600 l/s N2 into RFQ & linac Cryocooler Turbo-V 3K-T 2300 l/s H2 Solenoid of the spin-precessor HV terminal (150kV) SPI supporting frame

38. Hydrogen (deuterium) plasma generator Arc plasma source Fast gas valve

39.  D+ (  H+) extraction system of the charge-exchange ionizer 4 - electrodes ion optical system HV - shield

40. Spin precessor system electrostatic lens electrostatic mirror

41. General view of SPI & high-voltage terminal at the linac (Lu-20) Charge-exchange plasma ionizer hard ware status 70%ready Extraction chamber hard ware status ready ABS hard ware status ready

42. Assembly of the charge-exchangeplasmaionizer(JINR responsibility)

43. Assembly of the charge-exchangeplasmaionizer

44. Arc plasma source tests of equipment

45. Summary & Outlook • Intensive work on preparation of the ABS for tests is carried out at INR of RAS (Moscow) • Operating tests of the ABS systems are planned in 2011 • The first tests of the SPI charge-exchange ionizer at JINR are planned in 2011 also

46. Thank you