Presentation of Laboratory of Physics VINČA Institute of Nuclear Sciences Belgrade, Serbia - Dr Srdjan Petrović
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2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Presentation of Laboratory of Physics VINČA Institute of Nuclear Sciences Belgrade, Serbia Dr Srdjan Petrović
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Laboratory of Physics, Vinča Institute of Nuclear Sciences, University of Belgrade, Serbia • Science with Accelerators group – 22 employees (5 engineers and 6 technicians) • Advanced materials group – 16 employees • Physics and Detector Research and Development in High Energy Physics Experiments group – 5 employees • High Energy Physics with the CMS Detector group – 5 employees
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece International collaboration • CERIC – Central European Research Infrastructure Consortium • Joint Institute for Nuclear Research (JINR), Dubna, Russia • European Organization for Nuclear Research (CERN), Geneva, Switzerland • Two HORIZONT 2020 projects • Several coordination actions (COSTS) funded by the European Commission, bilateral and national projects funded by the Serbian MESTD • Coordinators in collaboration agreements between the Vinča Institute and Institute of High Energy Physics of the Chinese Academy of Science, Institute of Nuclear Physics, NCSR “Demokritos”, Athens, and National Technical University of Athens, Greece
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Historical introduction The TESLA Accelerator Installation, in the Vinča Institute of Nuclear Sciences, is a facility for use of ion beams in science and medicine. Its construction began in December 1989, on the basis of a special decision of the Government of Serbia. However, the endeavor was going on with frequent and long delays, due to the irregular and insufficient financing, caused dominantly by the severe political and economic crisis in Serbia. In November 2007, the Government of Serbia decided to stop the financing of construction of TESLA from the budget of Serbia and to continue it on the basis of the clearing debt of Russia to Serbia. The question was: to continue the construction of TESLA or to surrender and stop it? Our choice was to continue.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece In accordance with that decision of the Government of Serbia, we decided to divide TESLA in three parts – the low, medium and high energy parts. The reason was our conviction that it would be easier to fight for the completion of construction of these parts separately than for TESLA as a whole. The parts of TESLA and the programs of their use are: The low energy part, which was named FAMA – facility for modification and analysis of materials with ion beams, is a user facility for research in the field of modification and analysis of materials with ion beams. The medium energy part, which was named the H4 Facility, should be used for industrial production of radiopharmaceuticals with a cyclotron giving proton beams of the energies between 13 and 19 MeV, primarily for positron emission tomography. The high energy part comprises the VINCY Cyclotron, designed to give proton beams of the energies between 30 and 75 MeV, and its experimental channels should be used for routine proton therapy of eye tumors, radiation research, modification and analysis of materials, and physics of thin crystals. We have also decided to use the clearing debt of Russia to Serbia to upgrade FAMA.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Structure of FAMA FAMA comprises two parts: 1) Experimental set-up for modification of materials with ion beams (IBMM), consisting of: M1 – ECR ion source - multiply charged heavy ions, M2 – multicusp ion source - singly charged positive and negative light ions, C1 – channel for irradiation of monocrystalline targets, C2 – channel for irradiation of materials. 2) Experimental set-up for analysis of materials with ion beams (IBA), consisting of: M3 – proton cyclotron complex, C5 – channel for IBA in vacuum, C6 – channel for IBA in air.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece A three-dimensional view of the experimental set-up for modification of materials with ion beams In the future, two additional experimental channels, C3 and C4 should be included.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece M1 – ECR ion source Commissioned in May 1998. Constructed by the Joint Institute for Nuclear Research, Dubna, Russia, in close collaboration with the Vinča Institute. Refurbished in 2014.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Some of the ion beams produced with the extraction voltages between 15 and 20 kV Energy Current Ion species (keV) (eµA) Energy Current 4Hе+ Ion species 15 760 (keV) (eµA) 4He2+ 30 410 56Fe7+ 105 79 11B3+ 45 305 64-68Zn7+ 105 77 12C2+ 30 230 64-68Zn10+ 150 32 12C4+ 60 128 84Kr12+ 180 135 14N5+ 100 733 84Kr14+ 210 60 14N6+ 120 205 136Xe23+ 460 62 16O5+ 75 660 136Xe26+ 520 23 16O7+ 105 37 176-180Hf12+ 180 43 20Ne5+ 75 560 207Pb21+ 420 42 20Ne8+ 120 48 207Pb26+ 520 9 40Ar8+ 160 720 40Ar12+ 240 68
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece M2 – multicusp volume ion source It was commissioned in July 1997, as the light ion source of the VINCY Cyclotron. It was constructed by AEA Technology, Abingdon, Great Britain. From January 1998, the machine has been being used for surface modification of materials with light ion beams.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Some of the ion beams produced with the M2 machine with the extraction voltages between 16 and 30 kV Ion energy Ion current Ion species (keV) (eµA) H 30 1,480 H2+ 20 600 H3+ 20 960 D 18 420 4He+ 16 320 It can also produce H+, D+, D2+ and D3+ ion beams.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece C1 channel: Manufactured by Efremov Institute, St. Petersburg, Russia – presently in the phase of commissioning. To be used for irradiation of monocrystalline targets. The monocrystalline target holder assembly consists of a six-axis goniometer with the options of cooling (liquid nitrogen) and heating (electron gun) up 1 000 C0.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece C2 channel: constructed by Danfysik, Jyllinge, Denmark. Used for modification of materials with ions from M2 machine - various metal, semiconductor, carbon, polymer and ceramic targets. The interaction chamber of the C2 channel also includes the equipment for applying the technique of ion beam assisted deposition (IBAD), which can be combined with the technique of ion bombardment.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Cyclotron complex for Ion Beam Analysis of Materials C5 channel in vacuum: Rutherford backscattering spectrometry (RBS), proton induced X-ray emission (PIXE) spectroscopy and proton induced gamma-ray emission (PIGE) spectroscopy. C6 channel in air: PIXE and PIGE spectroscopies. Characteristics of the produced proton beam •Energy – between 1 and 3 MeV •Energy precision – below 1 keV •Energy spread – below 0.1 % •Current – between 10 and 100 nA
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece In the C5 channel, one will be able to analyse various materials in vacuum by Rutherford backscattering spectrometry (RBS), proton induced X-ray emission (PIXE) spectroscopy and proton induced gamma-ray emission (PIGE) spectroscopy.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece In the C6 channel, one will be able to analyze various materials in air by PIXE and PIGE spectroscopies.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Program of use of FAMA FAMA represents the largest part of the research infrastructure and the only user facility in Serbia. The program of its use is focused on new materials and directed to nanotechnologies. So far, 13 user groups from Serbia, two groups from Russia one from South Africa and one group from Greece have participated in its realization. The realization of the program of use of FAMA is controlled by the FAMA Advisory Committee – an expert body formed by the Ministry of Education, Science and Technological Development of Serbia in April 2014. The members of the Committee are: Prof. Hans Hofsäss, from the University of Göttingen, Germany, Prof. Roger Webb, from the University of Surrey, Guildford, Great Britain, and Prof. Mark Breese, from the University of Singapore.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece FAMA has potential for being a unique and valued facility in the region. The low energy cyclotron design is unique for this kind of work and the high beam currents of low mass ions could provide a capability rarely available elsewhere. Despite the funding difficulties, there is still quite an extensive user program that is managing to continue at FAMA. The nearest facilities with similar equipment are in Ljubljana and Zagreb. Both of these user facilities are compatible with FAMA, having in mind its ion implantation capability.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece CERIC-ERIC comprises the following user facilities: 1. The synchrotron light source ELETTRA, in Trieste 2. The synchrotron light source SOLARIS, in Krakow 3. The nuclear reactor in the Budapest Neutron Center 4. The accelerator facility in the Rudjer Boskovic Institute, in Zagreb 5. The instruments for light scattering in the Institute of Inorganic Chemistry of the Technical University of Graz 6. The instruments in the Surface Physics Laboratory of the Charles University, in Prague 7. The instruments for electron paramagnetic resonance and electron microscopy in the National Institute for Materials Physics, in Bucharest 8. The instruments for nuclear magnetic resonance in the National Institute of Chemistry, in Ljubljana FAMA is open to the users from all these institutions, and all these facilities will become open to the users of FAMA. “One shot proposal“.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Axial ion crystal channeling effect The scheme of axial ion channeling and dechanneling in a crystal channel.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Ion crystal channeling implantation Ion crystal channeling implantation is characterized by: A. Greater implantation depth, in comparison with the random ion implantation, and asymmetry in the ion concentration depth profile. B. Minimization of the induced crystal lattice damage. C. Sensitivity of choice of the interatomic potential, providing an excellent tool for studying the basic properties of the ion–solid interaction.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece M. Erić, S. Petrović, M. Kokkoris, A. Lagoyannis, V. Paneta, S. Harrisopulos and I. Telečki, Depth profiling of high energy nitrogen ions implanted in the , and randomly oriented silicon crystals, Nuclear Instruments and Methods in Physics Research Section B 274, 87–92 (2012). V. Paneta, M. Erich, S. Fazinić, M. Kokkoris, I. Kopsalis, S. Petrović and T. Tadić, Investigation of deep implanted carbon and oxygen channeling profiles in [110] silicon, using d-NRA and SEM, Nuclear Instruments and Methods in Physics Research Section B 320, 6–11 (2014).
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Future experiments using FAMA C1 channel Concentration depth profile of 100 keV Concentration depth profile of 100 keV carbon ions along Si crystal carbon ions in the random orientation in channels, calculated by using the Si crystal, calculated by using the MARLOWE code. MARLOWE code.
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Superfocusing effect of channeled ions N. Nešković, S. Petrović, and D. Borkа, Superfocusing of channeled protons and crystal rainbows, Nuclear Instruments and Methods in Physics Research B 267, 2616-2620 (2009). S. Petrović, N. Nešković, V. Berec, and M. Ćosić, Superfocusing of channeled protons and subatomic measurement resolution, Physical Review A 85, 032901/1–032901/9 (2012).
2nd Workshop of ENSAF, Oct. 3-4, Athens, Greece Thank you for your attention
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