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 Petrović2nd 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 employees2nd 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, Greece2nd 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 682nd 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 nA2nd 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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