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target

Paper Title Other Keywords Page
TUCHY01 Muon Collider Design Status emittance, collider, proton, acceleration 20
 
  • Y. Alexahin
    Fermilab, Batavia
  Muon Collider (MC) - proposed by G. I. Budker and A. N. Skrinsky almost half a century ago - is now considered as the most exciting option for the energy frontier machine in the post-LHC era. A national Muon Accelerator Program (MAP) is being formed in the USA with the ultimate goal of building a MC at the Fermilab site with c.o.m. energy in the range 1.5-3 TeV and luminosity of ~1-5*1034 cm-2s-1. As the first step on the way to MC it envisages construction of a Neutrino Factory (NF) for high-precision neutrino experiments. The baseline scheme of the NF-MC complex is presented and possible options for its main components are discussed.  
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TUPSA003 Study of Efficiency of Beam Collimation at U-70 Accelerator by Use of Crystal Targets collimation, proton, kicker, extraction 38
 
  • I. A. Yazynin, A. G. Afonin, V. T. Baranov, S. A. Belov, V. N. Chepegin, Y. A. Chesnokov, P. N. Chirkov, A. D. Ermolaev, V. N. Gorlov, I. V. Ivanova, D. M. Krylov, V. A. Maisheev, D. A. Savin, E. A. Syshikov, V. Terekhov
    IHEP Protvino, Protvino, Moscow Region
  New crystal technique – bent crystal array and veer – type reflector based on straight crystals were used like first stage in collimation system at U-70 accelerator. Efficiency of collimation was enhanced up to 90% in two-stage collimation system which included first crystal stage and long steel absorber like second stage. While in previous one-stage system without crystal only 40% protons hit deeply in absorber. For data taking and analysis of information modified modern beam diagnostic system was applied.  
 
TUPSA018 Intercation of the Biomolecular Ions with the Electron Target in the Electrostatic Storage Ring ion, electron, storage-ring, resonance 80
 
  • S. G. Shirkov
    JINR, Dubna, Moscow Region
  A nanostructure of the radiation damages is formed at an interaction of decelerated protons or carbon ions with DNA molecules at hadron therapy. A local interaction of the ion beam with the bimolecular structures in the human cells is defined mainly by parameters of the ion tracks. The track core is connected with ionization properties of the charged ion, its cross-section sizes are defined by the delta-electrons. The delta-electron energy varies statistically from several eV to few keV therefore they lead to substance ionization along their trajectory on a distance several nanometers from that point where they were produced. Interaction of the delta-electrons with DNA molecules and other biological structures is one of the important mechanisms realized in process of the hadron therapy. A study of interaction of the accelerated biomolecular ions with an electronic target in electrostatic storage ring was performed for modeling of an input of the delta-electrons in processes of the hadron therapy.  
 
TUPSA020 Development of Injector for ITEP Heavy Ion Synchrotron Based on Laser Plasma Generator laser, ion, plasma, heavy-ion 86
 
  • Yu. A. Satov, N. N. Alexeev, A. Balabaev, A. D. Belokurov, I. D. Hrisanov, B. Y. Sharkov, A. Shumshurov, A. A. Vasilyev
    ITEP, Moscow
  A schematic diagram of heavy ion injector based on laser ion sources is described. Two different basic laser configurations used in ITEP synchrotron. First laser excels in simplicity and consists of CO2 free-running laser that is applied for carbon target plasma heating and ionization at laser power density q=3·1012W/cm2 to create high current C4+ ion beam. Second master oscillator-amplifier (MOPA) laser configuration intends for production super high laser intensity at a target to provide considerable charge state in a plasma of heavy elements (Al, Fe, Ag etc). This laser configuration is founded on original physical principle* that simplifies the installation and ensures high reliability for long term operation. Laser characteristics for the different laser scheme and ion current for injector outlet beam of C4+ and Ag+19 are shown in this paper. The latter was accelerated in synchrotron for energy up to 100 MeV/u.

* K. N. Makarov et al. Quantum Electronics (Russian), 2001, 31 (1), pp. 23-29

 
 
TUPSA026 RTS&T Code Status simulation, radiation, resonance, ion 92
 
  • I. I. Degtyarev, O. A. Liashenko, F. N. Novoskoltsev, I. A. Yazynin
    IHEP Protvino, Protvino, Moscow Region
  • A. I. Blokhin
    Institute of Physics and Power Engineering (IPPE), Obninsk
  The paper describes the main features of the RTS&T–2010 — the modern version of the RTS&T (Radiation Transport Simulation and Isotopes Transmutation problem) code system. RTS&T performs detailed Monte Carlo simulations of many type of particles transport in complex spatial geometries with composite materials in the energy range from thermal energy up to 100 TeV. The RTS&T code considers interaction of low-, intermediate-, and high- energy particles with condensed matter, including hadron-nucleus interactions inside the target, generation and transportation of secondary particles, deposition of energy and production of radionuclides in the target. Recently, the transfer of ions was added and tested.  
 
WECHZ02 Progress with the 2 MeV Electron Cooler for COSY-Juelich/HESR electron, antiproton, vacuum, pick-up 147
 
  • J. Dietrich, V. Kamerdzhiev
    FZJ, Jülich
  • M. I. Bryzgunov, A. D. Goncharov, V. V. Parkhomchuk, V. B. Reva, D. N. Skorobogatov
    BINP SB RAS, Novosibirsk
  The 2 MeV electron cooling system for COSY-Juelich was proposed to further boost the luminosity even in presence of strong heating effects of high-density internal targets. The project is funded since mid 2009. Manufacturing of the cooler components has already begun. The space required for the 2 MeV cooler is being made available in the COSY ring. The design and construction of the cooler is accomplished in cooperation with the Budker Institute of Nuclear Physics in Novosibirsk, Russia. The 2 MeV cooler is also well suited in the start up phase of the High Energy Storage Ring (HESR) at FAIR in Darmstadt. It can be used for beam cooling at injection energy and is intended to test new features of the high energy electron cooler for HESR. The technical layout of the 2 MeV electron cooler is described and the status of component manufacturing is reported.  
 
WEPSB013 Reconstruction of the Beam Parameters and Structure Characteristics for INR Isotope Channel linac, emittance, proton, quadrupole 196
 
  • V. A. Moiseev, S. Bragin, A. Feschenko, O. V. Grekhov, Yu. V. Kiselev, A. N. Mirzojan, O. Volodkevich
    RAS/INR, Moscow
  The various treatments of profile measurements have been applied to estimate both the major beam parameters and structure functions for the INR isotope channel. The main problem for beam dynamics reconstruction consists in the presence of the dispersion function along the beam line studied. The reliable results were obtained and used to form the beam on the target of INR isotope complex.  
 
THCHA01 The Nonlinear Transformation of a Ions Beam in the Plasma Lens plasma, ion, focusing, luminosity 280
 
  • A. A. Drozdovsky, N. N. Alexeev, S. A. Drozdovsky, A. Golubev, Yu. B. Novozhilov, P. V. Sasorov, V. V. Yanenko
    ITEP, Moscow
  The focusing capabilities of a plasma lens depend on the stage of plasma development. Under certain conditions a magnetic field is linear, that allow to focus the beam to a very small spot. In other conditions, the magnetic field is nonlinear, that allow formation of hollow and others beam structures. The work deals with the study of the last type of a plasma lens. Calculations and measurements were performed for a C+6 and Fe+26 beams of 200 MeV/a.u.m. energy. The obtained results and analysis are reported.  
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THCHZ01 First Radiocarbon Measurements at BINP AMS ion, background, ion-source, vacuum 309
 
  • S. Rastigeev, A. R. Frolov, A. D. Goncharov, V. Klyuev, E. S. Konstantinov, S. G. Konstantinov, L. A. Kutnykova, V. V. Parkhomchuk, M. Petrichenkov, A. V. Petrozhitskii
    BINP SB RAS, Novosibirsk
  Present status of the BINP accelerator mass spectrometry (AMS) facility is described. The results of experiments for beam selection and radiocarbon concentration analysis in trial samples are presented.  
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THCHZ02 High Power ELV Accelerators for Industries Application controls, electron, extraction, radiation 313
 
  • N. K. Kuksanov, S. Fadeev, Yu. I. Golubenko, D. A. Kogut, A. I. Korchagin, A. Lavrukhin, P. I. Nemytov, R. A. Salimov
    BINP SB RAS, Novosibirsk
  Beginning from 1971, the Budker Institute of Nuclear Physics Siberian Branch of Russian Academy of Science (SB RAS) started its activity in the development and manufacturing of electron accelerators of the ELV-type for their use in the industrial and research radiation-technological installations. The family of ELV-type accelerators has the energy range from 0.4 to 2.5 MeV with a beam of accelerated electrons of up to 100 mA and maximum power of up to 100 kW for ordinary accelerators and 400 kW power for environmental purpose accelerator. The ELV accelerators are especially popular accelerators not only in Russia, but in China, Korea, and etc. BINP continuously improves design and increases parameters of accelerators. Due to this circumstance and improving of economics after crisis amount of orders for accelerators extremely increased.  
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THPSC010 The Electron Linear Accelerator LUE-200 - Driver the IREN Facility electron, gun, focusing, klystron 346
 
  • V. Kobets, J. Boettcher, A. S. Kayukov, I. N. Meshkov, V. Minashkin, V. G. Pyataev, V. A. Shvets, V. N. Shvetsov, A. P. Sumbaev, V. N. Zamriy
    JINR, Dubna, Moscow Region
  • P. V. Logachev, V. M. Pavlov
    BINP SB RAS, Novosibirsk
  • V. Shabratov
    JINR/VBLHEP, Moscow
  It is reported on startup of the first stage of the Intense REsonance Neutron source installation (IREN) at the Frank Laboratory of Neutron Physics of the Joint Institute for Nuclear Research. The general scheme and current status of the electron linear accelerator with accelerating structure on a S-band traveling wave (f = 2856 MHz) are presented. Results of adjustment of the basic functional systems of the linac and the measured parameters of the beam (pulse current of a beam – 3.0 A, electron energy - 30 MeV; duration of a pulse current - 100 ns; rep. rate - 50 Hz) are reported. The integral neutron yield from nonmultiplying target reaches (3…5)*1010 n/s.  
 
THPSC022 Development and Application of Electron Linac Electromagnetic Devices for Radiotechnologies linac, electron, controls, pick-up 369
 
  • V. A. Shendrik, A. N. Dovbnya, A. E. Tolstoy
    NSC/KIPT, Kharkov
  The creation and subsequent service of modern electron linear accelerators at the NSC KIPT have brought evidence for possible successful introduction of radiotechnology processes using electron irradiation. A further extension and complication of physical problems solvable on the basis of radiotechnologies have put forward new and increased requirements for the systems of beam scanning, extraction and formation on the targets and extended irradiated objects. The results of applying our methods developed for prompt measurement of the kinetic energy of the scanned electron beam are presented. For measurement and continuous control of the electron energy the hodoscope magnetic spectrometer technique has been used. The spectrometer includes only one deflecting magnet and has no magnetic focusing. If the real field topography in the magnet is known in detail, then using the input and output coordinates of deflected particles it is possible to determine their energy, and also the chromaticity of electron beam. The step-pulse scanning of the beam is realized through the use of an air-core short-pulse electromagnet. Development and tests of separate units of the device are under way  
 
THPSC026 Status of HITS Injector ion, ion-source, vacuum, tandem-accelerator 376
 
  • A. V. Semenov, V. G. Cherepkov, V. Klyuev, E. S. Konstantinov, E. A. Kuper, V. R. Mamkin, A. S. Medvedko, P. I. Nemytov, V. V. Repkov, V. B. Reva, R. A. Salimov, D. V. Senkov, V. A. Vostrikov
    BINP SB RAS, Novosibirsk
  Ion injector for cancer therapy facility HITS was designed and assembled at BINP. Injector is based on electrostatic tandem accelerator with 1.25 MV at the high voltage terminal. The negative ion beams are injected into tandem and charge exchanged in the vapor-magnesium target with vacuum heat insulation. The results of injector tests and working with carbon ion beam are presented.  
 
THPSC029 UEL-10-D New Linear Electron Accelerator for Non-Destructive Testing electron, controls, focusing, power-supply 382
 
  • I. Yu. Vakhrushin, V. Alexeev, L. Z. Kavalerchik, A. P. Klinov, A. S. Krestianinov, K. N. Maslov, Yu. P. Shchepin, M. F. Vorogushin
    NIIEFA, St. Petersburg
  A compact accelerator UEL-10-D for radiographic inspection of steel products up to 500mm thick has been designed and manufactured. The accelerator provides the 10 MeV energy and the photon dose rate 1m from target of 30Gy/min. The accelerator consists of an irradiator mounted on a yoke, heat-exchanger and industrial panel computer. The equipment of the accelerator is mostly located inside the irradiator including the HV power supply system, magnetron modulator and control system blocks. Using this yoke, the irradiator is installed on a bridge crane, which ensures its high manoerability necessary to test products of complicated geometry. Size of the irradiator without yoke is 2040*950*950 mm. In 2010, the accelerator was put into operation at the "Izhorskie Zavody", St. Petersburg. The UEL-10-D accelerator can be also used in radioscopic or tomographic systems.  
 
THPSC031 The Use of the Electron Beam from the Magnetron Gun-Based Accelerator for Zirconium Surface Modification electron, cathode, gun, vacuum 384
 
  • V. Zakutin, A. N. Aksyonova, A. N. Dovbnya, S. D. Lavrinenko, V. N. Pelykh, N. N. Pilipenko, N. G. Reshetnyak
    NSC/KIPT, Kharkov
  The paper presents the results of investigations on the zirconium specimen surface after irradiation them with an electron beam from the accelerator. The operating conditions were the following: electron energy from 7 to 80 keV, pulse duration of 15 μs, pulse frequency of 2 Hz. for two modes of the energy density on the samples, namely, 10 J/сm2 and 20 J/сm2. The experiments have demonstrated that the irradiation leads to the noticeable smoothing of the specimen surface roughness, the surface becomes smoother and unruffled. The results of investigations on the microhardness of irradiated and unirradiated areas of the zirconium specimen surface areas show that the microhardness value has been increased by ~20% of the initial value (1920 MPa) for the irradiation energy density of 10 J/cm2 and by ~35% for 20 J/cm2, that can be related with a different quantity of an transferred energy of the irradiated surface. By choosing the optimum electron irradiation characteristics this technique may be recommended for hardening and modification of the near-surface layer of zirconium materials applied in the nuclear-power engineering.  
 
THPSC034 Ion Scanning System in Beam Line of U-400M Cyclotron for Electronic Components Testing ion, controls, cyclotron, extraction 387
 
  • A. A. Fateev, E. V. Gorbachev, G. G. Gulbekyan, I. V. Kalagin, V. I. Kazacha, N. Yu. Kazarinov, E. V. Muravieva
    JINR, Dubna, Moscow Region
  The channel B5 of the U-400M cyclotron is designed for irradiation of integrated circuits by beams of accelerated ions to determine their radiation resistance. The results of the beam transport calculations for various ion types taking into account the beam parameter changes on passing a collimator and degrader are presented. The resulting beam size on a target is obtained for all beam variants. The calculated beam size on the target varies in the range from 15 cm up to 30 cm. An analysis of three variants of the magnetic scanning system is made. The working scheme, construction and main technical characteristics of the optimal variant are presented.  
 
THPSC035 Compromise Systems for Transport Proton and Ion Beams in Medical Aims ion, proton, quadrupole, beam-transport 390
 
  • M. M. Kats
    ITEP, Moscow
  Traditional GANTRY is not suitable for future centers of therapy by proton or ion beams by reasons of its enormous size, rotation with precision of significant mass, huge electricity consumption and extremely high cost. Review of various compromise solutions for beam transport to a patient is presented in the report: horizontal beam, rotation of patient around the vertical axis, beams with fixated directions, beams with fixated directions and with additional patient rotation around the horizontal axis (with the use of tomography and with additional adjustment after each rotation) and planar systems in different versions. It was shown that planar systems are the most promising solution at the present moment.  
 
FRCHX01 The High-Current Deuteron Accelerator for the Neutron Therapy ion, controls, radiation, power-supply 399
 
  • V. M. Skorkin, S. V. Akulinichev, A. V. Andreev
    RAS/INR, Moscow
  Physical project of neutron sources for the neutron therapy and neutron activation analysis is proposed. The neutron sources are based on beam provided by the high-current deuteron accelerator. Neutron sources produces 14 MeV fast neutrons with intensity up to 5*1012 n/s using T(D,n)4He threshold reaction at the energy of deuteron beam about 400 keV and average current up to 20 mA. Neutron source can be makes for neutron capture therapy (NCT) by using of moderator system consisted of the tungsten converter, bismuth reflector, graphite and polyethylene. Liquid-crystalline DNA-Gd nanoparticles, as a potential biomaterial for NCT were investigated on the thermal neutron beam.

S. V. Akulinichev, A. V. Andreev
Institute for Nuclear Research of RAS, Moscow, Russia

 
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FRCHA02 ELLUS-6M Linear Electron Accelerator for Radiotherapy radiation, controls, electron, monitoring 405
 
  • V. A. Shishov, A. A. Budtov, M. F. Vorogushin
    NIIEFA, St. Petersburg
  A compact medical accelerator of new generation "ELLUS-6M" has been designed and manufactured for radiotherapy by 6MeV photons in the multi-static and arc modes. The gantry can be rotated through ±1850 and ensures setting accuracies of the irradiator rotation velocity and positioning sufficient for the IMRT mode. The computerized control system is compatible with the treatment planning system and allows upgrading by adding new modules. To realize the conformal radiotherapy, the following additional medical equipment has been developed: a multi-leaf collimator a portal vision system for the dose field verification during irradiation and an upgraded treatment table made as a semi-pantograph. In 2010, it is planned to finish clinical tests of the "ELLUS-6M" accelerator with the additional medical equipment in the N. N. Petrov Scientific Research Oncology Institute, Pesochny, St. Petersburg.  
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