Paper | Title | Other Keywords | Page |
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TUXCH02 | New Developments in High Energy Electron Cooling | electron, high-voltage, laser, gun | 43 |
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Electron cooling of hadron beams is a powerful technique by which accelerator facilities achieve the necessary beam brightness for their physics research. An overview on the latest developments in high energy electron cooling (electron beam energy higher than 500 KeV) is given. Technical feasibility for electron beam energy up to 8 MeV is discussed. | |||
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Slides TUXCH02 [3.122 MB] | ||
WEXOR02 | New Developments and a Review of the Accelerator Facilities at iThemba LABS | proton, cyclotron, ion, controls | 98 |
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iThemba LABS is a multi-disciplinary research facility that provides accelerator-based facilities for physical, biomedical and material sciences, treatment of cancer patients with neutrons and protons and the production of radioisotopes and radiopharmaceuticals. The successful utilization of beam diagnostic equipment is critical and essential for the effective running of such a facility and will be discussed in more detail. The current status of the facility and future projects, which entail a radioactive-ion beam project as well as a dedicated facility for proton therapy, will also be discussed. | |||
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Slides WEXOR02 [6.188 MB] | ||
WEBOR01 | The C-80 Cyclotron System. Technical Characteristics, Current Status, Progress and Prospects. | cyclotron, proton, controls, power-supply | 106 |
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A C-80 cyclotron system is intended to produce proton beams with an energy ranging from 40 up to 80 MeV and current up to 200 mkA. The beams with these parameters will be used for commercial production of a wide spectrum of isotopes for medicine, proton radiation therapy of eye diseases and superficial oncologic diseases as well as for fundamental and applied researches. Manufacturing and installation of the cyclotron equipment and first section of the system for the beam transport to remote targets have been finished. Physical start-up of the cyclotron has been realized. In future, the C-80 cyclotron is supposed to be used as an injector of the C-230 synchrotron, which serves for additional acceleration of the extracted proton beam to energies of the order of 230 MeV. This will allow the Bragg's peak-based treatment procedures to be applied in the proton therapy of oncologic patients. | |||
FRXOR02 | Beam Diagnostic Instrumentation for the NSLS-II Booster | booster, vacuum, controls, radiation | 186 |
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For the NSLS-II synchrotron light source, a Booster synchrotron has been designed and produced by Budker Institute of Nuclear Physics. The Booster accelerates an electron beam from 200 MeV up to 3 GeV in both single-bunch and multi-bunch modes with repetition rate of 1 Hz. Accurate measurements of beam parameters are required during every work cycle to provide feed-forward tuning of the Booster. A set of beam diagnostic instruments has been developed for the Booster commissioning and operation. Six fluorescent screens are used for the first-turn beam observation. Electrostatic BPMs with signal processing electronics developed by BNL provide measurements of closed orbit and lattice functions as well as single-pass beam measurements for commissioning. A DC current transformer is used to measure average beam current and lifetime; the filling pattern is monitored by a fast current transformer. Two light-output ports are set up for observation of the beam image. Tune measurement system provides frequent measurements of betatron tunes during the energy ramp. Design and performance of the Booster beam instrumentation are presented; the commissioning plan is also discussed. | |||
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Slides FRXOR02 [5.121 MB] | ||
FRACH05 | Prospects for Introduction of Home-Made Equipment for Radionuclide Diagnostics | cyclotron, HOM, photon, positron | 197 |
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Radionuclide diagnostics that allows most diseases to be diagnosed at an early stage has recently been in the focus of attention. The current concept of radionuclide diagnostics advancement takes into account Russian geographic and demographic features and supports the application of the home-made equipment. As a basis, the concept assumes the establishment of regional diagnostic centers at hospitals in each Russian Federal district. In each such a center, a cyclotron of the CC-18/9 model, modules for radiopharmaceuticals' synthesis, single-photon emission (SPECT) and positron (PET) scanners should be installed. The yield of radiopharmaceuticals' production will satisfy the needs of such a center and of up to 30-35 SPECT-"satellites" located in diagnostic departments at hospitals situated up to 1000 km from the center. In future, on the basis of these diagnostic departments, autonomous PET-centers can be established, each equipped with СС-12 cyclotrons, modules for radiopharmaceuticals' synthesis and with 3-4 PET scanners. Implementation of the Federal Targeted Program on the serial production of cyclotrons and SPECT-scanners will allow the examination of population to be increased within 5-6 years up to 1.0-1.2 million people per year. | |||
FRBCH06 | Project of the Radioisotope Facility RIC-80 (Radioactive Isotopes at Cyclotrone C-80) in PNPI | target, cyclotron, ion, proton | 236 |
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It is well known presently that radionuclides produced with cyclotrons have very good nuclear-physical characteristics for use in medicine and a set of these nuclides is much wider than produced with the reactors. At PNPI a high current cyclotron C-80 with the energy of extracted proton beam of 40-80 MeV and the current up to 200 mkA is under construction. It is planned to start its operation at the end of 2012. One of the main goals of C-80 is production of a wide spectrum of medical radio- nuclides for diagnostics and therapy. At present time a project is worked out for the construction of radioisotope complex RIC-80 (Radio Isotopes at the cyclotron C-80) at the beam of C-80. In the presented submission the project of RIC-80 complex is discussed, which includes four target stations for the production of a wide set of radionuclides for medicine. The peculiarity of the proposed radioisotope facility is the use of the mass-separator with the target-ion source device as one of the target stations for on-line, or semi on-line production of a high purity separated radioisotopes. The possibility of production of different medical radionuclides, including relatively short-lived ones, is discussed as well. | |||
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Slides FRBCH06 [1.101 MB] | ||
WEPPC039 | Data Processing and Quantitation in Nuclear Medicine | ion, radiation, extraction | 526 |
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Accelerators of charged particles, radiation detectors are widely used in nuclear therapy and nuclear diagnostics. So there is necessity for diagnostic processing of data obtained using these devices. Nuclear diagnostics is based on analysis of radiation passing through the study object emitted from radiopharmaceuticals within the object or from external radiation source. First stage of data processing is presentation of detector signals in 2D or 3D image form. Further processing is based on mathematical modeling of processes within the investigated object. Mathematical modeling of static, dynamic and periodic processes is considered for quantitative analysis of studies in nephrology, osteology, endocrinology and cardiology. The data processing and quantitation software suite is presented. Clinical applications of the developed suite are discussed. Possibilities of software deployment in clinical centers are considered. | |||
WEPPD012 | Standing Wave RF Deflectors with Reduced Aberrations | impedance, emittance, cavity, controls | 590 |
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Funding: in part RBFR N 12-02-00654-a Deflecting structures are now widely used for bunch phase space manipulations either with bunch rotation for special bunch diagnostic or in emittance exchange experiments. Even if the field of synchronous harmonic is aberration free, the higher space harmonics provide non linear additives in the field distribution, leading to emittance growth during phase space manipulation. Standing wave operation is more RF efficient for short deflectors. The criterion of the field quality estimation and results is of deflecting structure consideration for minimization of non linear additives are presented. The solutions for dispersion correction together with end cells optimization are described too. |
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WEPPD040 | Precision Thermostatic Control for LUE-200 Accelerator Section | controls, linac, neutron, electron | 629 |
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According to the design of the IREN facility the system of thermostatting of LUE-200 linac sections is developed. Rated values of linac beam power depend basically on a microwave power input and stability of the phase. The latter is sustained by means of thermostatic control for the sections subject to the powerful microwave warming-up. Demanded both high accuracy of stabilization and low settling time of temperature for linac modes define development of the control system. The precise system of thermostatic control in which composition the programmable PID-controller and the platinum resistance thermometer with accuracy of 0.1%, and also thyristor regulators of heating power up to 15 kVА has been adapted for modes of the IREN microwave facility. The advanced system allows to control both power of heating and a flow of cooling water. The system supervises and changes over modes of the accelerated warming-up and controllable heating and cooling. Both high accuracy of the thermostat and energy saving at a smooth settling of temperature and at the subsequent long-term thermostabilization are substantially improved. Essential speed-up of a preliminary warming-up of the thermostat also is attained. | |||
WEPPD043 | Concept of the Software for ITEP-TWAC Control System | controls, synchrotron, proton | 638 |
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The work is in progress on the development of new control system for ITEP accelerators complex. All the software for the system should be developed from the very beginning. Core element of new software is PostgreSQL object-relational database management system. All interaction between the programms on device side and on operator side are made utilizing the database functionality. The database is also provides storage space for all configuration data, operational modes, logs and so on.Concept of the software for ITEP-TWAC control system. | |||
WEPPD047 | The Optimization of RF Deflector Input Power Coupler | coupling, emittance, electron, simulation | 650 |
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This paper concerns the investigation of different types of input power cell for S-band RF electron deflector. This device serving for slice emittance diagnostics is a disc-loaded waveguide which operates with TE11-like wave in traveling wave regime with 120 deg phase shift per cell. Since this deflector meets the restriction on its length and has to provide high enough deflecting potential to a particle during its flight time it is significant to increase the transversal field strength in coupling cell or to shorten it so that the deflecting potential remains constant. The total structure consists of 14 regular cells and two couplers. As it is now all cells have the same length equal to D=33.34 mm and the field in couplers is lower than that of regular cells. In this paper different length are considered and numerically simulated in order to choose the best one. | |||
WEPPD050 | Approximate Method for Calculation of Field of Charged Particle Moving through Dielectric Object | radiation, vacuum, simulation, plasma | 656 |
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Cherenkov radiation is widely used for particle detection. As well, it is prospective for particle bunch diagnostics. Therefore, it is actual to elaborate methods for calculation of the fields of bunches moving in the presence of different dielectric objects. We offer the approximate method based on calculation of the field in unbounded medium and accounting of boundary influence by geometrical optics. First, we consider the problem concerning the field of charge crossing a dielectric plate. This problem has an exact solution. It is used as a "test" problem for estimation of precision of the approximate method. Computation of the field is performed using both methods and the results have a good agreement. Further, we analyze the cases of more complex objects, in particular, a dielectric cone. Note, that the offered method allows to obtain wave fields using neither complex analytical transformations nor laborious numerical calculations. | |||