Paper | Title | Page |
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FRCAMH01 | Status of the Nuclotron | 150 |
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Since last RuPAC two runs of the Nuclotron operation were performed: in January - March of 2015 and June 2016. Presently we are providing the run, which has been started at the end of October and will be continued up to the end of December. The facility development is aimed to the performance increase for current physical program realization and preparation to the NICA Booster construction and Baryonic Matter at Nuclotron experiment. | ||
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Slides FRCAMH01 [20.777 MB] | |
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FRCAMH02 | Commissioning of New Light Ion RFQ Linac and First Nuclotron Run with New Injector | 153 |
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The new accelerator complex Nuclotron-based Ion Collider fAcility (NICA) is now under development and construction at JINR, Dubna. This complex is assumed to operate using two injectors: the Alvarez-type linac LU-20 as injector of light ions, polarized protons and deuterons and a new linac HILAc - injector of heavy ions beams. Old HV for-injector of the LU-20, which operated from 1974, is replaced by the new RFQ accelerator, which was commissioned in spring 2016. The first Nuclotron technological run with new fore-injector was performed in June 2016. Beams of D+ and H2+ were successfully injected and accelerated in the Nuclotron ring. Main results of the RFQ commissioning and the first Nuclotron run with new for-injector is discussed in this paper. | ||
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Slides FRCAMH02 [30.140 MB] | |
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FRCAMH03 | Commissioning of the New Heavy Ion Linac at the NICA Project | 156 |
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The new accelerator complex Nuclotron-based Ion Collider fAcility (NICA) is now under development and construction at JINR, Dubna. This complex is assumed to operate using two injectors: modernized old Alvarez-type linac LU-20 as injector of light polarized ions and a new Heavy Ion Linear Accelerator HILAc - injector of heavy ions beams. The new heavy ion linac accelerate ions with q/A values above 0.16 to 3.2 MeV/u is under commissioning. The main components are 4-Rod-RFQ and two IH - drift tube cavities is operated at 100.6 MHz. Main results of the HILAc commissioning with carbon beam from the laser ion source are discussed. | ||
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Slides FRCAMH03 [14.452 MB] | |
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TUPSA002 |
First Results of Startup of The Second Accelerating Section of The LUE-200 Linac | |
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It announces the startup of the second accelerating section of the LUE-200 electron linac of the pulsed resonance neutrons source (IREN)of the Laboratory of Neutron Physics. The block diagram, klystron and modulator parameters are presented. As a result of optimization of the accelerating system and focusing system the electron beam implemented to target. The basic parameters of the beam are measured: beam current, energy, and the energy spectrum of the beam. | ||
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TUPSA003 |
The Status of Works on the Linear Accelerator Electrons Accelerating Stand of JINR | |
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Work is continuing on a linear accelerator electrons accelerating stand JINR. Physical start of the second accelerator station was performed. Work is underway to harness the electron beam through the third and fourth station accelerator. The electron beam accelerator after the first station is used to test crystals and for radiation tests | ||
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TUPSA019 | Upgrade of the RF System on the LUE-200 | 256 |
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In the report works on upgrade of RF system of the LUE-200 (IREN) electron linac are provided. The main attention is paid to system of preliminary excitement of klystrons. After work on installation of the second accelerating section RF system of Installation it was considerably remade that allowed to carry out start-up of the second stage of the IREN installation successfully. Methods, features and problems in case of a training of two accelerating sections are discussed. Influence of the temperature and frequency modes on joint operation of accelerating sections. Results of setup of the RF system and a training of sections, and also results of posting of a bunch are given. | ||
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THPSC082 |
Control System of LUE-200 of IREN Facility - Status | |
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The control system of LUE-200 an intensive pulse source of resonant neutrons (IREN) is described. The architecture of a control system and equipment structure is shown. Control system construction bases on the maximum use of instrumentation and the software for industrial systems. The control system solves following problems: set and t control of parameters of the basic systems of the accelerator (modulators, the RF-systems, focusing elements, the synchronizer, vacuum system etc.) with display of these parameters; beam diagnostics (a beam current, a profile and a beam position, energy etc.); protection of elements of the accelerator at an exit of their parameters from a working range; creation of a database of operating regimes of the accelerator; monitoring radiation level and the organization of lockup. | ||
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