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TUCBMH01 | Status of the Kurchatov Synchrotron Light Source | controls, wiggler, electron, vacuum | 27 |
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The Kurchatov synchrotron light source operates in the range of synchrotron radiation from VUV up to hard X-ray. To improve facility capabilities in the last few years technical modernization of all facility systems is underway and new beam lines are constructed. In this report the present status and future plans of the Kurchatov synchrotron light source is presented. | |||
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Slides TUCBMH01 [10.384 MB] | ||
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TUCBMH02 | Numerical Analysis of the Effective Width of the Spectrum of Synchrotron Radiation | radiation, polarization, synchrotron-radiation, electron | 30 |
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A notation of an effective spectral width is introduced in the theory of synchrotron radiation, as an exact quantitative characteristic of the spectral properties. Within a classical theory, numerical calculations of the effective spectral width for polarization components of the synchrotron radiation have been carried out (for an effective width exceeding 100 harmonics). It is found how the effective spectral width and the initial harmonic change depending on the energy of the radiating particle. | |||
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Slides TUCBMH02 [0.265 MB] | ||
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THCDMH03 | The Progress on Manufacturing and Testing of the SC Magnets for the NICA Booster Synchrotron | booster, dipole, superconducting-magnet, collider | 144 |
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NICA is a new accelerator collider complex under construction at the Joint Institute for Nuclear Research in Dubna. The facility is aimed at providing collider experiments with heavy ions up to Gold in the center of mass energy from 4 to 11 GeV/u and an average luminosity up to 1*1027 cm-2 s−1 for Au79+. The collisions of polarized deuterons are also foreseen. The facility includes two injector chains, a new superconducting booster synchrotron, the existing 6 AGeV superconducting synchrotron Nuclotron, and a new superconducting collider consisting of two rings, each 503 m in circumference. The booster synchrotron is based on an iron-dominated "window frame"- type magnet with a hollow superconductor winding analogous to the Nuclotron magnet. The design of superconducting magnets for the NICA booster synchrotron is described. The progress of work on the manufacturing and testing of the magnets is discussed. The calculated and measured values of the characteristics of the magnets are presented. The status of the facility for serial test of superconducting magnets for the NICA and FAIR projects is described. | |||
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Slides THCDMH03 [8.068 MB] | ||
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TUPSA024 | On Stabilization of Systems of Linear Equations with Linear Increasing Time Delay by Observation | controls, feedback, acceleration, damping | 261 |
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Differential-difference equations with time delay are often used in mathematical models describing the dynamics of beams of the charged particles. For example linear equation of the second order with a constant time delay describes in the smoothed approach dynamics of a beam of the charged particles in synchrotrons with a feedback system. However the time delay cannot always be considered constant. The time proportional delay can occur at acceleration of beams of the charged particles in the cyclotron. It should be noted that such time delay is unbounded and well known approaches are not applicable for stability analysis such systems. The stabilizing control for the system of linear equations could be constructed by the information on a state vector of the system. Sometimes the state vector is unknown but we know some linear combinations of its components. Then there is a problem on construction of the stabilizing control with incomplete information. In this paper we investigate a possibility of stabilization of system of linear equations with time proportional delay by the linear observation. Using the sufficient conditions of asymptotic stability of system of linear equations with linear increasing delay we obtain some conditions of existence of the asymptotic evaluation system of the original system. Then we use the asymptotic evaluation system for the construction of the stabilizing control and derive the sufficient conditions for the existence of such control. | |||
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TUPSA063 | The Electron Trajectories Construction in the System With a "Real" Geometry of the Field Cathode | electron, cathode, controls, neutron | 339 |
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The problems of the trajectories constructing for field electrons and emission images simulation are considered. As an approximation of the emitter shape an explicitly and implicitly defined surfaces are selected. Hyperboloidal, ellipsoidal and paraboloidal models are studied. Also an equipotential surface of the charged sphere-on-orthogonal-cone system is used. A simple solution of the field distribution problem is allowed to formulate the Cauchy problem for the motion equations. The shape of the anode (the projector microscope screen) can be selected in any desired form. Achieving a screen by electrons is performed with dense output technique in numerical approach to the solution. The distribution of the work function on the cathode surface is obtained. The trajectories for the projection of the field emission activity as the image are used. | |||
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WEPSB014 | Symmetrical Parameterization for 6D Fully Coupled One-Turn Transport Matrix | coupling, emittance, lattice, operation | 389 |
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Symmetry properties of 6D and 4D one-turn symplectic transport matrices were studied. A new parameterization was proposed for 6D matrix, which is an extension of the Lebedev-Bogacz parameterization for 4D case. The parameterization is fully symmetric relative to radial, vertical and longitudinal motion. It can be useful for lattices with strong coupling between all degrees of freedom. | |||
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Poster WEPSB014 [0.908 MB] | ||
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WEPSB016 | Coupled Bunch Instabilities in the Storage Rings | impedance, wakefield, storage-ring, electron | 395 |
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Funding: The reported study was funded by RFBR according to the research project No. 16-32-00335 mola. Coherent instabilities of the bunched beam are one of the reasons that limit a total beam current in the storage rings. Although there are solutions of this problem, the estimation and reduction of wake-fields influence on the longitudinal beam dynamics remain important things. In the article we return to the subject of coherent instabilities of the unevenly-filled bunches in the storage rings. |
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WEPSB020 | On a New Approach for Description of Self-Consistent Distributions for a Charged Particle Beam | distributed, operation, electron, linac | 407 |
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The present report is concerned with the problem of particle phase space distributions for a charged particle beam. A new approach is presented. It provides the possibility to specify various coordinates in the phase space. The main attention has been focused on the case where motion integrals are taken as phase coordinates. Using such coordinates, one can obtain a lot of self-consistent distributions. Some distributions for a breathing beam are considered as examples: generalized Brillouin flow, generalized KV distribution, and others. Besides, this approach allows simple graphical representation of various self-consistent distributions. | |||
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THPSC017 | A Synchrotron Radiation Beamline Installed at BINP to Study the High Luminosity LHC Vacuum System | photon, electron, vacuum, radiation | 572 |
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In the framework of the HL-LHC project, the vacuum performance of new surface material needs to be studied. In particular, a-C coating is proposed as an anti-multipactor surface in the HL-LHC Inner Triplets. Since the protons in the HL-LHC Inner Triplets will generate synchrotron radiation (SR) with ~ 10 eV critical energy and ~ 1016 ph/m/s flux, it is therefore of great importance to study the impact of such photons on a-C coating held at room and cryogenic temperature and compare the results against present LHC material. This paper describes construction and parameters of experimental set-up based on new Synchrotron Radiation beamline from booster synchrotron BEP at BINP. The experimental program releasing in collaboration between CERN and BINP for performing measurements of photon stimulated gas desorption, photon distribution and photo-electron emission provoked by synchrotron radiation are presented | |||
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THPSC026 | The Automation of Energy Ramping for the Main Storage Ring of KSRS | controls, power-supply, radiation, synchrotron-radiation | 597 |
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Kurchatov Synchrotron Radiation Source (KSRS) is the complex of electron synchrotrons specialized as a source of synchrotron radiation. The running cycle of KSRS main storage ring includes the energy ramping from 450 MeV up to 2.5 GeV. Fast and reliable energy ramping algorithm was developed and implemented at KSRS main storage ring. Using the hardware decisions on the basis of the NI units and CAN-bus interface, the control system is developed and launched for the power supplies of magnetic elements. | |||
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THPSC052 | The Longitudinal Broadband Impedance and Energy Spread Measurements at VEPP-4M | impedance, damping, scattering, electron | 650 |
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The paper presents studies of the longitudinal broadband impedance of VEPP-4M and measurements of its bunch energy spread at different energies in range of 1.45 - 3.5 GeV. In order to measure the longitudinal bunch size at different currents we used PS-1/S1 streak camera with picosecond temporal resolution. Considering that influence of collective effects is negligible at low currents we determined bunch energy spread from its length at low currents. Collected bunch length data demonstrate microwave instability thresholds and potential well distortion lengthening. Potential well distortion was studied at 3 GeV and 3.5 GeV. Measured potential well distortion lengthening was used to estimate a value of the reactive part of the longitudinal impedance. Observed microwave instability thresholds was used to measure the value of broadband impedance. Measured value of the VEPP-4M is 7.9 ± 1.5 Ohm. | |||
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THPSC054 | Modernization of the Electron Beam Stabilization System in the KSRS | database, controls, radiation, synchrotron-radiation | 656 |
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The stabilization system is designed to prevent drift of the spot SR at the experimental stations by local changes of the orbit. This system was developed and implemented about twelve years ago as an element of the ACS and worked well. Produced by modernization has led to the need of adaptation of the system of stabilization not only in hardware but also in software. Work on updating of the stabilization system and will be shown next. | |||
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THPSC063 | System of Thermomonitoring and Thermostabilizing of Kurchatov Synchrotron Radiation Source | controls, radiation, synchrotron-radiation, electron | 680 |
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The modern system of thermomonitoring and thermostabilizing (TERMOCS) of KSRS - Kurchatov synchrotron radiation source is described. The TERMOCS system provides: a monitoring of temperatures of the magnets and RF-resonators of KSRS; informing operator on violations of the course of technological process; data protection from illegal access; an archiving and displaying of archive data in a trend type. The system includes 480 temperature sensors of the AD592 type, providing the accuracy of measurements 0,2 C. System of thermo stabilizing of the linear accelerator - the proportional integral differentiating regulator for support of stability of temperatures at the level of 0,05 C. During creation of the system the modern decisions on the basis of the modular complexes of NI, the modern servers and the Citect SCADA software system were used. | |||
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THPSC084 | The New Control for Magnet System of KSRS | controls, electron, software, radiation | 727 |
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The running cycle of Kurchatov Synchrotron Radiation Source (KSRS) includes the injection of electrons with energy 80 MeV from the linear accelerator in the booster storage ring Siberia-1, the accumulation of a electron current up to 400 mA and, then, electron energy ramping up to 450 MeV with the subsequent extraction of electrons in the main ring, storage ring Siberia-2, and accumulation there up to 300 mA, and at last the energy ramping up to 2.5 GeV. Several years ago, a modernization of the current system of automated control systems (ACS) has started. This article presents one of the most important parts - the new control subsystem of the magnet system | |||
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