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TUCOXBS03 | Beam Dynamics Layout of the MESA ERL | linac, experiment, operation, electron | 28 |
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Funding: This work has been supported by DFG through the PRISMA+ cluster of excellence EXC 2118/2019 and by the European Union’s Horizon 2020 Research and Innovation programme under Grant Agreement No 730871. The MESA project is currently under construction at Johannes Gutenberg-Universität Mainz. It will be used for high precision particle physics experiments in two different operation modes: external beam (EB) mode (0.15 mA; 155 MeV) and energy recovery (ERL) mode (1 mA; 105 MeV). The recirculating main linac follows the concept of a double sided accelerator design with vertical stacking of return arcs. Up to three recirculations are possible. Acceleration is done by four TESLA/XFEL 9-cell SRF cavities located in two modified ELBE cryomodules. Within this contribution the recirculation optics for MESA will be presented. Main goals are achieving best energy spread at the experimental setups in recirculating ERL and non-ERL operation and providing small beta-functions within the cryomodules for minimizing HOM excitation at high beam currents. |
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Slides TUCOXBS03 [5.077 MB] | |||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-ERL2019-TUCOXBS03 | ||
About • | paper received ※ 16 September 2019 paper accepted ※ 06 November 2019 issue date ※ 24 June 2020 | ||
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TUCOXBS05 | Beam Timing and Cavity Phasing | cavity, linac, target, injection | 39 |
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In a multi-pass Energy Recovery Linac (ERL), each cavity must regain all energy expended from beam acceleration during beam deceleration. The beam should also achieve specific energy targets during each loop that returns it to the linac. To satisfy the energy recovery and loop requirements, one must specify the phase and voltage of cavity fields, and one must control the beam flight times through the return loops. Adequate values for these parameters can be found by using a full scale numerical optimization program. If symmetry is imposed in beam time and energy during acceleration and deceleration, the number of parameters needed decreases, simplifying the optimization. As an example, symmetric models of the Cornell BNL ERL Test Accelerator (CBETA) are considered. Energy recovery results from recent CBETA single-turn tests are presented, as well as multi-turn solutions that satisfy CBETA optimization targets of loop energy and zero cavity loading. | |||
Slides TUCOXBS05 [5.186 MB] | |||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-ERL2019-TUCOXBS05 | ||
About • | paper received ※ 13 September 2019 paper accepted ※ 01 November 2019 issue date ※ 24 June 2020 | ||
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WEPNEC14 | Electromagnetic Design of a Superconducting dual axis Spoke Cavity* | cavity, linac, SRF, radiation | 94 |
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Funding: The reported study was funded by RFBR according to the research project 18-302-00990 Dual axis superconducting spoke cavity for Energy Recovery Linac application is proposed. Conceptual design of the cavity is shown and preliminary optimiza-tions of the proposed structure have been carried out to minimize the ratio of the peak magnetic and electric fields to the accelerating voltage. The new design and future work are discussed |
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DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-ERL2019-WEPNEC14 | ||
About • | paper received ※ 01 October 2019 paper accepted ※ 06 November 2019 issue date ※ 24 June 2020 | ||
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FRCOXBS03 | Beam Dynamics Simulations for the Twofold ERL Mode at the S-DALINAC* | linac, electron, GUI, cavity | 155 |
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Funding: *Work supported by DFG through GRK 2128 and BMBF through grant No. 05H18RDRB2 The recirculating superconducting electron accelerator S-DALINAC [1] at TU Darmstadt is capable to run as a onefold or twofold Energy Recovery Linac (ERL) with a maximum energy of approximately 34 or 68 MeV in ERL mode, respectively. Since the maximum kinetic energy for the twofold ERL mode at injection is less than 8 MeV (v/c<0.9982) and since several multi-cell cavities designed for v/c=1 are used in the main accelerator, the electrons suffer from the effect of phase slippage. Therefore, beam dynamics simulations for the 6D phase space were performed in order to provide a sufficient beam guiding. [1] N. Pietralla, Nuclear Physics News, Vol. 28, No. 2, 4 (2018). |
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DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-ERL2019-FRCOXBS03 | ||
About • | paper received ※ 17 October 2019 paper accepted ※ 01 November 2019 issue date ※ 24 June 2020 | ||
Export • | reference for this paper using ※ BibTeX, ※ LaTeX, ※ Text/Word, ※ RIS, ※ EndNote (xml) | ||