| Paper | Title | Page |
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| TUOCB1 | Progress in the Design of Beam Optics for FCC-ee Collider Ring* | 1281 |
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| The beam optics for the FCC-ee collider has been updated: (a) the layout is adjusted to a new footprint of FCC-hh, (b) the design around the interaction point is refined considering a number of machine-detecor interface issues, (c) the arc lattice is refined taking realistic magnet designs into account, (d) the β* and betatron tunes are re-optimized according to recent results of the beam-beam simulations, and more. These changes make the collider design more realistic without performance degradation. | ||
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Slides TUOCB1 [4.891 MB] | |
| DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2017-TUOCB1 | |
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TUOCB2 |
JLEIC Ultimate Luminosity With Strong Electron Cooling | |
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Funding: Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177 and DE-AC02-06CH11357. The design strategy of an electron-ion collider for reaching high luminosities is presently based on application of strong cooling of the ion beams during collisions. In this paper, we present the main design parameters for JLEIC, a Jefferson Lab proposal of an electron-ion collider, to reach ultimate high luminosity up to 2x1034 /cm2/s. |
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Slides TUOCB2 [4.129 MB] | |
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| TUOCB3 | CBETA - Cornell University Brookhaven National Laboratory Electron Energy Recovery Test Accelerator | 1285 |
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Funding: New York State Energy Research and Development Authority (NYSERDA) Cornell's Lab of Accelerator-based Sciences and Education (CLASSE) and the Collider Accelerator Department (BNL-CAD) are developing the first SRF multi-turn energy recovery linac with Non-Scaling Fixed Field Alternating Gradient (NS-FFAG) racetrack. The existing injector and superconducting linac at Cornell University are installed together with a single NS-FFAG arcs and straight section at the opposite side of the the linac to form an Electron Energy Recovery (ERL) system. Electron beam from the 6 MeV injector is injected into the 36 MeV superconducting linac, and accelerated by four successive passes: from 42 MeV up to 150 MeV using the same NS-FFAG structure made of permanent magnets. After the maximum energy of 150 MeV is reached, the electron beam is brought back to the linac with opposite Radio Frequency (RF) phase. Energy is recovered and reduced to the initial value of 6 MeV with 4 additional passes. There are many novelties: a single NS-FFAG structure, made of permanent magnets, brings electrons with four different energies back to the linac. A new adiabatic NS-FFAG arc-to-straight section merges 4 separated orbits into a single orbit in the straight section. |
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Slides TUOCB3 [41.888 MB] | |
| DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2017-TUOCB3 | |
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