002899611 001__ 2899611
002899611 003__ SzGeCERN
002899611 005__ 20240604232641.0
002899611 0247_ $$2DOI$$9IOP$$a10.1088/1742-6596/2687/2/022010
002899611 0247_ $$2DOI$$9JACOW$$a10.18429/JACoW-IPAC2023-MOPL094
002899611 0248_ $$aoai:cds.cern.ch:2899611$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
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002899611 035__ $$9https://inspirehep.net/api/oai2d$$aoai:inspirehep.net:2717634$$d2024-06-03T08:47:16Z$$h2024-06-04T04:10:44Z$$mmarcxml
002899611 035__ $$9Inspire$$a2717634
002899611 041__ $$aeng
002899611 100__ $$aAlharthi, [email protected]$$uIJCLab, Orsay$$uKACST, Riyadh$$vKACST, Riyadh, Saudi Arabia.
002899611 245__ $$9IOP$$aBenchmarking the FCC-ee positron source simulation tools using the SuperKEKB results
002899611 246__ $$9JACOW$$aBenchmarking the FCC-ee positron source simulation tools using the SuperKEKB results
002899611 260__ $$c2024
002899611 260__ $$c2023
002899611 300__ $$a7 p
002899611 520__ $$9IOP$$aFor the Future Circular Collider (FCC-ee), particular attention is drawn to the crucial role of the positron source. Two positron production schemes are considered for the FCC-ee: the conventional scheme and the crystal-based (hybrid) scheme that involves channelling radiation in the oriented crystals. A start-to-end simulation toolkit should be developed to design and optimize positron production and capture by considering the positron injector parameters, including the electron drive beam and final system acceptance. This paper presents the first results of benchmarking the FCC-ee positron source simulation tools using the SuperKEKB positron source currently in operation. The model starts with the production of positrons and target studies in Geant4. Then, the RF-Track code is used to capture and track the generated positrons through the capture section composed of a matching device and several accelerating structures embedded in the solenoid field to accelerate the positrons up to 120 MeV. After that, the positrons are further accelerated up to the energy of the Damping Ring (1.1 GeV). Finally, the SuperKEKB capture system is applied to the FCC-ee positron injector within the framework of the design studies.
002899611 520__ $$9JACOW$$aFor the Future Circular Collider (FCC-ee), particular attention is drowned to the crucial role of the positron source. Two positron production schemes are considered for the FCC-ee: conventional and crystal-based (hybrid), implying the use of channeling radiation in the oriented crystals. To design and optimize the positron production and capture by considering the positron injector parameters, including the electron drive beam and the final system acceptance, a start-to-end simulation toolkit should be developed. This paper will present the first results of benchmarking the FCC-ee positron source simulation tools using the SuperKEKB positron source currently in operation. The model starts with the production of positrons and target studies in Geant4. Then, a new tracking code RF-Track is used for capturing and tracking the generated positrons through the capture section composed of the matching device and several accelerating structures embedded in the solenoid field to accelerate the positrons until ~120 MeV. Afterward, the positrons are further accelerated to the energy of the Damping Ring (1.1 GeV).
002899611 540__ $$3publication$$aCC-BY-3.0$$bIOP$$uhttp://creativecommons.org/licenses/by/3.0/
002899611 540__ $$3publication$$aCC-BY-4.0$$bJACOW$$uhttps://creativecommons.org/licenses/by/4.0
002899611 65017 $$2SzGeCERN$$aAccelerators and Storage Rings
002899611 6531_ $$9author$$apositron
002899611 6531_ $$9author$$asimulation
002899611 6531_ $$9author$$atarget
002899611 6531_ $$9author$$aelectron
002899611 6531_ $$9author$$aelectronics
002899611 6531_ $$9author$$alinac
002899611 690C_ $$aARTICLE
002899611 690C_ $$aCERN
002899611 700__ $$aChaikovska, I$$uIJCLab, Orsay
002899611 700__ $$aChehab, R$$uIJCLab, Orsay
002899611 700__ $$aZhao, Y$$uCERN
002899611 700__ $$aLatina, A$$uCERN
002899611 700__ $$aEnomoto, Y$$uKEK, Tsukuba
002899611 700__ $$aMiyahara, F$$uKEK, Tsukuba
002899611 700__ $$aMytrochenko, V$$uKharkov, KIPT
002899611 773__ $$c022010$$n2$$pJ. Phys. : Conf. Ser.$$v2687$$y2024
002899611 773__ $$cMOPL094$$pJACoW IPAC$$qIPAC2023$$v2023$$wC23-05-07$$y2023
002899611 8564_ $$82534624$$s268497$$uhttps://cds.cern.ch/record/2899611/files/PublicationJACoW.pdf$$yFulltext
002899611 8564_ $$82534625$$s474242$$uhttps://cds.cern.ch/record/2899611/files/PublicationIOP.pdf$$yFulltext
002899611 960__ $$a13
002899611 962__ $$b2858945$$k022010$$nvenice20230507
002899611 980__ $$aARTICLE
002899611 980__ $$aConferencePaper