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dc.contributor.authorYıldız, Hatice Duran
dc.contributor.authorPorsuk, D.
dc.contributor.authorÇakır, Raşit
dc.contributor.authorTugay, H.
dc.date.accessioned2020-12-19T19:36:14Z
dc.date.available2020-12-19T19:36:14Z
dc.date.issued2019
dc.identifier.citationYıldız, H.D., Porsuk, D., Çakır, R. & Tugay, H. (2019). Design and comparison of superconducting rf gun cavities and beam dynamics for linear electron accelerators. Nuclear Instruments & Methods in Physics Research Section A-Accelerators Spectrometers Detectors and Associated Equipment, 939, 74-82. https://doi.org/10.1016/j.nima.2019.05.053en_US
dc.identifier.issn0168-9002
dc.identifier.issn1872-9576
dc.identifier.urihttps://doi.org/10.1016/j.nima.2019.05.053
dc.identifier.urihttps://hdl.handle.net/11436/1412
dc.descriptionCakir, Rasit/0000-0002-7104-9069en_US
dc.descriptionWOS: 000470966400011en_US
dc.description.abstractDesigns and simulations of 1.4, 1.5, 1.6, and 1.8-cell SRF gun cavities are studied at a linear accelerator gun system and they are compared with each other. We obtain high power beam from high energy electron beam produced at a photocathode with high quantum efficiency, high average current laser with high brightness, and high accelerating gradient. Beam energy of the whole accelerator system is effected mainly by the optimized RF power usage inside cells, the RF power interaction with particle beams, and the accelerated beam obtained by using SRF-gun cells. Thus, the optimized beam parameters, the RF parameters, and the accelerator gun cavity parameters that depend on each cavity geometries of SRF gun are obtained and presented in this paper. Additionally, the energy values of the electrons with optimized emittance at the gun exit are achieved and shown. We will conclude our paper by giving the gun output energies specifying which elliptical cavity-cell geometry is more appropriate to push the beam further in consistent conditions. For the cavity electromagnetic fields and the geometric designs of the cavities and the solenoid, we have utilized 2D Superfish/Poisson and 3D Computer Simulation Technology Programs. Also beam dynamics studies are included for only 1.6-cell SRF gun cavity which has the highest quality factor in order to figure out how the beam behaves along the beamline at the gun system. Transverse emittance (< 2 pi mm mrad) and beam energy (similar to 3.5 MeV) at the exit of the gun system are obtained as expected.en_US
dc.language.isoengen_US
dc.publisherElsevier Science Bven_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectLinear acceleratoren_US
dc.subjectSRF-gun cellen_US
dc.subjectElliptical cavity-cell geometryen_US
dc.subjectPhotocathodeen_US
dc.subjectQuantum efficiencyen_US
dc.subjectElectromagnetic fieldsen_US
dc.subjectBeam dynamicsen_US
dc.titleDesign and comparison of superconducting rf gun cavities and beam dynamics for linear electron acceleratorsen_US
dc.typearticleen_US
dc.contributor.departmentRTEÜ, Fen - Edebiyat Fakültesi, Fizik Bölümüen_US
dc.contributor.institutionauthorÇakır, Raşit
dc.identifier.doi10.1016/j.nima.2019.05.053
dc.identifier.volume939en_US
dc.identifier.startpage74en_US
dc.identifier.endpage82en_US
dc.relation.journalNuclear Instruments & Methods in Physics Research Section A-Accelerators Spectrometers Detectors and Associated Equipmenten_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US


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