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Yoon, Eisung
Fusion and Plasma Application Research Laboratory (FPL)
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Witness electron beam injection using an active plasma lens for a proton beam-driven plasma wakefield accelerator

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dc.contributor.author Kim, S.-Y. ko
dc.contributor.author Moon, K. ko
dc.contributor.author Chung, Moses ko
dc.contributor.author Sjobak, K. N. ko
dc.contributor.author Adli, E. ko
dc.contributor.author Dayyani, M. ko
dc.contributor.author Doebert, S. ko
dc.contributor.author Yoon, Eisung ko
dc.contributor.author Nam, I. ko
dc.contributor.author Hahn, G. ko
dc.date.available 2021-12-16T07:59:10Z -
dc.date.created 2021-12-11 ko
dc.date.issued 2021-12 ko
dc.identifier.citation PHYSICAL REVIEW ACCELERATORS AND BEAMS, v.24, no.12, pp.121304 ko
dc.identifier.issn 2469-9888 ko
dc.identifier.uri https://scholarworks.unist.ac.kr/handle/201301/55120 -
dc.description.abstract An active plasma lens (APL) focuses the beam in both the horizontal and vertical planes simultaneously using a magnetic field generated by a discharge current through the plasma. A beam size of 5-10 mu m can be achieved within a short distance using a focusing gradient on the order of 100 T/m. The APL is therefore an attractive element for plasma wakefield acceleration, because an ultrasmall size of the witness electron beam is required for injection into the plasma wakefield to minimize emittance growth and to enhance the capturing efficiency. When the drive beam and witness electron beam copropagate through the APL, interactions between the drive and witness beams, and the plasma must be considered. In this paper, through particle-in-cell simulations, we discuss the possibility of using an APL for the final focusing of the electron beam for the AWAKE RUN 2 experiments. It is confirmed that the amplitude of the plasma wakefield excited by proton bunches remains the same even after propagation through the APL. The emittance of the witness electron beam increases rapidly in the plasma density ramp regions of the lens. Nevertheless, when the witness electron beam has a charge of 100 pC, emittance of 10 mm mrad, and bunch length of 60 mu m, its emittance growth is not significant along the active plasma lens. For small emittance, such as 2 mm mrad, the emittance growth is found to be strongly dependent on the rms beam size, plasma density, and multiple Coulomb scattering. ko
dc.language 영어 ko
dc.publisher AMER PHYSICAL SOC ko
dc.title Witness electron beam injection using an active plasma lens for a proton beam-driven plasma wakefield accelerator ko
dc.type ARTICLE ko
dc.identifier.scopusid 2-s2.0-85121629717 ko
dc.identifier.wosid 000731574100002 ko
dc.type.rims ART ko
dc.identifier.doi 10.1103/physrevaccelbeams.24.121304 ko
dc.identifier.url https://journals.aps.org/prab/abstract/10.1103/PhysRevAccelBeams.24.121304 ko
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