2016
DOI: 10.1103/physrevlett.116.124801
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Physics of Phase Space Matching for Staging Plasma and Traditional Accelerator Components Using Longitudinally Tailored Plasma Profiles

Abstract: Phase space matching between two plasma-accelerator (PA) stages and between a PA and a traditional accelerator component is a critical issue for emittance preservation of beams accelerated by PAs. The drastic differences of the transverse focusing strengths as the beam propagates between different stages and components may lead to a catastrophic emittance growth in the presence of both finite energy spread and lack of proper matching. We propose using the linear focusing forces from nonlinear wakes in longitud… Show more

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Cited by 88 publications
(64 citation statements)
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“…1,2 Strong electric fields of the plasma wakefields guarantee the accelerating and focusing forces orders of magnitudes larger than the conventional accelerators. However, there remain several issues for the practical use of the plasma wakefield accelerators, such as difficulties of staging, 3 unstable propagation of drivers, 4 substantial energy spread, 5 and emittance growth of witness bunch, 6 to mention a few of them. For the successful injection of the witness bunch into the accelerating wakefield region of an ion cavity, its normalized transverse and longitudinal sizes are required to be much smaller than unity, k p r ( 1, where k p ¼ ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffi n 0 e 2 = 0 m e c 2 p is the plasma wave number.…”
Section: Introductionmentioning
confidence: 99%
“…1,2 Strong electric fields of the plasma wakefields guarantee the accelerating and focusing forces orders of magnitudes larger than the conventional accelerators. However, there remain several issues for the practical use of the plasma wakefield accelerators, such as difficulties of staging, 3 unstable propagation of drivers, 4 substantial energy spread, 5 and emittance growth of witness bunch, 6 to mention a few of them. For the successful injection of the witness bunch into the accelerating wakefield region of an ion cavity, its normalized transverse and longitudinal sizes are required to be much smaller than unity, k p r ( 1, where k p ¼ ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffi n 0 e 2 = 0 m e c 2 p is the plasma wave number.…”
Section: Introductionmentioning
confidence: 99%
“…Better control on the final direction can be achieved by fine tailoring of the ramp, as done in Ref. [26] for emittance conservation. As can be seen in Fig.…”
mentioning
confidence: 99%
“…Electron-bunch optimization shows that a small mean size and a small divergence is beneficial for both, the photon production, as well as the bandwidth of the Thomson source. LWFA-accelerated electron bunches are promoted with small emittances [92,107] and theoretical means have been published aiming at a divergence reduction and suppressed emittance growth at the transition from plasma to vacuum [108,109]. The photon production and bandwidth are determined by the mean electron bunch size, so that bunch focusing is not generally necessary.…”
Section: Interaction At the Plasma Exitmentioning
confidence: 99%