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Corkscrew modes in linear accelelators

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TLDR
In this paper, the authors investigated the corkscrew mode in linear accelerators, in which a solenoidal beam-transport system is used, both analytically and numerically.
Abstract
The corkscrew mode in linear accelerators, in which a solenoidal beam-transport system is used, is investigated both analytically and numerically. By assuming that both the acceleration gaps and the drift regions between the adjacent magnets are infinitesimal, it is possible to treat the corkscrew mode analytically and to obtain an expression for the corkscrew mode amplitude and the effective emittance growth as a function of the energy variation within the beam pulse and of the tilts of the injector and the solenoid magnets. Reduction of the corkscrew mode amplitude is possible by an energy compensation scheme. This energy compensation scheme is studied numerically for the Experimental Test Accelerator II (ETA-II) configuration. We find that applying the energy compensation scheme at the beginning of the accelerator can reduce the corkscrew mode amplitude by a factor of two.

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Citations
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Journal ArticleDOI

Beam dynamics of the Neutralized Drift Compression Experiment-II, a novel pulse-compressing ion accelerator

TL;DR: The Neutralized Drift Compression Experiment (NDCXII) at the Lawrence Berkeley National Laboratory (LBNL) as mentioned in this paper is a state-of-the-art NDCX-II particle accelerator with an initial nonneutralized compression that renders the pulse short enough that existing high-voltage pulsed power can be employed.
Journal ArticleDOI

The NDCX-II engineering design

TL;DR: The Neutralized Drift Compression Experiment (NDCX-II) is a user facility located at Lawrence Berkeley National Laboratory which is uniquely designed for ion-beam-driven high energy density laboratory physics and heavy ion fusion research as discussed by the authors.
Journal ArticleDOI

Control of transverse motion caused by chromatic aberration and misalignments in linear accelerators

TL;DR: In this paper, a time-independent steering algorithm is proposed to minimize the observed corkscrew-amplitude averaged over the beam pulse, which is not sensitive to the alignment, calibration and spacing of the beam position monitors.
Journal ArticleDOI

Prototype microwave source for a relativistic klystron two-beam accelerator

TL;DR: In this paper, a test facility is established at Lawrence Berkeley National Laboratory (LBNL) to study RF power sources for linear colliders based on the relativistic klystron two-beam accelerator (RK-TBA) concept.
References
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Beam dynamics in the advanced test accelerator (ata)

TL;DR: In this paper, the performance of the Advanced Test Accelerator, a 50 MeV, 10 KA induction linac, is reviewed and a discussion of the operation of the plasma cathode electron source, beam transport throughout the accelerator, and transverse instabilities.
Journal ArticleDOI

Beam Breakup (BBU) Instability Experiments on the Experimental Test Accelerator (ETA) and Predictions for the Advanced Test Accelerator (ATA)

TL;DR: In linear accelerators, the maximum achievable beam current is often limited by the Beam Breakup (BBU) instability, which arises from the interaction of a transversely displaced beam with the dipole modes of the acceleration cavities as discussed by the authors.
Proceedings ArticleDOI

The ETA-II Induction Linac as a High-Average-Power FEL Driver

TL;DR: The Experimental Test Accelerator II (ETA-II) as discussed by the authors is the first induction linac designed specifically to FEL requirements and is used to drive a 140 and 250 GHz microwave FEL for plasma heating experiments at LLNL.

Engineering aspects and initial performance of ETA-II

TL;DR: The Experimental Test Accelerator-II (ETA-II) as mentioned in this paper is a high-average-power induction accelerator constructed at the Lawrence Livermore National Laboratory (LLNL) in the US.
Journal ArticleDOI

Transverse misalignments in a driver

TL;DR: The transverse errors of the beam lines are usually corrected by an appropriate feedback to bring the beam back on axis In an induction linac, however, in this article the beam line errors are not corrected.
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