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Short-pulse dielectric two-beam acceleration

Published online by Cambridge University Press:  16 February 2012

W. GAI
Affiliation:
ANL, Argonne, IL 60439, USA ([email protected])
J. G. POWER
Affiliation:
ANL, Argonne, IL 60439, USA ([email protected])
C. JING
Affiliation:
Euclid Techlabs, LLC, Solon, OH 44139, USA

Abstract

We are exploring a new parameter space of the two-beam acceleration (TBA) scheme based on an ultra-short (~20 ns) rf pulse in a dielectric TBA. All two-beam accelerators (TBAs) use an electron drive beam to generate high-power rf in a decelerator and extract this power to drive an accelerating structure to high gradient. Typically, the rf pulse is on the order of hundreds of ns or greater in order to maintain good rf-to-beam efficiency. However, recent scaling arguments show that the rf breakdown threshold improves with decreasing rf pulse length, so it desirable to find a way to run at short-pulse length with good efficiency. In this paper, we discuss how we chose the design parameters of a short-pulse TBA for a TeV linear collider module. We then present plans for an experimental program to demonstrate TBA at Argonne wakefield accelerator (AWA) facility including high-power rf generation, high-gradient acceleration, and staging.

Type
Papers
Creative Commons
This is a work of the U.S. Government and is not subject to copyright protection in the United States.
Copyright
Copyright © Cambridge University Press 2012. This is a work of the U.S. Government and is not subject to copyright protection in the United States.

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References

[3]Blumenfeld, I., et al. Feb. 2007 Nature 445, 741744.CrossRefGoogle Scholar
[4]Leemans, W. P., et al. 2006 Nature Phy., 696699.Google Scholar
[5]Thompson, M. C., et al. 2008 Phy. Rev. Lett. 100, 214801.Google Scholar
[6]Dolgashev, V. 2010 In: Proc. Advanced Accelerator Concepts: 14th Workshop, vol. 1299 (ed. Gold, S. and Nusinovich, G.). Annapolis, MD: AIP, pp. 274279.Google Scholar
[7]Wang, F. et al. 2010 In: Proc. Advanced Accelerator Concepts: 14th Workshop, vol. 1299 (ed. Gold, S. and Nusinovich, G.). Annapolis, MD: AIP, pp. 280285.Google Scholar
[8]Jing, C., et al. 2011 In: Proc. PAC11, NYC. Piscataway, NJ: IEEE, pp. 22792281.Google Scholar
[9] WF-Note-239, unpublished, http://www.hep.anl.gov/awaGoogle Scholar
[11]Jing, C., et al. 2010 In: Proc. IPAC10. Kyoto, Japan: ICR, pp. 44344436.Google Scholar
[12]Gai, W. and Jing, C. 2006 The dielectric-loaded accelerating structures. In: Periodic Structures: ISBN: 81-308-0032-2 (ed. Bozzi, M. and Perregrini, L.).Google Scholar
[13]Chojnacki, E. et al. 1991 J. Appl. Phys. 69, 6257.CrossRefGoogle Scholar
[14]Gao, F. et al. 2008 Phys. Rev. S.T. Accel. Beams 11, 041301.Google Scholar
[15]Power, J. G. et al. Staging in dielectric two beam wakefield accelerators. IPAC'11; http://www.JACoW.org.Google Scholar
[16]Conde, M. et al. 2011 Upgrade of the Argonne wakefield accelerator facility (AWA) and commissioning of a new RF gun for drive beam generation. In: Proc. PAC'11, NYC, http://www.JACoW.org.Google Scholar
[17]Naito, T. et al. 2011 Phys. Rev. ST Accel. Beams 14, 051002.Google Scholar
[18]Browman, M. J. 2011 Using the Panofsky–Wenzel theorem in the analysis of radio-frequency deflectors. In: PAC'93, Washington DC, http://www.JACoW.org.Google Scholar
[19]Wangler, T. 1998 RF Linear Accelerators. New York: Wiley.Google Scholar
[20]Shi, J. et al. 2009 Nucl. Instr. and Meth. A 598, pp. 388393.Google Scholar
[21]Power, J. G. Estimate of the RF power required by the deflecting mode cavity. Internal Note.Google Scholar