نتایج جستجو برای: accelerator cavity

تعداد نتایج: 95148  

1999
C. Ohmori E. Ezura M. Fujieda Y. Mori R. Muramatsu H. Nakayama Y. Sato A. Takagi M. Toda T. Uesugi M. Yamamoto

Very high field-gradient has become available by a new Magnetic Alloy (MA)-loaded cavity developed for high intensity proton synchrotrons. The available RF voltage per core is ten times larger than that of the ordinary ferrite core. The maximum voltage of 20 kV has been achieved by the High-Field Gradient Cavity(HGC) of 40 cm in length[1]. Because the intrinsic Q-value of the MA core is low, ac...

2007
C. Rivetta T. Mastorides J. D. Fox D. Teytelman D. Van Winkle

A time domain modeling and simulation tool for beam-cavity interactions in LER and HER rings at PEP II are presented. The motivation for this tool is to explore the stability margins and performance limits of PEP II RF systems at higher currents and upgraded RF configurations. It also serves as test bed for new control algorithms and can define the ultimate limits of the architecture. The time ...

Journal: :Journal of physics 2022

Abstract The SSRF Phase-II Beamline Project started November 20, 2016 with a 6-year construction period. This project is mainly to construct 18 new beamlines and more than 30 end-stations, as well the corresponding storage ring upgrades, user auxiliary laboratories, beamline technology support infrastructures. Till now, 11 have passed technical acceptance test been in running. remaining seven w...

1995
S. Belomestnykh G. Flynn W. Hartung J. Kirchgessner D. Moffat H. Muller H. Padamsee

Plans for the next generation of electron-positron colliders (B-factories and B-factory-like machines) call for high beam currents to produce luminosities of the order of 1033. To store these high currents in a machine, special attention must be paid to the interaction of the beam with discontinuities in the surrounding vacuum chamber. RF cavities are among the biggest perturbations in accelera...

1998
J. Sekutowicz M. Ferrario C. Tang

We discuss the new layout of a cavity chain (superstructure) allowing, we hope, significant cost reduction of the RF system of both linacs of the TESLA linear collider. The proposed scheme increases the fill factor and thus makes an effective gradient of an accelerator higher. We present mainly computations we have performed up to now and which encouraged us to order the copper model of the sch...

2008
A. Candel A. Kabel L. Lee Z. Li C. Limborg C. Ng G. Schussman K. Ko

SLAC’s Advanced Computations Department (ACD) has developed the first parallel Finite Element 3D Particle-In-Cell (PIC) code, Pic3P, for simulations of RF guns and other spacecharge dominated beam-cavity interactions. Pic3P solves the complete set of Maxwell-Lorentz equations and thus includes space charge, retardation and wakefield effects from first principles. Pic3P uses higher-order Finite ...

2005
I. Ben-Zvi A. Burrill R. Calaga P. Cameron X. Chang D. Gassner H. Hahn A. Hershcovitch H. C. Hseuh P. Johnson D. Kayran J. Kewisch R. Lambiase V. Litvinenko G. McIntyre A. Nicoletti J. Rank T. Roser J. Scaduto K. Smith T. Srinivasan-Rao K.-C. Wu A. Zaltsman Y. Zhao H. Bluem A. Burger M. Cole A. Favale D. Holmes J. Rathke T. Schultheiss A. Todd

High-power Free-Electron Lasers were made possible by advances in superconducting linacs operated in energy-recovery mode. In order to get to very high power levels, say a fraction of a megawatt average power, many technological barriers are yet to be broken. We describe work on CW, high-current and high-brightness electron beams. This will include descriptions of a superconductinglaser-photoca...

2011
R. Agustsson L. Faillace A. Murokh

An X-band Traveling wave Deflector mode cavity (XTD) has been developed at Radiabeam Technologies to perform longitudinal characterization of the subpicosecond ultra-relativistic electron beams. The device is optimized for the 100 MeV electron beam parameters at the Accelerator Test Facility (ATF) at Brookhaven National Laboratory, and is scalable to higher energies. The XTD is designed to oper...

1997
Daniel White Joseph Koning Lawrence Livermore

We are interested in determining the electromagnetic fields within closed perfectly conducting cavities that may contain dielectric or magnetic materials. The vector Helmholtz equation is the appropriate partial differential equation for this problem. It is well known that the electromagnetic fields in a cavity can be decomposed into distinct modes that oscillate in time at specific resonant fr...

2012
Hyoung Suk Kim

Understanding electromagnetic wave phenomena is very important to be able to design RF cavities such as for atmospheric microwave plasma torch, microwave vacuum oscillator/amplifier, and charged-particle accelerator. This chapter deals with some electromagnetic wave equations to show applications to develop the analytic design formula for the cavity. For the initial and crude design parameter, ...

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