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Fukasawa, A.

Paper Title Page
WE1PBC05 Development of an Ultra-High Repetition Rate S-Band RF Gun for the SPARX Project 1815
 
  • L. Faillace, L. Palumbo
    Rome University La Sapienza, Roma
  • P. Frigola
    RadiaBeam, Marina del Rey
  • A. Fukasawa, B.D. O'Shea, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • B. Spataro
    INFN/LNF, Frascati (Roma)
 
 

We present here the design, including RF modelling, cooling, and thermal stress and frequency detuning, of an S-band RF gun capable of running near 500 Hz, for application to FEL and inverse Compton scattering sources. The RF design philosophy incorporates many elements in common with the LCLS gun, but the approach to managing cooling and mechanical stress diverges significantly. We examine the new proprietary approach of RadiaBeam Technologies for fabricating copper structures with intricate internal cooling geometries. We find that this approach may enable very high repetition rate, well in excess of the nominal project this design is directed for, the SPARX FEL.


*C.Limborg et al.,“RF Design of the LCLS Gun”,LCLS Technical Note LCLS-TN-05-3
**P. Frigola et al.,“A Novel Fabrication Technique for the Production of RF Photoinjectors”,published in EPAC08.

 

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Slides

 
WE5PFP013 Development of Solid Freeform Fabrication (SFF) for the Production of RF Photoinjectors 2015
 
  • P. Frigola, R.B. Agustsson, S. Boucher, A.Y. Murokh
    RadiaBeam, Marina del Rey
  • H. Badakov, A. Fukasawa, P. Musumeci, J.B. Rosenzweig, G. Travish
    UCLA, Los Angeles, California
  • D. Cormier, T. Mahale
    NCSU, Raleigh, North Carolina
  • L. Faillace
    INFN/LNF, Frascati (Roma)
 
 

Electron beam based additive fabrication techniques have been successfully applied to produce a variety of complex, fully dense, metal structures. These methods, collectively known as Solid Freeform Fabrication (SFF) are now being explored for use in radio frequency (RF) structures. SFF technology may make it possible to design and produce near-netshape copper structures for the next generation of very high duty factor, high gradient RF photoinjectors. The SFF process discussed here, Arcam Electron Beam Melting (EBM), utilizes an electron beam to melt metal powder in a layer-by-layer fashion. The additive nature of the SFF process and its ability to produce fully dense parts are explored for the fabrication of internal cooling passages in RF photoinjectors. Following an initial feasibility study of the SFF process, we have fabricated a copper photocathode, suitable as a drop-in replacement for the UCLA 1.6 cell photoinjector, with internal cooling channels using SFF. Material analysis of the prototype cathode and new designs for a high duty factor photoinjector utilizing SFF technology will be presented.

 
TH6REP049 Advanced Longitudinal Diagnostic for Single-Spike Operation at the SPARC FEL 4063
 
  • G. Marcus, G. Andonian, A. Fukasawa, P. Musumeci, S. Reiche, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • M. Ferrario, L. Palumbo
    INFN/LNF, Frascati (Roma)
  • L. Giannessi
    ENEA C.R. Frascati, Frascati (Roma)
 
 

It has been suggested that an ultra-short, very low charge beam be used to drive short wavelength single-spike operation at the SPARC FEL. This paper explores the development and construction of a longitudinal diagnostic capable of completely characterizing the radiation based on the Frequency-Resolved Optical Gating (FROG) technique. In particular, this paper explores a new geometry based on a Transient-Grating (TG) nonlinear interaction and includes studies of start to end simulations for pulses at the SPARC facility using GENESIS and reconstructed using the FROG algorithm. The experimental design, construction and initial testing of the diagnostic are also discussed.

 
FR5PFP056 Beam Dynamics and RF Cavity Design of a Standing/Traveling-Wave Hybrid Photoinjector for High Brightness Beam Generation 4434
 
  • A. Fukasawa, H. Badakov, B.D. O'Shea, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • D. Alesini, L. Ficcadenti, B. Spataro
    INFN/LNF, Frascati (Roma)
  • L. Palumbo
    Rome University La Sapienza, Roma
 
 

A hybrid photoinjector, which we present here, consists of a 6-cell traveling wave structure with a standard 1.6-cell RF gun attached to the one end and a 3-m long linac following for further acceleration. With this structure, no reflection observed at the input port. This enables to build the accelerator without a circulator which limits the power and the frequency of RF. From the beam dynamics point of view, the beam is produced as the normal RF guns and gets short by velocity bunching in the traveling wave section right after the gun. The peak current can reach more than 1 kA, with about 2 mm.mrad of the emittance at 20 MeV. We discuss more details about the beam dynamics as well as the RF structure.

 
FR5PFP057 Beam Dynamics Simulations of the Velocity Bunching in a Superconducting Linac 4437
 
  • A. Fukasawa, B.D. O'Shea, J.B. Rosenzweig
    UCLA, Los Angeles, California
 
 

The velocity bunching is a hot topic in normal conducting photoinjectors to generate high-brightness beams instead of magnetic chicanes in the low energy region. We apply this technique to the superconducting photoinjectors. The linac considered here consists of several 9-cell TESLA cavities, the standard 1.6-cell normal conducting RF gun is assumed, though. In the case of 1.1 nC injection, the peak current increases to 1 kA with 2.6 mm.mrad of the emittance. The peak current can be higher but the emittance becomes worse in that case, and vice versa. We discuss more details on the spot.

 
FR5RFP094 Development of a 1.5+0.5 Cell Photoinjector 4758
 
  • B.D. O'Shea, A. Fukasawa, J.T. Moody, P. Musumeci, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • L. Faillace
    Rome University La Sapienza, Roma
 
 

We present the status of development of a 1.5+0.5 cell photoinjector run in the blowout regime. LANL Parmela simulation results indicate a near uniform beam of slice energy spread on the order of 500 eV when neglecting thermal effects. We examine the use of an extra half cell to control longitudinal beam growth and compare the system in development with previous 1.6 cell photoinjector designs.