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MOOBI2 XFEL/SPring-8 Construction and SCSS Operation Status undulator, LLRF, status, klystron 20
 
  • T. Shintake
    RIKEN/SPring-8, Hyogo
 
 

XFEL/SPring-8 construction was started in 2006, aiming at generating X-ray laser at 1 Angstrom. The building construction was completed in April 2009, followed by installation of accelerator components. In March 2010, we completed all accelerating structure installation. The klystron modulator and LLRF systems are under installation. We use 19 undulator of in-vacuum type (5 m each). At this moment 10 undulators have been installed and careful qualification of undulator field is carried out. We will start high power processing in this October, and we will send the first electron beam into beam dump before April 2011, followed by beam commissioning for X-ray lasing.

 

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WEPB05 Conditioning of a New Gun at PITZ Equipped with an Upgraded RF Measurement System gun, laser, electron, cavity 398
 
  • M. Otevrel, G. Asova, J.W. Bähr, M. Hänel, Ye. Ivanisenko, M. Krasilnikov, M. Mahgoub, D.A. Malyutin, A. Oppelt, S. Rimjaem, F. Stephan, M. Tanha, G. Vashchenko, X.H. Wang
    DESY Zeuthen, Zeuthen
  • A. Brinkmann, K. Flöttmann, D. Reschke
    DESY, Hamburg
  • M.A. Khojoyan
    YerPhI, Yerevan
  • J. Saisut
    Chiang Mai University, Chiang Mai
 
 

A new photocathode electron gun is about to be characterized at PITZ*. It is an L-band normal conducting 1.6 copper cell cavity with improved cooling system. It has the same design as the previously installed gun, characterized at PITZ during the run period 2008/9**. Due to the particle-free surface cleaning method utilizing dry ice, a significant reduction of the dark current was achieved in case of the previously tested cavity. This effect is also expected for the new gun. To improve the accuracy of the RF power measurement and control, a new in-vacuum directional coupler was installed between the T-combiner combining the two 5 MW arms of the RF source and the input coaxial coupler. The new in-vacuum coupler will provide much more accurate information about the RF power in the gun and will allow applying appropriate control feedback. Consequently improved stability of the gun operation is expected. Tuning and conditioning results of this new gun cavity will be presented as well as the results of the measurements of the gradient and the gun phase measurements using this new coupler.


* Photoinjector Test Facility at Zeuthen
** S. Rimjaem et al., EPAC 2008, Genoa, Italy.

 
WEPB36 Status of the LBNL Normal-conducting CW VHF Electron Photo-gun cathode, cavity, gun, laser 475
 
  • F. Sannibale, B.J. Bailey, K.M. Baptiste, A.L. Catalano, D. Colomb, J.N. Corlett, S. De Santis, L.R. Doolittle, J. Feng, D. Filippetto, G. Huang, R. Kraft, D. Li, H.A. Padmore, C. F. Papadopoulos, G.J. Portmann, S. Prestemon, J. Qiang, J.W. Staples, M.E. Stuart, T. Vecchione, R.P. Wells, M.S. Zolotorev
    LBNL, Berkeley, California
  • M. J. Messerly, M.A. Prantil
    LLNL, Livermore, California
  • M. Yoon
    POSTECH, Pohang, Kyungbuk
 
 

The fabrication and installation at the Lawrence Berkeley National Laboratory of a high-brightness high-repetition rate photo-gun, based on a normal conducting 187 MHz (VHF) RF cavity operating in CW mode, is in its final phase. The cavity will generate an electric field at the cathode plane of ~20 MV/m to accelerate the electron bunches up to ~750 keV, with peak current, energy spread and transverse emittance suitable for FEL and ERL applications. The gun vacuum system has been designed for pressures compatible with high quantum efficiency but "delicate" semiconductor cathodes to generate up to a nC bunches at MHz repetition rate with present laser technology. Several photo-cathode/laser systems are under consideration, and in particular photo-cathodes based on K2CsSb are being developed and have already achieved a QE of 8% at 532 nm wavelength, or close to 20% including the Schottky barrier lowering. The cathode will be operated by a microjoule fiber laser in conjunction with refractive optics to create a flat top transverse profile, as well as a birefringent pulse stacker to create a flat top temporal profile. The present status and the plan for future activities are presented.

 
WEPB43 A Low-Energy RF Deflector for the FERMI@Elettra Project cavity, linac, coupling, pick-up 493
 
  • P. Craievich, S. Biedron, M. Ferianis, D. La Civita
    ELETTRA, Basovizza
  • D. Alesini, L. Palumbo
    INFN/LNF, Frascati (Roma)
  • L. Ficcadenti
    Rome University La Sapienza, Roma
  • M. Petronio, R. Vescovo
    DEEI, Trieste
 
 

A RF deflector is a useful tool to completely characterize the beam phase space by means of measurements of the bunch length and the transverse slice emittance. At FERMI@Elettra, a soft X-ray next-generation light source under development at the Sincrotrone Trieste laboratory in Trieste, Italy, we are installing low-energy and high-energy deflectors. In particular, two deflecting cavities will be positioned at two points in the linac. One will be placed at 1.2 GeV (high energy), just before the FEL process starts; the other at 250 MeV (low energy), after the first bunch compressor (BC1). This paper concerns only the low-energy deflector. The latter was built over the past year in collaboration with the SPARC project team at INFN-LNF-Frascati, Italy and the University of Rome. In this paper we will describe the RF measurements performed to characterize the standing wave cavity before the installation in the FERMI@Elettra linac, and we will compare them with the simulations done using the electromagnetic code HFSS.

 
WEPB46 Resonant Tunneling and Extreme Brightness from Diamond Field Emitters and Carbon Nanotubes electron, brightness, cathode, emittance 504
 
  • J.D. Jarvis, C.A. Brau, J.L. Davidson, N. Ghosh, B.L. Ivanov, J.L. Kohler
    Vanderbilt University, Nashville, TN
 
 

We report recent advances in the development of electron sources of extreme brightness approaching the quantum degenerate limit. These cathodes comprise either a diamond field emitter or carbon nanotube and an individual adsorbed atom or molecule. Both emitters are covalent carbon structures and thus have the benefits of high activation energy for atomic migration, chemical inertness, and high thermal conductivity. The single adsorbate produces surface states which result in dramatic resonant enhancement of the field emission current at the allowed energies of those states. The result is a beam with a narrow energy spread that is spatially localized to roughly the size of a single atom. Thus far, we have observed short lived (~1 sec) beams from residual gases of ~6 microamps corresponding to a normalized transverse brightness of ~3·1018 A/m2-str. Whereas conventional field emitters have a quantum degeneracy of <10-4, we estimate the degeneracy of our observed beams to be ~0.1. The use of metal adsorbates should stabilize the effect, allow higher current operation, and provide a long lived source whose brightness approaches the quantum limit.

 
THPC22 Performance of Bulk HTSC Staggered Array Undulator at Low Temperature undulator, solenoid, FEL, controls 679
 
  • R. Kinjo, M. A. Bakr, Y.W. Choi, K. Ishida, T. Kii, N. Kimura, K. Masuda, K. Nagasaki, H. Ohgaki, T. Sonobe, M. Takasaki, S. Ueda, K. Yoshida
    Kyoto IAE, Kyoto
 
 

The bulk high temperature superconductor staggered array undulator (Bulk HTSC SAU) has several advantages: such as strong magnetic field, potential of short period undulator, K value variability without gap control. In addition to these advantages, the Bulk HTSC SAU can be used near the electron beam because the undulator is expected to show good performance at 20 – 30 K. In the conference, we will report the expected performance of the undulator at low temperature through magnetic measurement by using a superconducting quantum interference device (SQUID) magnetometer. Also we will report the results of the first operation at 4 – 77 K of new prototype undulator consisting of a helium cooling system and a 2 T superconducting solenoid.

 
THOC4 Improvement in High-Frequency Properties of Beam Halo Monitor Using Dimond Detectors for SPring-8 XFEL electron, wakefield, undulator, radiation 700
 
  • H. Aoyagi, T. Bizen, N. Nariyama
    JASRI/SPring-8, Hyogo-ken
  • Y. Asano, T. Itoga, H. Kitamura, T. Tanaka
    RIKEN/SPring-8, Hyogo
 
 

An interlock sensor is indispensable to protect the undulator magnets against radiation damage. The beam halo monitor using diamond detectors, which are operated in photoconductive mode, has been developed for the X-ray free electron laser facility at SPring-8 (XFEL/SPring-8). Pulse-by-pulse measurements are adopted to suppress the background noise efficiently, and to improve the detective sensitivity. The feasibility tests of this monitor have been demonstrated at the SPring-8 compact SASE source (SCSS) test accelerator for SPring-8 XFEL. As the next step, we are trying to improve the high-frequency properties: (a) dimension of diamond detectors was newly designed to optimize the beam halo monitor for SPring-8 XFEL, (b) the microstripline structure is applied in the vacuum chamber to improve the high-frequency property, (c) RF fingers are also applied to suppress the effect of the wake field from intense electron beam. Details of these devices and experimental results are presented.

 

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