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simulation

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MOPB01 Fully Electromagnetic FEL Simulation via Lorentz-Boosted Frame Transformation undulator, FEL, radiation, electron 48
 
  • W.M. Fawley, J.-L. Vay
    LBNL, Berkeley, California
 
 

Numerical electromagnetic simulation of some systems containing charged particles with highly relativistic directed motion can by sped up by orders of magnitude by choice of the proper Lorentz-boosted frame*. A particularly good application for boosted frame calculation is short wavelength FEL simulation. In the optimal boost frame (i.e., the ponderomotive rest frame), the red-shifted FEL radiation and blue-shifted undulator field have identical wavelengths and the number of required time-steps for fully electromagnetic simulation (relative to the laboratory frame) decreases by a factor of gamma squared. We have adapted the WARP code** to apply this method to several FEL problems including coherent spontaneous emission from prebunched e-beams, strong exponential gain in a single pass amplifier configuration, and FEL emission from e- beams in undulators with multiple harmonic components. We discuss our results and compare with those obtained using the "standard" FEL simulation approach which applies the eikonal and wiggler-period-averaging approximations.


* J.-L. Vay, Phys. Rev. Lett. 98, 130405 (2007).
** D.P. Grote, A. Friedman, J.-L. Vay, and I. Haber, AIP Conf. Proc. 749, 55 (2005).

 
MOPB23 Three-Dimensional Modes of a Lamellar Grating for Smith-Purcell Experiments radiation, bunching, electron, gun 83
 
  • J.T. Donohue
    CENBG, Gradignan
  • J. Gardelle
    CESTA, Le Barp
 
 

Several years ago Andrews and Brau * presented a two-dimensional (2-D) theory for the production of coherent Smith-Purcell radiation by an initially continuous beam. An essential component of their analysis was the dispersion relation for a lamellar grating (i.e., rectangular profile) relating frequency and axial wave number k. Both simulations and an experiment performed at CESTA ** using a wide beam have confirmed the validity of their approach. However, all gratings are three-dimensional objects, and one may ask what modifications of the theory might be necessary. We present here our solution to the problem, which assumes a progressive wave in the direction of the grooves, with wave number q. A surprisingly simple modification of the Andrews and Brau 2-D dispersion relation is found. We have extensively tested our theory, both with simulations using the 3-D PIC code "MAGIC", and with measurements of the properties of the surface wave on the CESTA grating made using a network analyzer. Extremely good agreement is found, both with and without sidewalls on the grating.


* H. L. Andrews and C. A. Brau, Phys. Rev. ST Accel. Beams 7, 070701 (2004).
** J. Gardelle, L. Courtois, P. Modin and J.T. Donohue, Phys. Rev. ST Accel. Beams 12, 110701 (2009).

 
MOPB32 Beam Quality and Transport Stability Simulations in Echo Enabled Harmonic Generation bunching, electron, undulator, laser 99
 
  • J. Henderson, B.W.J. McNeil
    USTRAT/SUPA, Glasgow
  • D.J. Dunning
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

The method of Echo Enabled Harmonic Generation is a possible method of achieving coherent short wavelengths in an FEL amplifier. In this paper the effects of noise variations is some of the important parameters affecting the stability of the final harmonic bunching of the electron beam are investigated numerically.

 
MOPC08 Measurement of Sliced-Bunch Parameters at FLASH FEL, radiation, diagnostics, electron 131
 
  • C. Behrens, C. Gerth
    DESY, Hamburg
 
 

The capability of the free-electron laser (FEL) user facility FLASH at DESY was expanded by several upgrades during the shutdown in 2009/2010. A key extension is the installation of a third-harmonic (3.9 GHz) RF system for the linearization of the longitudinal phase space in front of the bunch compressors. In order to control the bunch compression and make full use of the third-harmonic RF system, a new diagnostic section for the measurements of sliced bunch parameters directly in front of the undulators was designed and commissioned. In this paper, we describe the beam imaging systems and their optical performance. The achievable resolution of both time and energy is shown and compared to the design values. First measurements of the linearized longitudinal phase space with high resolution are presented.

 
MOPC16 Transverse-Coherence Properties of the FEL at the LCLS FEL, undulator, electron, radiation 151
 
  • Y.T. Ding, Z. Huang
    SLAC, Menlo Park, California
  • S.A. Ocko
    MIT, Cambridge, Massachusetts
 
 

The Linac Coherent Light Source has achieved stable operation at x-ray wavelengths of 20-1.2 Angstrom with peak brightness many orders of magnitude beyond conventional synchrotron sources. Understanding transverse coherence properties of such a SASE source is of great practical importance for user experiments. Based on a fast Monte Carlo algorithm, we present numerical analysis of the LCLS coherence properties for the simulated radiation fields at different wavelengths and bunch charges.

 
MOOCI1 FEL Simulations: History, Status and Outlook electron, FEL, undulator, radiation 165
 
  • S. Reiche
    PSI, Villigen
 
 

The coupled system of radiation interacting with a co-propagating electron beam within an undulator of an FEL exhibits many degrees of freedom. Only in an idealized and simplified model can the FEL equations be solved analytically and a more complete description requires numerical methods. Therefore numerical codes have been developed along with the advances in FEL theory, starting from a simple 1 D model to today's fully time-dependent 3D simulations, utilizing large scale parallel computers. This presentation gives a brief history of FEL simulation and addresses the remaining challenges in FEL modeling which we hope to solve in the near future.

 

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MOOCI2 Coherence Properties of the Radiation From X-Ray FELs FEL, radiation, electron, emittance 173
 
  • E. Schneidmiller, M.V. Yurkov
    DESY, Hamburg
 
 

Start-up of the amplification process in x-ray FELs from the shot noise in the electron beam defines a specific behavior of longitudinal and transverse coherence properties of the radiation. Particularly important is the case of an x-ray FEL optimized for maximum gain of the fundamental radiation mode. Applying similarity techniques to the results of numerical simulations allowed us to find universal scaling relations for the main characteristics of an optimized X-ray FEL operating in the saturation regime: efficiency, coherence time and degree of transverse coherence. We find that with an appropriate normalization of these quantities, they are functions of only the ratio of the geometrical emittance of the electron beam to the radiation wavelength. Statistical and coherence properties of the higher harmonics of the radiation are highlighted as well.

 

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TUPA05 Mode-Stability in FEL Oscillators FEL, coupling, cavity, electron 219
 
  • S. Krishnagopal, S.A. Samant
    BARC, Mumbai
 
 

Mode stability can restrict the tuning range of FEL oscillators. We investigate the stability of FEL oscillators as a function of wavelength as well as size of the coupling hole. We show that concentric configurations are preferred to confocal ones. We study mode-stability using multi-particle simulations, for both, symmetric as well as asymmetric modes.

 
TUPA07 Dependence of Gain on Current in the Coherent Smith-Purcell Experiment at Cesta radiation, bunching, electron, cathode 226
 
  • J.T. Donohue
    CENBG, Gradignan
  • J. Gardelle, P. Modin
    CESTA, Le Barp
 
 

At FEL 2009, we presented experimental results on coherent Smith-Purcell obtained at CESTA in the microwave frequency domain * . Those results strongly supported the two-dimensional theory proposed by Andrews and Brau some years ago ** , and were consistent with simulations performed with the PIC code "MAGIC". That experiment used a large current, 200 A, for a grating of width 10 cm. In a follow-up experiment, emittance slits were used to reduce the current to as low as 2 A, with a quite thin, flat, and wide beam. The gain as a function of current and also of vertical beam position was measured in detail. In particular, the start current for our set-up was found. In parallel, 2-D simulations of the experiment with "MAGIC" were extensively compared with the experimental results. Very good agreement between simulations and experiment is obtained. This lends confidence that simulations of a scaled-down version of our experiment will be a reliable guide for Terahertz frequency coherent Smith Purcell experiments. Such simulations suggest that radiation in the range 100-200GHz should be feasible.


* J. T. Donohue, J. Gardelle, L. Courtois and P Modin, Proceeedings of FEL 2009.
** H. L. Andrews and C. A. Brau, Phys. Rev. ST Accel. Beams 7, 070701 (2004).

 
TUPA12 XFEL Oscillator Simulation Including Angle-Dependent Crystal Reflectivity undulator, FEL, radiation, electron 234
 
  • W.M. Fawley
    LBNL, Berkeley, California
  • K.-J. Kim, R.R. Lindberg, Yu. Shvyd'ko
    ANL, Argonne
 
 

The oscillator package within the GINGER FEL simulation code has now been extended to include angle-dependent reflectivity properties of Bragg crystals. Previously, the package was modified to include frequency-dependent reflectivity in order to model x-ray FEL oscillators[*] from start up from shot noise to saturation. We will present a summary of the algorithms used for modeling the crystal reflectivity and radiation propagation outside the undulator, discussing various numerical issues relevant to the domain of high Fresnel number and efficient Hankel transforms. We give some sample XFEL-O simulation results obtained with the angle-dependent reflectivity model, with particular attention directed to the longitudinal and transverse coherence of the radiation output.


[*] R.R. Lindberg et al., submitted to PRST-AB, 2010.

 
TUPB08 Staged Self-Seeding Scheme for Narrow Bandwidth, Ultra-Short X-ray Harmonic Generation Free Electron Laser at LINAC Coherent Light Source FEL, undulator, electron, photon 266
 
  • J. Wu, P. Emma, J.B. Hastings
    SLAC, Menlo Park, California
  • C. Pellegrini
    UCLA, Los Angeles, California
 
 

Success of the world's first x-ray (0.15-1.5 nm) free electron laser (FEL) - LCLS - at SLAC opens the gate for new science. In this paper, we study the FEL performance for a two-stage self-seeding scheme by introducing a photon monochromator and an electron by-pass in the undulator system. The FEL generated in the first part of the undulator system is purified in spectrum, recombines with the electron bunch, and is amplified in the second part of the undulator system to saturation. Such modifications will improve the FEL longitudinal coherence, reducing the FEL band-width by two-orders of magnitude, but with similar peak power; hence improving the peak brightness by two-orders of magnitude. Such a self-seeding scheme is studied for both soft x-ray (200 eV to 2 keV) and hard x-ray (800 eV to 8 keV) cases with single electron bunch. The photon monochromator system is configurated as variable line spacing gratings for soft x-ray and single crystal for hard x-ray. Harmonic Generation and Chirped FEL are also considered aiming at reaching even shorter wavelength x-ray photons and at generating FEL pulse with even shorter temporal duration, respectively.

 
TUPB12 Noise Amplification in Echo-Enabled Harmonic Generation (EEHG) undulator, laser, FEL, electron 278
 
  • G.V. Stupakov, Z. Huang, D.F. Ratner
    SLAC, Menlo Park, California
 
 

It is generally accepted that harmonic-generation seeding in FELs amplifies the noise in the beam and enhances the spontaneous component of the FEL radiation. In this paper we analyze the noise dynamics caused by particle interaction in the undulators of the EEHG seeding mechanism. We develop a 1D model of the noise evolution through the system and calculate the amplification factor as a function of frequency. Our results are applied to a typical soft x-ray EEHG FEL.

 
TUPB13 Echo-Seeding Options for LCLS-II radiation, laser, FEL, bunching 282
 
  • D. Xiang, G.V. Stupakov
    SLAC, Menlo Park, California
 
 

The success of LCLS has opened up a new era of x-ray sciences. An upgrade to LCLS is currently being planned to enhance its capabilities. In this paper we study the feasibility of using the echo-enabled harmonic generation (EEHG) technique to generate narrow bandwidth soft x-ray radiation in the proposed LCLS-II soft x-ray beam line. We focus on the conceptual design, the technical implementation and the expected performances of the echo-seeding scheme. We will also show how the echo-seeding scheme allows one to generate two color x-ray pulses with the higher energy photons leading the lower energy ones as is favored by the x-ray pump-probe experiments.

 
TUPB16 Numerical Study on Coherent Harmonic Generation Free Electron Laser Seeded by Chirped External Laser laser, FEL, electron, radiation 286
 
  • H. Zen, M. Adachi, M. Katoh
    UVSOR, Okazaki
  • M. Hosaka, Y. Taira, N. Yamamoto
    Nagoya University, Nagoya
  • T. Tanikawa
    Sokendai - Okazaki, Okazaki, Aichi
 
 

Coherent Harmonic Generation Free Electron Laser (CHG-FEL)* ** is a short pulse and coherent radiation source in vacuum ultra-violet regime. A measurement of CHG-FEL spectrum*** has been done and sidebands in spectrum were observed under an over-bunching condition. The measurement was done with chirped seed laser to avoid strong over-bunching of electron beam and to obtain larger pulse energy for high signal to noise ratio. In the paper ***, however, the seed laser chirping was not taken into account in the numerical analysis and the numerical results qualitatively agreed with experimental results but quantitatively not. We consider that the discrepancy was caused by the chirping property of the seed laser, and thus we have developed a time dependent simulation code which can deal the effect of seed laser chirping. Results of the code qualitatively agreed well with the shape of measured spectrum, not only bandwidth but also the sideband structure. And the code was used to evaluate the temporal and spectral property of CHG-FEL seeded by a chirped laser. The code revealed the spectral widening and chirped property of CHG-FEL pulse when the CHG-FEL is driven by a chirped seed laser.


* L. H. Yu et al., Phys. Rev. A 44, 5178 (1991).
** G. D. Ninno et al., Phys. Rev. Lett. {10}1, 053902 (2008).
***M. Labat et al., Phys. Rev. Lett. {10}2, 014801 (2009).

 
TUPB23 Experimental Demonstration of Wideband Tunability of an Ultrafast Laser-Seeded Free-Electron Laser electron, FEL, laser, radiation 302
 
  • X. Yang, Y. Hidaka, J.B. Murphy, B. Podobedov, S. Seletskiy, Y. Shen, X.J. Wang
    BNL, Upton, Long Island, New York
 
 

We report the first experimental characterization of the wideband tunability of an ultrafast laser seeded FEL using a short seed laser pulse (140 fs in FWHM) and a variable energy electron beam. The experiments were conducted at the NSLS SDL and the FEL output spectrum and pulse energy were measured versus the electron beam energy. A significant spectral tuning range (8%) was observed. The experiment is in good agreement with predictions using the Perseo simulation code.

 
TUOCI2 Tunable Soft X-Ray Oscillator FEL, cavity, laser, electron 315
 
  • J.S. Wurtele, G. Penn, M.W. Reinsch
    LBNL, Berkeley, California
  • P.R. Gandhi, X.W. Gu, J.S. Wurtele
    UCB, Berkeley, California
  • K.-J. Kim, R.R. Lindberg, A. Zholents
    ANL, Argonne
 
 

A concept for a tunable soft x-ray free electron laser (FEL) oscillator is proposed and studied numerically. It is based on the idea of echo enabled harmonic generation [1] and takes advantage of the oscillator’s ability to start up from spontaneous emission, thereby eliminating the need for optical lasers. In the proposed concept, harmonic tunability is accomplished through beam manipulations using magnetic chicanes and a tunable radiator while two FEL oscillators remain at a fixed frequency. An additional advantage of the proposed technique is the possibility to utilize multilayer x-ray mirrors with a high backward reflectivity of the order of 70%, allowing the initial beam manipulation to be accomplished at a short wavelength, close to the final soft x-ray output. The high repetition rate soft x-ray output is expected to have longitudinal coherence and a narrow bandwidth.


[1] G. Stupakov, PRL, 2009

 

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WEOAI1 Pulse-Splitting in Short Wavelength Seeded Free Electron Laser laser, electron, FEL, free-electron-laser 329
 
  • M. Labat, M.-E. Couprie
    SOLEIL, Gif-sur-Yvette
  • S. Bielawski, C. Szwaj
    PhLAM/CERCLA, Villeneuve d'Ascq Cedex
  • C. Bruni
    LAL, Orsay
  • N. Joly
    University of Erlangen-Nuremberg, Erlangen-Nuremberg
 
 

We investigate a dynamical behaviors occurring in single-pass free electron lasers (FELs), depending on the electron beam, undulator and seed laser parameters. We put in evidence a complex spatiotemporal deformation of the amplified pulse, leading ultimately to a pulse splitting effect with two sub-pulses. This phenomenon has been first observed in PERSEO simulations in the case of ARC-EN-CIEL project studies, and then been analyzed more in details with the Colson-Bonifacio FEL equations. This studies reveal that slippage length as well as the seed laser pulse wings are the main ingredients of this dynamics [1]. We show that the splitting results from the nonhomogeneous saturation of the gain by the optical field copropagating with the electron beam.


M.Labat et al. “Pulse-splitting in short wavelength seeded free electron laser,” Phys. Rev. Lett. {10}3, 264801 (2009)

 

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WEOBI2 Ultra-Short Low Charge Operation at FLASH and the European XFEL radiation, emittance, FEL, collective-effects 345
 
  • I. Zagorodnov
    DESY, Hamburg
 
 

The Free Electron Laser in Hamburg (FLASH) is a SASE FEL user facility and in addition serves as a prototype for the European XFEL. The recent upgrade of FLASH with a higher harmonic RF module opens a new possibility for ultra-short low charge operation. The advantage of small transverse emittance at low charges can be used only with strong, linearized bunch compression. At this report we consider simulations of the beam dynamics at low charges and estimate the expected properties of the radiation at FLASH and the European XFEL. We present first experimental results at FLASH.

 

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WEOB4 Implementation of Single-Stage ECHO-Enabled Harmonic Generation on the FERMI@eELETTRS FEL FEL, electron, laser, undulator 354
 
  • E. Allaria
    ELETTRA, Basovizza
  • G. De Ninno
    University of Nova Gorica, Nova Gorica
 
 

FERMI@Elettra will have two different seeded FELs for covering the spectral range between 80 and 4nm. The shorter wavelength FEL, namely FEL-2, will cover the spectral range between 20 and 4 nm, and will be based on a double cascade high gain harmonic generation scheme. Moreover, the system has been designed to allow the implementation of other seeding schemes, like seeding with high-order harmonics generated in gas and echo-enhanced harmonic generation (EEG). In this work, we present the studies on the possible implementation on FERMI of the EEHG, reporting about the expected performance. The number of photons per pulse and the FEL bandwidth are calculated by means of time dependent start-to- end simulations.

 

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WEPA07 Variable Gap Undulator for 1.5-48 keV Free Electron Laser at LINAC Coherent Light Source FEL, electron, undulator, photon 370
 
  • C. Pellegrini
    UCLA, Los Angeles, California
  • J. Wu
    SLAC, Menlo Park, California
 
 

Success in commissioning the world's first x-ray (0.15-1.5 nm) free electron laser (FEL) - the LINAC Coherent Light Source (LCLS) - at SLAC National Accelerator Laboratory opens the gate for new science. Further improving the FEL spectrum bandwidth, shortening the FEL pulse temporal duration, and generating even higher energy x-ray photons are urged by various potential users. In this paper, we study the possibility of generating femtosecond duration X-ray pulses with a variable photon energy from 1.5 to 48 keV, using an electron beam with the same characteristics of the LCLS beam, and a planar undulator with additional focusing. We assume that the beam energy can be changed, and the undulator has a variable gap, allowing the undulator parameter to be changed from zero to a maximum value. It is assumed to be operated in an ultra-low charge and ultra-short pulse regime.

 
WEPB07 Investigations on the Impact of Modulations of the Transverse Laser Profile on the Transverse Emittance at PITZ emittance, electron, laser, cathode 406
 
  • M. Hänel, M. Krasilnikov, F. Stephan
    DESY Zeuthen, Zeuthen
 
 

The Photoinjector Test Stand at DESY, Zeuthen site (PITZ) was established to develop and optimize electron bunch sources for linac-based free electron lasers like FLASH or the future European XFEL. The successful operation of such FELs requires electron bunches of very low normalized transverse emittance of the order of 1 mm mrad at a charge of 1 nC. One key issue for obtaining low-emittance electron bunches is the possibility to influence the electron bunch properties by varying the photocathode laser pulse characteristics. This contribution focuses on the discussion of deviations from the optimum transverse shape of a circular flat-top. Different types of modulations are added to the flat-top and the resulting change in transverse emittance will be discussed based on beam dynamics simulations.

 
WEPB10 Low-charge Simulations for Phase Space Tomography Diagnostics at the PITZ Facility emittance, space-charge, electron, quadrupole 414
 
  • J. Saisut, G. Asova, M. Krasilnikov, S. Rimjaem, F. Stephan
    DESY Zeuthen, Zeuthen
  • J. Saisut
    ThEP Center, Commission on Higher Education, Bangkok
  • C. Thongbai
    Chiang Mai University, Chiang Mai
 
 

The Photo-Injector Test Facility at DESY, Zeuthen site (PITZ) aims to optimize high brightness electron sources for linac-based FELs. Since the performance of an FEL strongly depends on the transverse electron beam emittance, the electron source is studied in details at PITZ by measuring the emittance with the help of the Emittance Measurement Systems (EMSYs). The EMSY employs the slit scan technique which is optimized for 1nC bunch charge and, therefore, it might not be an optimal choice for low charge bunches. To extend the ability of the facility for transverse phase space measurements, a module for phase-space tomography diagnostics and its matching section are installed in 2010. The basic components of the module are four screens separated by FODO cells. It is designed for operation with high charge and low energy beams*. This work studies the performance of the tomography module when it is operated with low charge beams. The influence of different beam parameters is evaluated according to the requirement to match the envelope to the optics of the FODO lattice. Simulation results and phase space reconstructions are presented.


G. Asova et al., ‘Design considerations for phase space tomography diagnostics at the PITZ facility', proceedings of DIPAC 2007, Mestre, Italy.

 
WEPB37 Multiobjective Optimization for the Advanced Photoinjector Experiment (APEX) emittance, FEL, electron, gun 479
 
  • C. F. Papadopoulos, J.N. Corlett, D. Filippetto, J. Qiang, F. Sannibale, J.W. Staples, M. Venturini, M.S. Zolotorev
    LBNL, Berkeley, California
 
 

The Advanced Photoinjector Experiment (APEX) is a part of the Next Generation Light Source (NGLS), a proposed soft x-ray FEL concept being studied at LBNL. The requirements for the beam delivered to the FELs pose restrictions on the beam parameters at the injector. In addition, different modes of operation of the machine may pose different requirements on the beam. In order to optimize the performance of the injector, a genetic multiobjective algorithm has been used. A genetic algorithm is used because of the inherent complexity of the beam dynamics at the energy range in question (0-30 MeV) and the large number of parameters available for optimization. On the other hand, the multiplicity of requirements on the beam, which include beam emittance, beam pulse length, energy chirp, as well as pulse shape and peak current, leads to a mutliobjective approach for the optimization technique. In this paper, we present the status of the optimization simulations, using the ASTRA particle-in-cell code. Different injector setups are presented and the resulting transport solutions are compared to each other and the requirements of the downstream sections of the accelerator.

 
WEPB45 Benchmarking Multipacting Simulation for FEL Components electron, plasma, cathode, free-electron-laser 501
 
  • P. Stoltz, C. Nieter, C. Roark
    Tech-X, Boulder, Colorado
  • J.D.A. Smith
    TXUK, Warrington
 
 

Multipacting is a potential limit on the power one can deliver to different components of an FEL source, including the power couplers and the electron source cathode. Simulation is a main tool in helping to understand and mitigate multipacting. We present recent work on benchmarking multipacting simulation, including comparison with other codes and with rectangular waveguide experiment.

 
WEPB50 Models of Space-Charge Induced Optical Micro-Bunching electron, space-charge, bunching, plasma 512
 
  • A. Marinelli, J.B. Rosenzweig
    UCLA, Los Angeles, California
 
 

Longitudinal space-charge forces can be a major source of micro-bunching instability. We will discuss a three-dimensional theoretical model for the high frequency limit of space-charge interactions leading to density modulation at the optical scale. Particular emphasis will be given to the effect of transverse thermal motion on the angular distribution of micro-bunching and to its connection to the physics of Landau damping in longitudinal plasma oscillations. A comparison with the results of high resolution molecular dynamics simulations will also be discussed.

 
WEOC4 Phase Space Measurements with Tomographic Reconstruction at PITZ quadrupole, emittance, focusing, laser 529
 
  • G. Asova, J.W. Bähr, H.-J. Grabosch, L. Hakobyan, M. Hänel, Ye. Ivanisenko, M.A. Khojoyan, G. Klemz, M. Krasilnikov, M. Mahgoub, M. Otevrel, B. Petrosyan, S. Rimjaem, A. Shapovalov, L. Staykov, F. Stephan, G. Vashchenko
    DESY Zeuthen, Zeuthen
  • S. Lederer
    DESY, Hamburg
  • B.D. O'Shea
    UCLA, Los Angeles, California
  • D. Richter
    HZB, Berlin
 
 

The major objectives of the Photo-Injector Test Facility at DESY in Zeuthen, PITZ, are research and development of high brightness electron sources suitable to drive FELs like FLASH and the European XFEL. In the 2008/2009 run period the facility has been operated with a new photo-cathode laser system and a dry-ice cleaned RF gun cavity. Characterization of the transverse phase space of the electron source has been performed in details using a single slit scan technique with a dedicated Emittance Measurement System. In preparation for the forthcoming run, a number of quadrupole magnets have been installed and tomography reconstruction with data from quadrupole scans with two magnets has been carried out in semi-parallel manner to the slit scans. This contribution summarizes the experience from the phase-space tomography reconstruction with nominal beam conditions. Advantages and drawbacks of the measurement procedure and the analysis are superimposed and results are compared to ones obtained with the slit scans.

 

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THOB3 Preliminary Study for the OFFELO FEL, radiation, electron, feedback 554
 
  • Y. Hao, V. Litvinenko
    BNL, Upton, Long Island, New York
 
 

OFFELO (optics-free FEL oscillator) is a brand new idea for obtaining hard X-ray wavelength radiation using an oscillator without concerning the damage to the mirror. By using an extra electron beam to transport the radiation information, OFFELO also provide pleasant flexibility compared with traditional oscillator scheme. We simulated the lasing process and carry out the saturation condition and explore other properties of this scheme.

 

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THOB4 Mode Locked Optical Klystron Configuration in an FEL Cavity Resonator FEL, cavity, electron, radiation 558
 
  • B.W.J. McNeil
    USTRAT/SUPA, Glasgow
  • N. Thompson
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

Chicanes placed between undulator modules in a high-gain FEL amplifier have been shown to generate a set of axial modes that may be locked to generate attosecond pulse trains in the x-ray [1]. Using numerical simulations, it is shown in this paper that a similar system of undulator/chicane modules may be used in a low-gain FEL cavity resonator to generate a equally spaced set of frequency modes with a spacing much greater than those of the cavity. As with the high-gain FEL amplifier case, these mode can lock to generate a pulse train.


[1] N.R. Thompson & B.W.J. McNeil, Phys. Rev. Lett. 100, 203901 (2008)

 

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THPB04 Emittance Growth Induced by Microbunching Instability in the FERMI@Elettra High Energy Transfer Line emittance, optics, lattice, quadrupole 608
 
  • S. Di Mitri, M. Cornacchia
    ELETTRA, Basovizza
  • W.A. Barletta
    LBNL, Berkeley, California
 
 

Simulations of the microbunching instability through the FERMI@elettra lattice have been carried out with elegant particle tracking code. This paper focuses on the emittance growth induced by the microbunching instability in the high energy transfer line that guides the electron beam from the linac to the undulator chain. The perturbation to the transverse emittance induced by coherent synchrotron radiation and longitudinal space charge as function of the R56 transport matrix element in the transfer line have been investigated separately and in the presence of their mutual interaction. Simulation results show that the betatron phase mismatch may have a detrimental impact on the final beam emittance.

 
THPB13 A Simulation for the Optimization of Bremsstrahlung Radiation for Nuclear Applications Using Laser Accelerated Electron Beam electron, photon, laser, radiation 618
 
  • H.H. Lee, K. Min
    KAIST, Daejeon
  • Y.U. Jeong, K. Lee, S. H. Park
    KAERI, Daejon
  • H. Seo
    Hanyang University, Seoul
  • H. Shim
    Korea University, Seoul
 
 

Laser accelerated electron beam can be a compact source for high energetic photon generation for nuclear application. A simulation code using GEANT4 has been developed for the estimation of Bremsstrahlung radiation from laser accelerated electron beams impinging on a metalic target and the photonuclear reaction of a sample target. It includes ElectroMagnetic physics , Photonuclear reaction and Radio Active Decay physics, so that the calculation from Bremsstrahlung radiation to decay process can be conveyed in series. The energy and angular distribution of Bremsstrahlung radiation depending on different target thickness and electron parameters as well as the emission spectrum by radioactive decay due to photonuclear reaction can give us an idea of optimal condition for the desired nuclear applications. We discussed the critical issues of high energy photon generation for photonuclear reaction experiments.

 
THPC11 Cavity BPM Design, Simulations and Testing for the FERMI@Elettra Project cavity, electron, diagnostics, linac 671
 
  • P. Craievich
    ELETTRA, Basovizza
  • M. Dal Forno
    DEEI, Trieste
 
 

The cavity Beam Position Monitor (BPM) is a fundamental beam diagnostic instrument for a seeded FEL, like FERMI@Elettra. It allows the measurements of the electron beam trajectory in a non-destructive way and with sub-micron resolution. The high resolution cavity BPM relies on the excitation of the dipole mode that is originated when the bunch passes off axis in the cavity. In this paper we present the prototype of cavity BPM developed for the FERMI@Elettra facility. The RF parameters of the cavities have been determined by means of Ansoft HFSS; while using the CST Particle Studio the level of the output signals from the cavities have been also estimated. Furthermore, the design of the RF frontend for the acquisition and conditioning of the signals from the BPM cavities is presented as well. The prototype has been succesfully installed in the FERMI Linac during the last commissioning phase and preliminary results with the electron beam are also presented.