free electron laser projects x-fel and the others s. bertolucci infn

Download Free Electron Laser Projects X-FEL and the others S. Bertolucci INFN

If you can't read please download the document

Upload: kat

Post on 05-Jan-2016

30 views

Category:

Documents


2 download

DESCRIPTION

Free Electron Laser Projects X-FEL and the others S. Bertolucci INFN. European Initiatives. Scientific case: new research frontiers in. Atomic, molecular and cluster physics Plasma and warm dense matter Condensed matter physics Material science Femtosecond chemistry Life science - PowerPoint PPT Presentation

TRANSCRIPT

  • Free Electron Laser ProjectsX-FEL and the others

    S. BertolucciINFN

  • European Initiatives

  • Scientific case: new research frontiers in Atomic, molecular and cluster physics Plasma and warm dense matter Condensed matter physics Material science Femtosecond chemistry Life science Single Biological molecules and clusters Imaging/holography Micro and nano lithography

  • X-Ray FELs are based on SASE (no mirrors !) need Ultra-High Brightness e- BeamsSelf-Amplified-Spontaneous-Emission amplifies the spontaneous radiation exponentially in a single passInteraction of a bright electron beam with noise in an undulator magnet results in a density modulation of the electron bunch at the optical wavelength: SASE instability leads to COHERENT EMISSION

  • Undulator RadiationThe electron trajectory is inside the radiation cone ifThe electron trajectory is determined by the undulator field and the electron energy

  • Relativistic MirrorCounter propagating pseudo-radiationCompton back-scattered radiation in the moving mirror frameDoppler effect in the laboratory frameTUNABILITY

  • Due to the finite duration the radiation is not monochromatic but contains a frequency spectrum which is obtained by Fourier transformation of a truncated plane wave

  • Spectral IntensityLine width

  • Conditions for SASE

  • SASE Saturation ResultsSince September 2000:3 SASE FELs demonstrate saturation

  • TTF FELLEUTL

    LCLS [email protected]

    Linac Coherent Light Source

    Project DescriptionInjector

    LCLS [email protected]

    Estimated Cost, Revised Schedule$200M-$240M Total Estimated Cost range$245M-$295M Total Project Cost rangeFY2005Long-lead purchases for injector, undulatorFY2006 Construction beginsJanuary 2008 FEL Commissioning beginsSeptember 2008 Construction complete

    CD-1CD-2aCD-2bCD-3aCD-3bCD-0Title IDesignCompleteXFELCommissioningCD-4

    LCLS [email protected]

    CapabilitiesSpectral coverage: 0.15-1.5 nmPeak Brightness: 1033Average Brightness: 3 x 1022Pulse duration:

  • Conditions for SASE

  • Photo-Injector Beam dynamics R&D challenges for future X-ray sourcesThree Major Tasks to accomplish:Minimize all mechanisms leading to degradation of the rms normalized transverse emittance en Peak current enhancement by a factor 20-100 Damp the beam energy spread below the threshold Dg/g < r

  • S orgenteP ulsataA uto-amplificataR adiazioneC oerente

    Self-Amplified Pulsed Coherent Radiation@ LNF

  • SPARC project

    R&D program towards:

    - high brightness 150 MeV electron beam, - a SASE-FEL experiment- Ultrashort X-ray generation- X-ray optics & diagnostics

  • Under INFN responsibility

    SPARC 3D CAD modelUnder ENEAresponsibility

  • SPARCBrightness State of the ArtPITZATF SUMITOMO

  • Innovative Concepts / Components to reach max. brightness Use of Shaped Laser Pulses (minimize space charge non-linearities)Implementation of new optimized lay-out for an integrated photo-injector (proper phase tuning of emittance oscillations for max. brightness)Produce RF bunch compression with Emittance Preservation (increasing peak current at no expense of transverse emittance)

  • Emittance measurementsfor gaussian and square laser pulse shapesCourtesy of F. SakaiAchieving Record Emittances @ Sumitomo SHI + FESTA

  • LLaser Pulse Shaping TechniquesCollinear Acousto-Optic modulator (AOM)zTeO2DAZZLERLiquid Crystal Phase Mask

  • LINAC Working Point - Emittance

  • Slice analysis through the bunch

  • RF Deflector: principle of operation

  • Slice selection @ SPARC using a slit and RF Deflector, with and without clippingSPARC Review - Sept. 23rd 2003Bunch headBunch tailZ(m)300 mmCoupling of time-transverse coordinate with 1:1 c.c.

  • Brightness is crucial for many ApplicationsSASE FELsPlasma AcceleratorsRelativistic Thomson Monochromatic X-Ray SourcesCourtesy of D. Umstadter, Univ. of Michigan

  • Collaborations and UE programs SPARCDESYBNLUCLASLACUEMOUMOUUEEUROFELPITZMOU

  • FERMIA VUV - FEL user facility at 40-100 nm

    SPARXAn R&D program for a X-ray FEL test facility Next steps in Italy: (only half of the original budget available from the Research Ministry to support two programs)

  • SPARX- test facility

    upgrade the DAFNE Linac to drive a 5-10 nm SASE-FELand with seeding

    Beam energy : 1.2 - 1.5 GeV

    upgrade the injector to a RF photo-injector (SPARC-like)

    Study group will preparea proposal within 2005

  • SPARC Injector + DAFNE LinacSPARX-inoa 5-10 nm SASE FEL source at LNFRFgunLinac 1IVPCE= .44 GeVE= .145 GeVf= -25Linac 2sz~ 210 mmsz~ 5080 mmsd < 1 E-3E= 1.25 GeVR56= 34 mm

  • Low Energy section

  • High energy sectiondogleg start

  • Time to conclude

    FELs are opening new scenarios in many branches of scienceNo FELs possible without the skills of the accelerator physicistsNo FEL useful without a robust R&D in innovative instrumentationExciting possibilities to be investigated also in fundamental science