• High Power Laser Science and Engineering
  • Vol. 6, Issue 4, 04000e65 (2018)
Paul Mason1, Saumyabrata Banerjee1, Jodie Smith1, Thomas Butcher1, Jonathan Phillips1, Hauke Höppner2, Dominik Möller2, Klaus Ertel1, Mariastefania De Vido1, Ian Hollingham1, Andrew Norton1, Stephanie Tomlinson1, Tinesimba Zata1, Jorge Suarez Merchan1, Chris Hooker1, Mike Tyldesley1, Toma Toncian2, Cristina Hernandez-Gomez1, Chris Edwards1, and John Collier1
Author Affiliations
  • 1Central Laser Facility , STFC Rutherford Appleton Laboratory , Didcot , OX11 0QX , UK
  • 2Institute for Radiation Physics , Helmholtz-Zentrum Dresden-Rossendorf e.V. , D-01328 Dresden , Germany
  • show less
    DOI: 10.1017/hpl.2018.56 Cite this Article Set citation alerts
    Paul Mason, Saumyabrata Banerjee, Jodie Smith, Thomas Butcher, Jonathan Phillips, Hauke Höppner, Dominik Möller, Klaus Ertel, Mariastefania De Vido, Ian Hollingham, Andrew Norton, Stephanie Tomlinson, Tinesimba Zata, Jorge Suarez Merchan, Chris Hooker, Mike Tyldesley, Toma Toncian, Cristina Hernandez-Gomez, Chris Edwards, John Collier. Development of a 100 J, 10 Hz laser for compression experiments at the High Energy Density instrument at the European XFEL[J]. High Power Laser Science and Engineering, 2018, 6(4): 04000e65 Copy Citation Text show less
    Schematic of DiPOLE100X amplifier chain, showing typical output energy at each amplifier stage: YDFO Yb–silica fibre oscillator; YDFA Yb–silica fibre amplifier (inc. temporal pulse shaping); PA room-temperature preamplifier (1 Yb:CaF2regenerative, 2 Yb:YAG multi-pass); MA main cryogenic amplifier (ceramic Yb:YAG multi-slab).
    Fig. 1. Schematic of DiPOLE100X amplifier chain, showing typical output energy at each amplifier stage: YDFO  Yb–silica fibre oscillator; YDFA  Yb–silica fibre amplifier (inc. temporal pulse shaping); PA  room-temperature preamplifier (1  Yb:CaF 2 regenerative, 2  Yb:YAG multi-pass); MA  main cryogenic amplifier (ceramic Yb:YAG multi-slab).
    3D model of DiPOLE100X: FFE fibre front end, DP diode pumps, cGC cryogenic gas coolers, DM deformable mirrors, BD beam diverter, FFE fibre front end (not shown).
    Fig. 2. 3D model of DiPOLE100X: FFE  fibre front end, DP  diode pumps, cGC  cryogenic gas coolers, DM  deformable mirrors, BD  beam diverter, FFE  fibre front end (not shown).
    Schematic layout of the front end for DiPOLE100X.
    Fig. 3. Schematic layout of the front end for DiPOLE100X.
    X-ray pulse timing diagram for SASE II beamline.
    Fig. 4. X-ray pulse timing diagram for SASE II beamline.
    DiPOLE100X timing diagram.
    Fig. 5. DiPOLE100X timing diagram.
    Schematic showing 7-pass angularly multiplexed extraction architecture of the 10 J cryo-preamplifier. DP diode pumps, DM1 10 J deformable mirror, BS beam splitters.
    Fig. 6. Schematic showing 7-pass angularly multiplexed extraction architecture of the 10 J cryo-preamplifier. DP  diode pumps, DM1  10 J deformable mirror, BS  beam splitters.
    (a) Photograph of the DiPOLE100X 10 J bimorph deformable mirror, built at the CLF, with inset showing schematic of electrode pattern, (b) corrected output wave front and (c) far-field CCD camera image measured at 10 J, 10 Hz on the DiPOLE prototype amplifier.
    Fig. 7. (a) Photograph of the DiPOLE100X 10 J bimorph deformable mirror, built at the CLF, with inset showing schematic of electrode pattern, (b) corrected output wave front and (c) far-field CCD camera image measured at 10 J, 10 Hz on the DiPOLE prototype amplifier.
    Energy stability over half an hour with inset showing measured temporal pulse shape for amplification of 2.2 ns pulses at 8 J, 10 Hz.
    Fig. 8. Energy stability over half an hour with inset showing measured temporal pulse shape for amplification of 2.2 ns pulses at 8 J, 10 Hz.
    Schematic showing 4-pass, off-axis, angularly multiplexed extraction architecture of the 100 J cryo-amplifier. DP diode pumps, DM2 100 J deformable mirror, BD beam diverter.
    Fig. 9. Schematic showing 4-pass, off-axis, angularly multiplexed extraction architecture of the 100 J cryo-amplifier. DP  diode pumps, DM2  100 J deformable mirror, BD  beam diverter.
    (a) Photograph of new 100 J deformable mirror, (b) target aberrated wave front and (c) residual error in generated wave front.
    Fig. 10. (a) Photograph of new 100 J deformable mirror, (b) target aberrated wave front and (c) residual error in generated wave front.
    Synoptic screen for control and monitoring of 10 J cryo-preamplifier. Red lines correspond to the main 1030 nm laser beam path, input from the FE (left) and output to the beam transport section (right); blue lines represent diagnostic beam paths; and orange lines correspond to 940 nm pump diode beam paths.
    Fig. 11. Synoptic screen for control and monitoring of 10 J cryo-preamplifier. Red lines correspond to the main 1030 nm laser beam path, input from the FE (left) and output to the beam transport section (right); blue lines represent diagnostic beam paths; and orange lines correspond to 940 nm pump diode beam paths.
    Temporal pulse shaping results at 6.5 J, 10 Hz obtained using the DiPOLE prototype amplifier (a) flat-top and (b) multi-step pyramid pulse profiles.
    Fig. 12. Temporal pulse shaping results at 6.5 J, 10 Hz obtained using the DiPOLE prototype amplifier (a) flat-top and (b) multi-step pyramid pulse profiles.
    Time lapse photographs of DiPOLE100X build with 3D CAD view of completed system.
    Fig. 13. Time lapse photographs of DiPOLE100X build with 3D CAD view of completed system.
    Schematic showing the main components of the HED instrument.
    Fig. 14. Schematic showing the main components of the HED instrument.
    Layout of DiPOLE100X in laser hutch at the HED instrument.
    Fig. 15. Layout of DiPOLE100X in laser hutch at the HED instrument.
    ParameterTargetDemonstrated
    Wavelength nm1029.5 nm
    Pulse energy100 J107 J
    Energy stability 2.5% RMS 1% RMS
    Pulse rateSingle shot, 1, 2, 5 or 10 Hz1 & 10 Hz
    Jitter 25 ps RMS
    Pulse duration2 to 15 ns10 ns
    Pulse shapeUser selectableFlat top
    Beam size & shape75 mm square, ,
    super-Gaussiansuper-Gaussian ( )
    Beam quality1.7 DL ( )
    2.3 DL ( )
    Pointing stabilityWithin radWithin rad
    (shot to shot) 4% RMS1% RMS
    Table 1. Target parameters for DiPOLE100X and demonstrated performance
    Control screenFunctions
    OverviewsAccess to summary/overview screens for each of the main sub-systems (FE, 10 J, 100 J) and the beam transport section.
    SynopticsReal-time, interactive visual displays of the status of the main sub-systems (FE, 10 J, 100 J) and their individual components. Synoptic screens use a traffic light system to indicate the status of each individual component, with green indicating that all is okay, amber indicating a component requires attention, and red indicating that either the component is off or that there is an error that requires action. Control screens can be accessed directly by touching the component symbol on-screen, minimizing the number of actions needed to view and adjust settings. An example synoptic display for the 10 J cryo-preamplifier is shown in Figure  11 .
    AutomationUseful information related to beam steering and machine safety.
    AlignmentOverview of the current status of the automatic beam alignment system at various points within the system based on data from relevant near- and far-field diagnostic cameras. Again a traffic light system is used to indicate alignment status.
    InterlockStatus of system interlocks.
    HazardsImportant information on the status of all laser hazards. This screen can also be displayed on a remote monitor, sited outside the laser laboratory, to show whether it is safe to enter the area.
    Table 2. Functionality of user control screens in DiPOLE100X control system
    Paul Mason, Saumyabrata Banerjee, Jodie Smith, Thomas Butcher, Jonathan Phillips, Hauke Höppner, Dominik Möller, Klaus Ertel, Mariastefania De Vido, Ian Hollingham, Andrew Norton, Stephanie Tomlinson, Tinesimba Zata, Jorge Suarez Merchan, Chris Hooker, Mike Tyldesley, Toma Toncian, Cristina Hernandez-Gomez, Chris Edwards, John Collier. Development of a 100 J, 10 Hz laser for compression experiments at the High Energy Density instrument at the European XFEL[J]. High Power Laser Science and Engineering, 2018, 6(4): 04000e65
    Download Citation