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X-ray free-electron laser based dark-field X-ray microscopy - a simulation-based study

MetadataDetails
Publication Date2022-01-19
JournalJournal of Applied Crystallography
AuthorsTheodor S. Holstad, Trygve Magnus Réder, Mads Carlsen, Erik Knudsen, Leora E. Dresselhaus‐Marais
InstitutionsSLAC National Accelerator Laboratory, Stanford University
Citations12
AnalysisFull AI Review Included

This study demonstrates the numerical feasibility of implementing Dark-Field X-ray Microscopy (DFXM) using an X-ray Free-Electron Laser (XFEL) source combined with a pump-probe scheme.

  • Time Resolution Breakthrough: The proposed method extends DFXM time resolution from milliseconds (synchrotron) to the femtosecond regime, achieving up to nine orders of magnitude improvement for studying ultrafast dynamics.
  • Target Phenomenon: The simulations successfully visualize the propagation of laser-generated longitudinal strain waves (phonons) in a bulk diamond single crystal.
  • Key Achievement: Single-pulse DFXM imaging of the strain wave is shown to be feasible, yielding clear contrast and a good signal-to-noise ratio, with a maximum strain amplitude of 4 x 10-4.
  • Simulation Basis: The study uses the specifications of the XCS instrument at the Linac Coherent Light Source (LCLS), combining thermo-mechanical modeling (udkm1Dsim) with DFXM forward simulations (geometrical and wave optics).
  • Spatial Resolution: The technique maintains high spatial resolution (down to 30-100 nm) while probing deeply embedded structures (millimeter scale).
  • Future Impact: This approach opens the door to investigating critical ultrafast phenomena, including strain-defect interactions, rapid material failure, and diffusionless phase transitions in bulk crystalline materials.

The following parameters were used for the XFEL-based DFXM simulations, based on the LCLS XCS instrument setup:

ParameterValueUnitContext
X-ray Photon Energy10keVXFEL Probe Beam
XFEL Pulse Duration35fsTime resolution limit
XFEL Pulse Energy2mJTotal energy per pulse
Estimated Incident Photons2 x 1010photons/pulseIncident on sample (after optics)
X-ray Horizontal Thickness (Ax)3”mLine beam focus FWHM
X-ray Vertical Width (Ay)500”mLine beam height
Optical Laser Pulse Duration100fsPump Pulse
Optical Laser Fluence0.8J/cm2Heating the Au film
Diamond Crystal Size0.6 x 1 x 2mmSimulated dimensions
Au Film Thickness600nmThermal expansion layer
Maximum Simulated Strain (epsilon)4 x 10-4(unitless)Longitudinal strain wave amplitude
Objective TypeCompound Refractive Lens (CRL)N/A30 Be lenslets
Objective Magnification (M)27.9(unitless)X-ray Objective
Effective Numerical Aperture (NA)0.000845(unitless)Objective FWHM
Detector Pixel Size (Effective)466 x 664nmIn the object plane (2x binned)
Diamond Thermal Conductivity (kl)1200W/mKAt 300 K

The simulation process involved a multi-step approach combining thermo-mechanical modeling with two distinct DFXM forward simulation formalisms:

  1. Strain Wave Generation (Pump):

    • A 100 fs optical laser pulse was directed onto a 600 nm Au film deposited on a diamond crystal facet.
    • The resulting impulsive heating and thermal expansion of the Au film launched a longitudinal strain wave into the diamond.
  2. Thermo-mechanical Modeling:

    • The 1D Python package udkm1Dsim was used, employing the Two-Temperature Model (electrons and lattice treated separately) to compute temperature profiles and subsequent thermal expansion.
    • A linear chain of point masses connected by springs was used to compute the resulting crystal lattice dynamics and the strain wave profile (maximum strain ~4 x 10-4).
  3. DFXM Forward Simulation (Geometrical Optics):

    • This formalism was used for rapid optimization and parameter space exploration.
    • It relies on analytical expressions relating the displacement gradient tensor field (strain) to the resulting detector intensity distribution.
    • The instrumental resolution function was determined via Monte Carlo ray tracing, revealing significant anisotropy in reciprocal space resolution.
  4. DFXM Forward Simulation (Wave Optics):

    • The Takagi-Taupin formalism was used to model the coherent X-ray wavefront propagation and scattering, accounting for dynamical diffraction effects (e.g., multiple scattering and Pendellösung fringes).
    • This method was used to verify results under ‘strong-beam’ conditions where geometrical optics are less reliable.
  5. Contrast Optimization:

    • The optimal visualization was achieved using rocking-type weak-beam contrast.
    • The sample was rotated (rocked) by an angular offset (Delta-phi = 0.00974°) relative to the Bragg condition, causing the unstrained bulk crystal to diffract negligibly.
    • The highly strained regions of the propagating wave were then brought closer to the Bragg condition, maximizing the contrast of the wave structure against a dark background.

The ability to image ultrafast strain dynamics in bulk crystalline materials, particularly diamond, has direct relevance across several high-technology sectors:

  • Advanced Semiconductor Manufacturing: Studying phonon transport and thermalization in wide-bandgap materials (like diamond and GaN) critical for high-power electronics and thermal management systems.
  • Quantum Sensing and Computing: Mapping and controlling local strain fields in diamond to optimize the performance and coherence of solid-state quantum defects (e.g., Nitrogen-Vacancy centers), which are highly sensitive to lattice strain.
  • Materials Reliability and Failure Analysis: Investigating the fundamental mechanisms of rapid material failure, crack propagation, and shock physics at the atomic level, relevant for aerospace and defense applications.
  • Structural Materials Engineering: Direct visualization of the interaction between strain waves and microstructural features (dislocations, twin walls, grain boundaries) to inform the design of materials with enhanced mechanical properties and toughness.
  • Diffusionless Phase Transformations: Enabling the study of ultrafast structural changes and phase transitions induced by mechanical or thermal shock, which occur on picosecond timescales.
View Original Abstract

Dark-field X-ray microscopy (DFXM) is a nondestructive full-field imaging technique providing three-dimensional mapping of microstructure and local strain fields in deeply embedded crystalline elements. This is achieved by placing an objective lens in the diffracted beam, giving a magnified projection image. So far, the method has been applied with a time resolution of milliseconds to hours. In this work, the feasibility of DFXM at the picosecond time scale using an X-ray free-electron laser source and a pump-probe scheme is considered. Thermomechanical strain-wave simulations are combined with geometrical optics and wavefront propagation optics to simulate DFXM images of phonon dynamics in a diamond single crystal. Using the specifications of the XCS instrument at the Linac Coherent Light Source as an example results in simulated DFXM images clearly showing the propagation of a strain wave.