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ParaTAXIS X-ray Scattering Input & Output

<p>This dataset describes the&nbsp;science case of the SIMEX platform tool chain for EUCALL WP4 Milestone M4.3.</p> <p>The file <em>opt_thick_1.6x1.6x3_micron_10fs_around_laser_max.h5</em> &nbsp;contains the ParaTAXIS density input data in openPMD format for the optically thick&nbsp;case (milestone 4.2.2.10). The data was obtained in a&nbsp;2D PICLS simulation (milestone 4.2.2.7) which modeled&nbsp;the temporal evolution of a silicon grating irradiated by a <span class="math-tex">\(\tau_\mathrm{FWHM} = 83\,\mathrm{fs},\ \lambda = 800\,\mathrm{nm}\)</span> laser pulse of normalized amplitude <span class="math-tex">\(a_0 = 0.25\)</span>. Here&nbsp;959 slices which correspond to subsequent PIC time steps of length <span class="math-tex">\(\Delta t_\mathrm{PIC} = 1.042 \cdot 10^{-17}\,\mathrm{s}\)</span> were stacked in propagation direction of the XFEL probe pulse thus taking time evolution of the target during X-ray pulse propagation into account.&nbsp; ParaTAXIS reads the density into&nbsp;a simulation volume of 1024 x 512 x 512 cells. The cell sizes of the PIC and the ParaTAXIS simulations are&nbsp;equally&nbsp;<span class="math-tex">\(3.125\,\mathrm{nm}\)</span> in every spatial direction. Density data is given in units of critical densities with respect to the <span class="math-tex">\(800\,\mathrm{nm}\)</span> laser. One critical density corresponds to&nbsp;<span class="math-tex">\(n_\mathrm{c} = 1.7422 \cdot 10^{27}\,\mathrm{m}^{-3}\)</span>. The time window&nbsp;chosen is situated from&nbsp;<span class="math-tex">\(5\,\mathrm{fs}\)</span>&nbsp;before until&nbsp;<span class="math-tex">\(5\,\mathrm{fs}\)</span>&nbsp;after the optical laser main pulse maximum hits the foil indicating a delay of <span class="math-tex">\(\Delta t = 0\)</span>. The optical laser incidence is in z-direction (ParaTAXIS coordinates) under 0&deg;.</p> <p>The total illuminated area for both the optically thick and thin cases was&nbsp;<span class="math-tex">\(1.6 \times 1.6\, \mathrm{\mu m}\)</span>. We assume&nbsp;a target thickness of&nbsp;<span class="math-tex">\(3\,\mathrm{\mu m}\)</span>. The detector distance was&nbsp;<span class="math-tex">\(d = 1.4\,\mathrm{m}\)</span>&nbsp;and the detector pixel size was&nbsp;<span class="math-tex">\(a_\mathrm{D} = 13.5\,\mathrm{\mu m}\)</span>. For Thomson scattering most photons are scattered in forward direction. We therefore assumed a maximum polar scattering angle of&nbsp;<span class="math-tex">\(0.01\,\mathrm{rad}\)</span> in order to increase statistics on the detector.</p> <p>Via 16 simulations we obtained the detector outputs in the optically thick case&nbsp;which can be found in&nbsp;opt_thick_run_&lt;run-number&gt;_detector_&lt;number-of-simulated-photons&gt;_photons.h5 in openPMD format.</p> <p>The file&nbsp;<em>opt_thin_integrated_1.6x1.6x3_micron_10fs_around_laser_max</em>&nbsp;contains the total electron density data for the optically thin&nbsp;case (milestone 4.2.2.9) integrated over 959 slices in the propagation direction of the probe laser beam. The&nbsp;density is only non-zero in the 6th cell of the simulation volume thus enforcing single-scattering in the ParaTAXIS simulation as can be assumed for an optically thin medium. This data was read by a&nbsp;ParaTAXIS into a simulation volume of 12 x 512 x 512 cells.</p> <p>We launched 10 parallel simulations, each arriving at detector images for <span class="math-tex">\(10^{12}\)</span>&nbsp;simulated photons. The detector output of these simulations can be found in&nbsp;<em>opt_thin_detector_1e12_photons_run&lt;run-number&gt;.h5</em>&nbsp;also in openPMD format.</p> <p>&nbsp;</p>

ShareScore

48/100

Overall dataset sharing score

Score breakdown

These five areas show where the dataset supports — or may limit — practical reuse.

Stewardship
8
Harmonization
8
Access
20
Reuse readiness
8
Engagement
4

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