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Abstract
Short-wavelength free-electron lasers with their ultrashort pulses at high intensities have originated new approaches for tracking molecular dynamics from the vista of specific sites. X-ray pump X-ray probe schemes even allow to address individual atomic constituents with a ‘trigger’-event that preludes the subsequent molecular dynamics while being able to selectively probe the evolving structure with a time-delayed second X-ray pulse. Here, we use a linearly polarized X-ray photon to trigger the photolysis of a prototypical chiral molecule, namely trifluoromethyloxirane (C3H3F3O), at the fluorine K-edge at around 700 eV. The created fluorine-containing fragments are then probed by a second, circularly polarized X-ray pulse of higher photon energy in order to investigate the chemically shifted inner-shell electrons of the ionic mother-fragment for their stereochemical sensitivity. We experimentally demonstrate and theoretically support how two-color X-ray pump X-ray probe experiments with polarization control enable XFELs as tools for chiral recognition.
Ultrashort circularly polarised light pulses from free-electron lasers offer a route for exploring chiral molecules and their dynamics, but remain challenging to harness. Here, X-ray pump-probe experiments enable a site-specific photoelectron circular dichroism measurement on a dissociating chiral molecule.
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1 Universität Kassel, Institut für Physik und CINSaT, Kassel, Germany (GRID:grid.5155.4) (ISNI:0000 0001 1089 1036); European XFEL GmbH, Schenefeld, Germany (GRID:grid.434729.f) (ISNI:0000 0004 0590 2900); Stanford PULSE Institute, Menlo Park, USA (GRID:grid.434729.f)
2 Universität Kassel, Institut für Physik und CINSaT, Kassel, Germany (GRID:grid.5155.4) (ISNI:0000 0001 1089 1036); European XFEL GmbH, Schenefeld, Germany (GRID:grid.434729.f) (ISNI:0000 0004 0590 2900)
3 Universität Kassel, Institut für Physik und CINSaT, Kassel, Germany (GRID:grid.5155.4) (ISNI:0000 0001 1089 1036); Southern Federal University, Institute of Physics, Rostov-on-Don, Russia (GRID:grid.182798.d) (ISNI:0000 0001 2172 8170)
4 Universität Kassel, Institut für Physik und CINSaT, Kassel, Germany (GRID:grid.5155.4) (ISNI:0000 0001 1089 1036); Helmholtz-Zentrum Berlin für Materialien und Energie, Berlin, Germany (GRID:grid.424048.e) (ISNI:0000 0001 1090 3682)
5 Max-Planck-Institut für Kernphysik Heidelberg, Heidelberg, Germany (GRID:grid.419604.e) (ISNI:0000 0001 2288 6103)
6 SLAC National Accelerator Laboratory, Menlo Park, USA (GRID:grid.445003.6) (ISNI:0000 0001 0725 7771)
7 Universität Kassel, Institut für Physik und CINSaT, Kassel, Germany (GRID:grid.5155.4) (ISNI:0000 0001 1089 1036)
8 European XFEL GmbH, Schenefeld, Germany (GRID:grid.434729.f) (ISNI:0000 0004 0590 2900)
9 Technische Universität Dortmund, Fakultät für Physik, Dortmund, Germany (GRID:grid.5675.1) (ISNI:0000 0001 0416 9637)
10 Center for Free-Electron Laser Science CFEL, Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany (GRID:grid.7683.a) (ISNI:0000 0004 0492 0453)
11 Stanford PULSE Institute, Menlo Park, USA (GRID:grid.445003.6); SLAC National Accelerator Laboratory, Menlo Park, USA (GRID:grid.445003.6) (ISNI:0000 0001 0725 7771)
12 Center for Free-Electron Laser Science CFEL, Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany (GRID:grid.7683.a) (ISNI:0000 0004 0492 0453); Peking University, State Key Laboratory for Mesoscopic Physics, School of Physics, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)