| Literature DB >> 28582620 |
Maurice Tia1, Martin Pitzer1,2, Gregor Kastirke1, Janine Gatzke1, Hong-Keun Kim1, Florian Trinter1, Jonas Rist1, Alexander Hartung1, Daniel Trabert1, Juliane Siebert1, Kevin Henrichs1, Jasper Becht1, Stefan Zeller1, Helena Gassert1, Florian Wiegandt1, Robert Wallauer1, Andreas Kuhlins1, Carl Schober1, Tobias Bauer1, Natascha Wechselberger1, Phillip Burzynski1, Jonathan Neff1, Miriam Weller1, Daniel Metz1, Max Kircher1, Markus Waitz1, Joshua B Williams1,3, Lothar Ph H Schmidt1, Anne D Müller2, André Knie2, Andreas Hans2, Ltaief Ben Ltaief2, Arno Ehresmann2, Robert Berger4, Hironobu Fukuzawa5, Kiyoshi Ueda5, Horst Schmidt-Böcking1, Reinhard Dörner1, Till Jahnke1, Philipp V Demekhin2, Markus Schöffler1.
Abstract
Most large molecules are chiral in their structure: they exist as two enantiomers, which are mirror images of each other. Whereas the rovibronic sublevels of two enantiomers are almost identical (neglecting a minuscular effect of the weak interaction), it turns out that the photoelectric effect is sensitive to the absolute configuration of the ionized enantiomer. Indeed, photoionization of randomly oriented enantiomers by left or right circularly polarized light results in a slightly different electron flux parallel or antiparallel with respect to the photon propagation direction-an effect termed photoelectron circular dichroism (PECD). Our comprehensive study demonstrates that the origin of PECD can be found in the molecular frame electron emission pattern connecting PECD to other fundamental photophysical effects such as the circular dichroism in angular distributions (CDAD). Accordingly, distinct spatial orientations of a chiral molecule enhance the PECD by a factor of about 10.Entities:
Year: 2017 PMID: 28582620 DOI: 10.1021/acs.jpclett.7b01000
Source DB: PubMed Journal: J Phys Chem Lett ISSN: 1948-7185 Impact factor: 6.475