C. Schober
Goethe University Frankfurt
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Featured researches published by C. Schober.
Physical Review Letters | 2013
F. Trinter; Joshua Williams; M. Weller; M. Waitz; M. Pitzer; J. Voigtsberger; C. Schober; Gregor Kastirke; C. Müller; C. Goihl; Phillip Burzynski; Florian Wiegandt; R. Wallauer; Anton Kalinin; L. Schmidt; M. Schöffler; Ying-Chih Chiang; Kirill Gokhberg; T. Jahnke; R. Dörner
We investigate the ionization of HeNe from below the He 1s3p excitation to the He ionization threshold. We observe HeNe+ ions with an enhancement by more than a factor of 60 when the He side couples resonantly to the radiation field. These ions are an experimental proof of a two-center resonant photoionization mechanism predicted by Najjari et al. [Phys. Rev. Lett. 105, 153002 (2010)]. Furthermore, our data provide electronic and vibrational state resolved decay widths of interatomic Coulombic decay in HeNe dimers. We find that the interatomic Coulombic decay lifetime strongly increases with increasing vibrational state.
Physical Review Letters | 2013
F. Trinter; Joshua Williams; M. Weller; M. Waitz; M. Pitzer; J. Voigtsberger; C. Schober; Gregor Kastirke; C. Müller; C. Goihl; Phillip Burzynski; Florian Wiegandt; Tobias Bauer; R. Wallauer; H. Sann; Anton Kalinin; L. Ph. H. Schmidt; M. Schöffler; Nicolas Sisourat; T. Jahnke
During the past 15 years a novel decay mechanism of excited atoms has been discovered and investigated. This so-called interatomic Coulombic decay (ICD) involves the chemical environment of the electronically excited atom: the excitation energy is transferred (in many cases over long distances) to a neighbor of the initially excited particle usually ionizing that neighbor. It turned out that ICD is a very common decay route in nature as it occurs across van der Waals and hydrogen bonds. The time evolution of ICD is predicted to be highly complex, as its efficiency strongly depends on the distance of the atoms involved and this distance typically changes during the decay. Here we present the first direct measurement of the temporal evolution of ICD using a novel experimental approach.
Proceedings of the National Academy of Sciences of the United States of America | 2016
S. Zeller; Maksim Kunitski; J. Voigtsberger; Anton Kalinin; Alexander Schottelius; C. Schober; M. Waitz; H. Sann; Alexander Hartung; Tobias Bauer; M. Pitzer; F. Trinter; C. Goihl; Christian Janke; Martin Richter; Gregor Kastirke; M. Weller; A. Czasch; Markus Kitzler; Markus Braune; R. E. Grisenti; Wieland Schöllkopf; L. Schmidt; M. Schöffler; J. B. Williams; T. Jahnke; R. Dörner
Significance In bound matter on all length scales, from nuclei to molecules to macroscopic solid objects, most of the density of the bound particles is within the range of the interaction potential which holds the system together. Quantum halos on the contrary are a type of matter where the particle density is mostly outside the range of the interaction potential in the tunneling region of the potential. Few examples of these fascinating systems are known in nuclear and molecular physics. The conceptually simplest halo system is made of only two particles. Here we experimentally image the wavefunction of the He2 quantum halo. It shows the predicted exponential shape of a tunneling wavefunction. Quantum tunneling is a ubiquitous phenomenon in nature and crucial for many technological applications. It allows quantum particles to reach regions in space which are energetically not accessible according to classical mechanics. In this “tunneling region,” the particle density is known to decay exponentially. This behavior is universal across all energy scales from nuclear physics to chemistry and solid state systems. Although typically only a small fraction of a particle wavefunction extends into the tunneling region, we present here an extreme quantum system: a gigantic molecule consisting of two helium atoms, with an 80% probability that its two nuclei will be found in this classical forbidden region. This circumstance allows us to directly image the exponentially decaying density of a tunneling particle, which we achieved for over two orders of magnitude. Imaging a tunneling particle shows one of the few features of our world that is truly universal: the probability to find one of the constituents of bound matter far away is never zero but decreases exponentially. The results were obtained by Coulomb explosion imaging using a free electron laser and furthermore yielded He2’s binding energy of 151.9±13.3 neV, which is in agreement with most recent calculations.
ChemPhysChem | 2016
M. Pitzer; Gregor Kastirke; Maksim Kunitski; Pd Till Jahnke; Tobias Bauer; C. Goihl; F. Trinter; C. Schober; Kevin Henrichs; Jasper Becht; S. Zeller; H. Gassert; M. Waitz; Andreas Kuhlins; H. Sann; F. Sturm; Florian Wiegandt; R. Wallauer; L. Schmidt; Allan S. Johnson; Manuel Mazenauer; Benjamin Spenger; Sabrina Marquardt; Sebastian Marquardt; H. Schmidt-Böcking; Jürgen Stohner; R. Dörner; M. Schöffler; Robert Berger
The absolute configuration of individual small molecules in the gas phase can be determined directly by light-induced Coulomb explosion imaging (CEI). Herein, this approach is demonstrated for ionization with a single X-ray photon from a synchrotron light source, leading to enhanced efficiency and faster fragmentation as compared to previous experiments with a femtosecond laser. In addition, it is shown that even incomplete fragmentation pathways of individual molecules from a racemic CHBrClF sample can give access to the absolute configuration in CEI. This leads to a significant increase of the applicability of the method as compared to the previously reported complete break-up into atomic ions and can pave the way for routine stereochemical analysis of larger chiral molecules by light-induced CEI.
Journal of Physical Chemistry Letters | 2017
Maurice Tia; M. Pitzer; Gregor Kastirke; Janine Gatzke; H.-K. Kim; F. Trinter; J. Rist; Alexander Hartung; Daniel Trabert; Juliane Siebert; Kevin Henrichs; Jasper Becht; S. Zeller; H. Gassert; Florian Wiegandt; R. Wallauer; Andreas Kuhlins; C. Schober; Tobias Bauer; Natascha Wechselberger; Phillip Burzynski; Jonathan Neff; M. Weller; D. Metz; Max Kircher; M. Waitz; Joshua Williams; L. Schmidt; Anne D. Müller; André Knie
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.
Nature Communications | 2017
M. Waitz; R. Y. Bello; D. Metz; J. Lower; F. Trinter; C. Schober; M. Keiling; U. Lenz; M. Pitzer; K. Mertens; M. Martins; Jens Viefhaus; S. Klumpp; Thorsten Weber; L. Ph. H. Schmidt; J. B. Williams; M. Schöffler; V. V. Serov; Anatoli Kheifets; Luca Argenti; A. Palacios; Fernando Martín; T. Jahnke; R. Dörner
The toolbox for imaging molecules is well-equipped today. Some techniques visualize the geometrical structure, others the electron density or electron orbitals. Molecules are many-body systems for which the correlation between the constituents is decisive and the spatial and the momentum distribution of one electron depends on those of the other electrons and the nuclei. Such correlations have escaped direct observation by imaging techniques so far. Here, we implement an imaging scheme which visualizes correlations between electrons by coincident detection of the reaction fragments after high energy photofragmentation. With this technique, we examine the H2 two-electron wave function in which electron–electron correlation beyond the mean-field level is prominent. We visualize the dependence of the wave function on the internuclear distance. High energy photoelectrons are shown to be a powerful tool for molecular imaging. Our study paves the way for future time resolved correlation imaging at FELs and laser based X-ray sources.Electron-electron correlation is a complex and interesting phenomenon that occurs in multi-electron systems. Here, the authors demonstrate the imaging of the correlated two-electron wave function in hydrogen molecule using the coincident detection of the electron and proton after the photoionization.
Physical Review A | 2014
Phillip Burzynski; F. Trinter; J. B. Williams; M. Weller; M. Waitz; M. Pitzer; J. Voigtsberger; C. Schober; Gregor Kastirke; C. Müller; C. Goihl; Florian Wiegandt; R. Wallauer; Anton Kalinin; L. Ph. H. Schmidt; M. Schöffler; G. Schiwietz; Nicolas Sisourat; T. Jahnke; R. Dörner
We investigate the onset of photoionization shake-up-induced interatomic Coulombic decay (ICD) in
Physical Review Letters | 2016
H. Sann; C. Schober; A. Mhamdi; F. Trinter; C. Müller; S. K. Semenov; M. Stener; M. Waitz; Tobias Bauer; R. Wallauer; C. Goihl; J. Titze; F. Afaneh; L. Ph. H. Schmidt; Maksim Kunitski; H. Schmidt-Böcking; Ph. V. Demekhin; N. A. Cherepkov; M. Schöffler; T. Jahnke; R. Dörner
{\mathrm{He}}_{2}
Nature Communications | 2018
M. Waitz; R. Y. Bello; D. Metz; J. Lower; F. Trinter; C. Schober; M. Keiling; U. Lenz; M. Pitzer; K. Mertens; M. Martins; Jens Viefhaus; S. Klumpp; Thorsten Weber; L. Ph. H. Schmidt; J. B. Williams; M. Schöffler; V. V. Serov; Anatoli Kheifets; Luca Argenti; A. Palacios; Fernando Martín; T. Jahnke; R. Dörner
at the
XXIX International Conference on Photonic, Electronic, and Atomic Collisions (ICPEAC2015), Toledo, 22 –28 July 2015 | 2015
M. Pitzer; Maksim Kunitski; Gregor Kastirke; T. Jahnke; Tobias Bauer; C. Goihl; F. Trinter; C. Schober; Kevin Henrichs; Jasper Becht; S. Zeller; H. Gassert; M. Waitz; Andreas Kuhlins; Florian Wiegandt; R. Wallauer; L. Ph. H. Schmidt; Manuel Mazenauer; Benjamin Spenger; Sabrina Marquardt; H. Schmidt-Böcking; Jürgen Stohner; R. Dörner; M. Schöffler; Robert Berger
{\mathrm{He}}^{+*}(n=2)