Zoltan Harman

Enhanced One-Color-Two-Photon Resonant Ionization in Highly Charged Ions by Fine-Structure Effects

Moto Togawa [1,2], Chunhai Lyu [2], Chintan Shah [3,2,4], Marc Botz [2,5], Joschka Goes [2], Jonas Danisch [2], Marleen Maxton [2], Kai Köbnick, Filipe Grilo [6], Pedro Amaro [6], Katharina Kubicek [1,7], Mohammed Sekkal [1,7], Awad Mohamed [8], Rebecca Boll [1], Alberto De Fanis [1], Simon Dold [1], Tommaso Mazza [1], Jacobo Montano [1], Nils Rennhack [1], Björn Senfftleben, Sergey Usenko [1], Zoltan Harman [2], Christoph H. Keitel [2], Maurice Leutenegger [3], Michael Meyer [1], Thomas Pfeifer [2], José R. Crespo López-Urrutia, Thomas M. Baumann [1]

Abstract

Ultraintense pulses from X-ray free-electron lasers can drive, within femtoseconds, multiple processes in the inner shells of atoms and molecules in all phases of matter. The ensuing complex ionization pathways of outer-shell electrons from the neutral to the final highly charged states make a comparison with theory enormously difficult. We resolve these pathways by preparing highly charged ions in an electron beam ion trap before exposing them to the pulsed radiation. This reveals how relativistic fine-structure effects shift electronic energies, largely compensate the core-screening potential, and enable the consecutive, resonant absorption of two quasi-monochromatic X-ray photons that would generally be unfeasible. This doubly-resonant channel enhances the efficiency of two-photon ionization by more than two orders of magnitude, dominating in this regime the nonlinear interaction of light and matter with possible application for future precision X-ray metrology.

Detection of metastable electronic states by Penning trap mass spectrometry

Rima Xenia Schüssler, Hendrik Bekker, Martin Braß, Halil Cakir, José R. Crespo López-Urrutia, Menno Door, Pavel Filianin, Zoltan Harman, Maurits W. Haverkort, Wen Jia Huang, Paul Indelicato, Christoph Helmut Keitel, Charlotte Maria König, Kathrin Kromer, Marius Müller, Yuri N. Novikov, Alexander Rischka, Christoph Schweiger, Sven Sturm, Stefan Ulmer, Ssergey Eliseev, Klaus Blaum

Abstract

State-of-the-art optical clocks achieve fractional precisions of $10^{-18}$ and below using ensembles of atoms in optical lattices or individual ions in radio-frequency traps. Promising candidates for novel clocks are highly charged ions (HCIs) and nuclear transitions, which are largely insensitive to external perturbations and reach wavelengths beyond the optical range, now becoming accessible to frequency combs. However, insufficiently accurate atomic structure calculations still hinder the identification of suitable transitions in HCIs. Here, we report on the discovery of a long-lived metastable electronic state in a HCI by measuring the mass difference of the ground and the excited state in Re, the first non-destructive, direct determination of an electronic excitation energy. This result agrees with our advanced calculations, and we confirmed them with an Os ion with the same electronic configuration. We used the high-precision Penning-trap mass spectrometer PENTATRAP, unique in its synchronous use of five individual traps for simultaneous mass measurements. The cyclotron frequency ratio $R$ of the ion in the ground state to the metastable state could be determined to a precision of $δR=1\cdot 10^{-11}$, unprecedented in the heavy atom regime. With a lifetime of about 130 days, the potential soft x-ray frequency reference at $ν=4.86\cdot 10^{16}\,\text{Hz}$ has a linewidth of only $Δν\approx 5\cdot 10^{-8}\,\text{Hz}$, and one of the highest electronic quality factor ($Q=\fracν{Δν}\approx 10^{24}$) ever seen in an experiment. Our low uncertainty enables searching for more HCI soft x-ray clock transitions, needed for promising precision studies of fundamental physics in a thus far unexplored frontier.