Welcome to the research group on clusters and nanostructures!

Josef Tiggesbäumker and Karl-Heinz Meiwes Broer

Our main field of research is the investigation of clusters, i.e. of particles as small as only a few nanometers, or even less. Such small particles are benchmark systems for nanostructured materials and offer the unique chance to explore the development of many-body phenomena in finite quantum systems. We study the properties of free atomic clusters and complexes embedded in ultracold helium droplets, with a special focus on the interaction between light and matter, ranging from electron emission up to ultrafast nonlinear dynamics in nanoplasmas. Read more...

Recent Topics

Auger emission from the Coulomb explosion of helium nanoplasmas

The long-time correlated decay dynamics of strong-field exposed helium nanodroplets is studied by means of photoelectron spectroscopy. As a result of the adiabatic expansion of the laser-produced, fully inner-ionized nanoplasma, delocalized electrons in the deep confining mean field potential are shifted towards the vacuum level. Meanwhile, part of the electrons localize in bound levels of the helium ions. The simple hydrogenlike electronic structure of He+ results in clear signatures in the experimentally observed photoelectron spectra, which can be traced back to bound-free and bound-bound transitions. Auger electron emission takes place as a result of the transfer of transition energy to weakly bound electrons in the quasifree electron band. Hence, the spatial and temporal development of the nanoplasma cloud is encoded in the experimental spectra, whereas the electronic properties of He+ help resolve the different contributions.

Kelbg et al. J. Chem. Phys. 150, 204302 (2019)

 

Highly charged Rydberg ions from the Coulomb explosion of clusters

Ion emission from a nanoplasma produced in the interaction of intense optical laser pulses with argon clusters is studied resolving simultaneously charge states and recoil energies. By applying appropriate static electric fields we observe that a significant fraction of the ions Arq+ ( q = 1 − 7 ) have electrons with binding energies lower than 150 meV, i.e. nRyd ≥ 15 levels are populated. Charge state changes observed on a μs time scale can be attributed to electron emission due to autoionizing Rydberg states, indicating that high- ℓ Rydberg levels are populated as well. The experiments support theoretical predictions that a significant fraction of delocalized electrons, which are bound with hundreds of eV to the nanoplasma after the laser exposure, fill up meV bound ion states in the adiabatic expansion. We expect the process to be relevant for the long-term evolution of expanding laser-induced dense plasmas in general.

D. Komar et al., Phys. Rev. Lett. 120, 133207 (2018)

Nanoplasmonic electron acceleration by attosecond-controlled forward rescattering in silver clusters

In the strong-field photoemission from atoms, molecules, and surfaces, the fastest electrons emerge from tunneling and subsequent field-driven recollision, followed by elastic backscattering. This rescattering picture is central to attosecond science and enables control of the electron’s trajectory via the sub-cycle evolution of the laser electric field. Here we reveal a so far unexplored route for waveform-controlled electron acceleration emerging from forward rescattering in resonant plasmonic systems. We studied plasmon-enhanced photoemission from silver clusters and found that the directional acceleration can be controlled up to high kinetic energy with the relative phase of a two-color laser field. Our analysis reveals that the cluster’s plasmonic near-field establishes a sub-cycle directional gate that enables the selective acceleration. The identified generic mechanism offers robust attosecond control of the electron acceleration at plasmonic nanostructures, opening perspectives for laser-based sources of attosecond electron pulses.

J. Passig et al., Nature Commun. 8, 1181 (2017)