Attosecond Spectroscopy of Gases

Actively-stabilized attosecond beamline

We have built a compact and versatile beamline for attosecond spectroscopy. The setup consists of a gas cell for high-harmonic generation followed by a delay line that spatially separates and then recombines the extreme-ultraviolet (XUV) and residual infrared (IR) pulses. The beamline introduces a controlled and actively-stabilized delay between the XUV and IR pulses on the attosecond timescale. A new active-stabilization scheme combining a helium-neon-laser and a white-light interferometer minimizes fluctuations and allows to control delays accurately (26 as rms for 1.5 h) over long timescales. The high-order harmonic-generation region is imaged via optical systems, independently for XUV and IR, into an interaction volume to perform pump-probe experiments. As a consequence of the spatial separation, the pulses can be independently manipulated in intensity, polarization and frequency content. The beamline can be combined with a variety of detectors for measuring attosecond dynamics in gases and liquids.

Enlarged view: Attosecond Spectroscopy Setup
Figure 1. Setup for attosecond spectroscopy measurements.

Attosecond delays in molecular photoionization

We report measurements of energy-dependent photoionization delays between the two outermost valence shells of N2O and H2O. The combination of single-shot signal referencing with the use of different metal foils to filter the attosecond pulse train enables us to extract delays from congested spectra.
Remarkably large delays up to 160 as are observed in N2O, whereas the delays in H2O are all smaller than 50 as in the photon-energy range of 20–40 eV. These results are interpreted by developing a theory of molecular photoionization delays. The long delays measured in N2O are shown to reflect the population of molecular shape resonances that trap the photoelectron for a duration of up to ∼110 as. The unstructured
continua of H2O result in much smaller delays at the same photon energies. Our experimental and theoretical methods make the study of molecular attosecond photoionization dynamics accessible.

Enlarged view: huppert16afig1
Figure 2: (a) Photoelectron spectrum of N2O generated by an attosecond pulse train transmitted through a Sn filter (black line) and in the presence of the dressing IR field (orange line). Difference spectra, obtained by subtracting XUV only from XUV+IR photoelectron spectra and vice versa, are shown in red and blue, respectively. (b) Difference spectrum as a function of the IR-XUV delay.

Publications:
[2]    M. Huppert, I. Jordan, D. Baykusheva, A. von Conta, H. J. Wörner
DownloadAttosecond delays in molecular photoionization (PDF, 585 KB)
Phys. Rev. Lett. 117, 093001 (2016)
doi: Download10.1103/PhysRevLett.117.093001

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