Abstract

The dream of physico-chemists to control molecular reactions with light beyond electronic excitations pushes the development of laser pulse shaping capabilities in the mid-infrared (MIR) spectral range. Here, we present a compact optical parametric amplifier platform for the generation and shaping of MIR laser pulses in the wavelength range between 8 μm and 15 μm. Opportunities for judiciously tailoring the electromagnetic waveform are investigated, demonstrating light field control with a spectral resolution of 59 GHz at a total spectral bandwidth of 5 THz. In experiments focusing on spectral amplitude manipulation these parameters result in a time window of 1.8 ps available for shaping the temporal pulse envelope and a phase modulation resolution of 100 mrad for several picosecond delays.

Highlights

  • Microscopic understanding of chemical dynamics on a molecular level is of fundamental importance in many science disciplines

  • The dream of physico-chemists to control molecular reactions with light beyond electronic excitations pushes the development of laser pulse shaping capabilities in the midinfrared (MIR) spectral range

  • Molecular function manifests itself in time-dependent changes of geometric structure, i. e. bond distances and bond angles describing the molecular dynamics of the system

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Summary

Introduction

Microscopic understanding of chemical dynamics on a molecular level is of fundamental importance in many science disciplines. Ultrashort deliberately shaped mid-infrared (MIR) laser pulses are suitable for a systematic investigation of these reactions, because they provide three key properties [6, 8] Their interaction takes place on the immanent time scales of molecular dynamics. Thereby a vibrational mode can be excited in a step-wise fashion, in which the laser pulse provides always a matching quantum of the energy needed to excite the higher vibrational level in the anharmonic potential This approach of vibrational ladder climbing populates high lying vibrational states creating non-thermal vibrational ensembles [9, 10]. We demonstrate AOM-technique with its advantages of spectral amplitude and phase shaping and with very high spectral resolution by using an acousto-optic modulator (AOM) mask in a 4 f configuration to wavelengths beyond 10 μm In the following it will be discussed, what capabilities are at hand to stretch and manipulate laser pulses.

Adjustable 8–15 μm OPA design
The AOM MIR pulse shaper
Shaping window and pulse trains
Spectral resolution and pulse separation
CEP modulation of subsequent pulses
Conclusion
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