Munich-Centre for Advanced Photonics

Ultrawide-band light wave synthesis in the visible and ultraviolet

Fig. 1: Schematic of ultrawide-band optical waveform synthesis.

Few-cycle laser pulses tunable across the entire visible and ultraviolet spectral ranges have long been desired for site-selective triggering of molecular dynamics. Their coherent addition with adjustable delays would, on the opther hand, provide an electric field variable on the electronic (sub-fs) time scale for steering electrons in excited electronic states (Öffnet internen Link im aktuellen FensterC.2.4, Öffnet internen Link im aktuellen FensterC.2.5). Here we aim at realising both objectives. To this end, waveform-stabilised, few-cycle (~5 fs) near-infrared (~750 nm) pulses will be parametrically amplified to the millijoule level. Subsequently, they first produce attosecond xuv pulses and will then — following separation from the xuv beam — be used for supercontinuum generation in a gas-filled capillary (see Fig. 1).

The continuum generation will be followed by a LiF or CaF2 prism sequence for dispersion control. In the Fourier plane, a static transparent LiF phase mask will ensure that the delay line is disperson-free to all orders over the entire spectral range of ~130–1300 nm, whereas thin and narrow rotatable LiF plates will permit adjusting the delay between different groups of frequencies to synthesise intense light fields controllable on a sub-femtosecond scale. Alternatively, we may select a quasi-monochromatic pulse of predetermined carrier wavelength by introducing an adjustable slit.

An alternative concept for the compression relies on the separation of regions of the ultra-broadband spectrum, selective phase correction for each part and subsequent recombination with interferometric precision. For all approaches the spectral phase of the pulses and sub-pulses have to be measured as well as the phase properties of newly developed optical elements. ZAP-SPIDER1) will be used for this purpose. Finally, the synthesis will be completed by measuring the waveform with an attosecond xuv pulse 2).

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