LCLS Time Tool

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a, b, and c show the transmitted single-shot spectra, stacked so that the abscissa and ordinate correspond to the spectrum (mapped to time delay) and shot-number respectively. a The delay between the X-rays and the laser was scanned in 500 fs steps, twice the full width at half maximum (FWHM) natural jitter of the LCLS. Panels b and c incrementally zoom as indicted by the white lines in previous a and b, respectively. d shows lineouts of shot in c shots.
Figure from: Mina R. Bionta, H. T. Lemke, J. P. Cryan, et al., “Spectral encoding of x-ray/optical relative delay,” Opt. Exp. 19(21), 21855 (2011).
 

The Linac Coherent Light Source (LCLS) is an X-ray free electron laser (FEL) at the SLAC National Accelerator Laboratory in Menlo Park, CA. It is a unique facility designed to reveal fundamental processes in materials, technologies and living things. It provides an ultrafast, coherent, X-ray probe with a pulse duration on the order of 1-10 fs, that can be used to track dynamics on their natural, femtosecond timescales with atomic-level resolution.

While the facility provides short pulses ideal for investigating fast processes, there is an uncorrectable inherent temporal jitter between the X-ray pulses and other tools used to study these phenomena. Unless compensated for, this jitter renders it impossible to obtain fine time-resolved mesaurements. I developed a measure-and-sort approach that time-stamps the arrival time of each LCLS pulse with respect to the optical laser pulse so that users can time sort their data in post processing, yielding time-dependent results with fine time resolution. This is done using a spectral encoding method.

A broadband super-continuum probe is chirped such that its different frequency components arrive at slightly different times, providing a mapping of wavelength to time. The probe is passed simultaneously with an X-ray pulse through an optically transparent sample, such as Si3N4 or Ce:YAG, during which the X-ray induces a change in the complex index of refraction of the material. This produces a feature in the transmitted spectrum, the location of which corresponds to the arrival time of the X-ray pulse. The spectral time-tool is now part of the standard configuration for all LCLS experiments. This means that nearly every time-resolved experiment performed at the LCLS uses this tool to temporally sort data. Time-stamps are now automatically calculated and saved into the data stream as experiments are being performed.

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