Abstract

High harmonic generation (HHG) is an established means of producing coherent, short wavelength, ultrafast pulses from a compact set-up. Table-top high-harmonic sources are increasingly being used to image physical and biological systems using emerging techniques such as coherent diffraction imaging and ptychography. These novel imaging methods require coherent illumination, and it is therefore important to both characterize the spatial coherence of high-harmonic beams and understand the processes which limit this property. Here we investigate the near- and far-field spatial properties of high-harmonic radiation generated in a gas cell. The variation with harmonic order of the intensity profile, wavefront curvature, and complex coherence factor is measured in the far-field by the SCIMITAR technique. Using the Gaussian-Schell model, the properties of the harmonic beam in the plane of generation are deduced. Our results show that the order-dependence of the harmonic spatial coherence is consistent with partial coherence induced by both variation of the intensity-dependent dipole phase as well as finite spatial coherence of the driving radiation. These findings are used to suggest ways in which the coherence of harmonic beams could be increased further, which would have direct benefits to imaging with high-harmonic radiation.

Highlights

  • Beams, this technique averages over the bandwidth of the incident radiation and, for the case of coherence measurements, requires a subsidiary measurement of the transverse beam profile

  • We extend these treatments by interpreting our results within the more general Gaussian-Schell model (GSM) for the propagation of light from partially coherent sources[18]

  • In this paper we report the results of experiments using the SCIMITAR technique to measure the variation with harmonic order q of the intensity width, wavefront curvature, and complex coherence factor (CCF) in the far-field

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Summary

Methods

The SCIMITAR technique can be used to measure the spatial properties of a beam from a single scan. As expected, this diameter is smaller than the measured spot size of the driving beam. It has been shown previously[27] that the peak intensity of a harmonic order in the plateau region generated by a single atom can be approximated by: I(qω0) ∝I(ω0)n, with n > 1 and ω0 refers to the angular frequency of the fundamental. A simple model which includes both of these effects is able to reproduce the harmonic dependence of the spatial coherence width quite closely

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