X-ray pulse compression using strained crystals
Introduction
Synchrotrons have had an enormous impact of many areas of science and technology. X-rays of very high brightness are now available from modern third-generation sources. However there appears to be an insatiable demand for X-rays of even greater brightness, or coherence, and work towards fourth generation, free-electron laser (FEL) X-ray sources [1] is now being actively pursued.
The Linac Coherent Light Source (LCLS) [2] is such a proposed fourth-generation source and will produce X-rays with a high-transverse coherence in the wavelength range 1.5–15 Å. This device is proposed for construction at the Stanford Linear Accelerator Center (SLAC). The photon output will consist of high brightness, transversely coherent pulses with duration 230 fs and relative spectral bandwidth (Δλ/λ) of 0.05%. At a wavelength of 1.5 Å the peak power of the pulse will be 9 GW, or approximately 2×1012 photons per pulse. The peak brightness of the source will be about ten orders of magnitude greater than current third-generation synchrotron sources [3].
A major area of application for this instrument will require high fluence X-ray pulses with a pulse length somewhat shorter than the 230 fs pulses currently envisaged. Indeed, the proposed biological imaging experiments will need a pulse length of 20 fs or less [4]. Shorter X-ray pulses may be generated by either compressing the pulse using techniques analogous to those used for optical lasers, or selecting a small time section out of the X-ray pulse (time-slicing). It has been proposed to “chirp” the FEL electron pulse [5] to imprint a time measure on the X-ray pulse and use this as the basis for the generation of shorter X-ray pulses. As an example of a time-slicing approach, it would in principle be possible to extract a short segment of the pulse with a monochromator of appropriate bandwidth [6], [7]. While it is possible to envisage simple time-slicing approaches, they are inevitably only able to use a fraction of the total pulse energy (equal to the fractional reduction in pulse length). Pulse compression, on the other hand, attempts to preserve the total pulse energy. The short wavelength and lack of purely refracting materials means that a simple adaptation of the ideas developed for optical lasers, based on dispersive elements such as gratings [8], [9], lead to impractical geometries and poor efficiencies that do not offer a significant advantage over time slicing. The aim of this paper is propose and analyze a technique for compressing a chirped X-ray pulse by diffraction from a strained crystal.
Section snippets
The strained crystal compressor concept
The basic concept of the strained crystal compressor is that the lattice spacing varies with depth into the crystal and different wavelengths of the chirped beam reflect at different depths according to Bragg diffraction (see Fig. 1). The different wavelengths in the pulse therefore experience different optical paths in such a manner as to compress the pulse. That is, the leading wavelength of the pulse, which diffracts more deeply in the crystal, is delayed by an entire pulse length relative
Conclusions
This paper has presented a simple technique that shows promise of being an effective and efficient method for the compression of X-ray FEL pulses to the length at which they become interesting for biological imaging experiments. The method should be simple to implement using technology that is largely available now. An interesting remaining challenge is the development of the technology to measure the length of X-ray pulses in the femtosecond time domain.
Acknowledgements
The authors acknowledge helpful discussions with Alan Wootton, John Arthur, Carl Schroeder, and Jerry Hastings. This work was performed under the auspices of the US Department of Energy by the University of California, Lawrence Livermore National Laboratory under contract No. W-7405-Eng-48.
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