Analysis on partial coherence propagation using the four-dimensional coherence function

The mutual optical intensity (MOI) is a four-dimensional coherence function and contains the full coherence information of the beam. The propagation of mutual optical intensity through a soft x-ray beamline is analyzed with a new developed model named MOI. The MOI model is based on statistical optics. The wavefront is separated into many elements and every element is assumed to has full coherence and constant complex amplitude, which is reasonable if the dimension of element is much smaller than the coherent length and beam spot size. The propagation of MOI for every element can be analytically solved with Fraunhofer or Fresnel approximations. The total MOI propagation through free space can be obtained by summing the contribution of all elements. Local stationary phase approximation is implemented to simulate MOI propagating through ideal mirrors and gratings. The MOI model provides not only intensity profile, but also wavefront and coherence information of the beam. These advantages make MOI model a useful tool for beamline design and optimization. The nano-ARPES beamline at SSRF is analyzed using the MOI model. A zone plate is used to focus the beam. The intensity profile and local coherence degree at the zone plate are acquired. The horizontal coherence is much worse than the vertical one. By cutting the horizontal beam with the exit slit the horizontal coherence can be improved but at the flux loss. The quantitative analysis on the coherence improvement and flux loss at different exit slit size are obtained with the MOI model.

[1]  Gerhard Grübel,et al.  X-ray spectroscopy: Revealing the atomic dance. , 2009, Nature materials.

[2]  J. Goodman Statistical Optics , 1985 .

[3]  K. Nugent Coherent methods in the X-ray sciences , 2009, 0908.3064.

[4]  Liubov Samoylova,et al.  Cross-platform wave optics software for XFEL applications , 2011, Optical Engineering + Applications.

[5]  M Sánchez del Río New challenges in ray tracing simulations of X-ray optics , 2013 .

[6]  Bo Liu,et al.  Large-scale uniform Au nanodisk arrays fabricated via x-ray interference lithography for reproducible and sensitive SERS substrate , 2014, Nanotechnology.

[7]  E. H. Linfoot Principles of Optics , 1961 .

[8]  Tim Salditt,et al.  Coherence filtering of x-ray waveguides: analytical and numerical approach , 2011 .

[9]  Oleg Chubar,et al.  Recent updates in the “Synchrotron Radiation Workshop” code, on-going developments, simulation activities, and plans for the future , 2014, Optics & Photonics - Optical Engineering + Applications.

[10]  Stefan Eisebitt,et al.  High-resolution magnetic-domain imaging by Fourier transform holography at 21 nm wavelength , 2013 .

[11]  E. M. Lifshitz,et al.  Classical theory of fields , 1952 .

[12]  L. Mandel,et al.  Optical Coherence and Quantum Optics , 1995 .

[13]  Andrej Singer,et al.  Coherence properties of focused X-ray beams at high-brilliance synchrotron sources , 2013, Journal of synchrotron radiation.

[14]  Manuel Sanchez del Rio,et al.  SHADOW3: a new version of the synchrotron X-ray optics modelling package , 2011, Journal of synchrotron radiation.

[15]  Yong Wang,et al.  Numerical analysis of partially coherent radiation at soft x-ray beamline. , 2015, Optics express.

[16]  Xianbo Shi,et al.  A hybrid method for X-ray optics simulation: combining geometric ray-tracing and wavefront propagation , 2014, Journal of synchrotron radiation.