K D. Finkelsteina,1, R. Jonesb, A. Paulinga, Z. Browna, A. Tarunc, S. Jupitzd, D C. Sagane, D S. Misrac
aCHESS, Cornell University, bDepartment of Physics, University of Connecticut, cIIa Technologies, Singapore, dSt. Mary’s College of Maryland, eCLASSE Cornell University
Users can collect rocking curve maps with angle resolution as small as 2μradians, spatial resolution to 3 microns, and field of view up to 7mm. The capability has been applied to: improve CVD-diamond growth, evaluate perfection of ultra-thin diamond membranes, correlate performance of diamond electronics to crystal defect structure, and for defect analysis of single crystal silicon carbide.

Figure 2: Left: shows simulated intensity distribution at the sample for 1mm(V) by 8mm(H) beam at the mono, done using Bmad[1]. The figure at right shows effective vertical angle distribution ψV = θV - (Δk / k0) tan(θBragg) vs. vertical position y at sample. ΘV, Δk / k0 are respectively beam vertical divergence, and bandwidth emerging from monochrometer. These simulations assume a Gaussian vertical source size 280 microns(RMS), 50 uradian source divergence, distance to silicon (331) mono 10.5 m, expansion factors: b=8 (reflecting up) followed by b=1 (reflecting down), mono-sample distance 4.0 meters, and diamond (220) target reflecting up. Results on right assume slits do not limit incident beam at mono.
Typical Applications
IIa Technologies grows ultra-high purity CVD diamond plate detectors, correlating width histograms from rocking curve maps with measured charge collection efficiency(CCE) and gamma ray energy resolution[2,3]. Samples with broad distribution and high average width have low CCE, while poor energy resolution is correlated with long histogram tails. Lattice disruption is thought to affect drift velocity of holes and electrons reducing detector energy resolution.

GlueX[4] experiments at Jefferson Lab measure the spectrum and decays of excited mesons. Probing the dynamics of gluons in the atomic nucleus requires a polarized beam of high energy (≥ 9 GeV) photons. The source of photons is a diamond crystal that emits high-energy polarized light when high-energy electrons pass through by the process of coherent bremsstrahlung. This is similar in many ways to x-ray diffraction but it takes place at orders of magnitude higher energy when the product of incidence angle and photon wavelength matches the atomic scale. At 9 GeV, this requires control of the beam incidence angle at the μradian level. Achieving this degree of alignment requires lattice flatness and strain characterization using high-resolution x-ray diffraction at a facility like CHESS.

References:
[1] D.C. Sagan, Nuclear Instruments and Methods in Physics Research A, 558, (2006).
[2] J. W. Keister, et al., Nucl. Instrum. Methods Phys. Res. A 649, 91 (2011).
[3] A. Tarun, et al., “Performance of CVD Diamond based Detectors”, Diamond & Related Materials, in press
[4] https://halldweb.jlab.org/wiki/index.php/GlueX_Physics