| Home > Publications database > Hybrid diamond-silicon angular-dispersive x-ray monochromator with 025-meV energy bandwidth and high spectral efficiency > print |
| 001 | 167422 | ||
| 005 | 20250717142940.0 | ||
| 024 | 7 | _ | |a 10.1364/OE.21.030932 |2 doi |
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| 037 | _ | _ | |a DESY-2014-01774 |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |a Stoupin, S. |0 P:(DE-H253)PIP1014022 |b 0 |e Corresponding author |
| 245 | _ | _ | |a Hybrid diamond-silicon angular-dispersive x-ray monochromator with 025-meV energy bandwidth and high spectral efficiency |
| 260 | _ | _ | |a Washington, DC |c 2013 |b Soc. |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 336 | 7 | _ | |a article |2 DRIVER |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1448961143_16501 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 500 | _ | _ | |3 POF3_Assignment on 2016-02-09 |
| 520 | _ | _ | |a We report on the design, implementation, and performance of an x-ray monochromator with ultra-high energy resolution (ΔE/E ≃ 2.7 × 10−8) and high spectral efficiency using x rays with photon energies E ≃ 9.13 keV. The operating principle of the monochromator is based on the phenomenon of angular dispersion in Bragg back-diffraction. The optical scheme of the monochromator is a modification of a scheme reported earlier [Shvyd’ko et al., Phys. Rev. A 84, 053823 (2011)], where a collimator/wavelength selector Si crystal was replaced with a 100-μm-thick type IIa diamond crystal. This modification provides a very-small-energy bandwidth ΔE ≃ 0.25 meV, a 3-fold increase in the aperture of the accepted beam, a reduction in the cumulative angular dispersion rate of x rays emanating from the monochromator for better focusing on a sample, a sufficient angular acceptance matching the angular divergence of an undulator source (≈ 10 μrad), and an improved throughput due to low x-ray absorption in the thin diamond crystal. The measured spectral efficiency of the monochromator was ≈ 65% with an aperture of 0.3 × 1 mm2. The performance parameters of the monochromator are suitable for inelastic x-ray spectroscopy with an absolute energy resolution ΔE < 1 meV. |
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| 700 | 1 | _ | |a Shvyd’ko, Y. V. |0 P:(DE-HGF)0 |b 1 |
| 700 | 1 | _ | |a Shu, D. |0 P:(DE-HGF)0 |b 2 |
| 700 | 1 | _ | |a Blank, V. D. |0 P:(DE-HGF)0 |b 3 |
| 700 | 1 | _ | |a Terentyev, S. A. |0 P:(DE-HGF)0 |b 4 |
| 700 | 1 | _ | |a Polyakov, S. N. |0 P:(DE-HGF)0 |b 5 |
| 700 | 1 | _ | |a Kuznetsov, M. S. |0 P:(DE-HGF)0 |b 6 |
| 700 | 1 | _ | |a Lemesh, I. |0 P:(DE-HGF)0 |b 7 |
| 700 | 1 | _ | |a Mundboth, K. |0 P:(DE-HGF)0 |b 8 |
| 700 | 1 | _ | |a Collins, S. P. |0 P:(DE-HGF)0 |b 9 |
| 700 | 1 | _ | |a Sutter, J. P. |0 P:(DE-HGF)0 |b 10 |
| 700 | 1 | _ | |a Tolkiehn, M. |0 P:(DE-H253)PIP1007498 |b 11 |
| 773 | _ | _ | |a 10.1364/OE.21.030932 |g Vol. 21, no. 25, p. 30932 - |0 PERI:(DE-600)1491859-6 |n 25 |p 30932-30946 |t Optics express |v 21 |y 2013 |x 1094-4087 |
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