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Volume 2012 (2012), Article ID 151092, 3 pages
Plastic Deformation in Profile-Coated Elliptical KB Mirrors
1X-ray Science Division, Argonne National Laboratory, Argonne, IL 60439, USA
2National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, NY 11973, USA
3Synchrotron Soleil, BP 48 Saint-Aubin, 91192 Gif-sur-Yvette, France
4Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA
Received 19 July 2012; Accepted 8 August 2012
Academic Editors: K. Hane and S. R. Restaino
Copyright © 2012 Chian Liu et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Profile coating has been successfully applied to produce elliptical Kirkpatrick-Baez (KB) mirrors using both cylindrical and flat Si substrates. Previously, focusing widths of 70 nm with 15-keV monochromatic and 80 nm with white beam were achieved using a flat Si substrate. Now, precision elliptical KB mirrors with sub-nm figure errors are produced with both Au and Pt coatings on flat substrates. Recent studies of bare Si-, Au-, and Pt-coated KB mirrors under prolonged synchrotron X-ray radiation and low-temperature vacuum annealing will be discussed in terms of film stress relaxation and Si plastic deformation.
It has long been recognized that mirror figure can be modified by controlled thin-film deposition [1, 2]. We have developed a profile-coating technique to make ultraprecise elliptical mirrors for X-ray microfocusing [3, 4]. Elliptical KB mirrors with sub-nm figure errors can now be produced using flat Si substrates with only two profile coatings. Sub-100-nm focusing has been demonstrated using a synchrotron X-ray beamline . Nested KB mirrors have also been successfully fabricated [6, 7]. One serious concern of X-ray mirrors is their long-term figure stability. We have noticed changes in mirror figure during prolonged X-ray irradiation when the mirror is too thin and narrow. The observed changes are believed to result from plastic deformation of profile-coated KB mirrors. This plastic deformation is a surprise since in our applications there is very little heat load on each KB mirror and the Si substrate has a brittle-ductile transition of 847°C .
The plastic deformation may be related to film stress introduced during coatings. The film stress can be relaxed at temperatures as low as a few hundred degrees C . We found that low-temperature vacuum annealing can cause plastic deformation similar to that introduced by prolonged X-ray radiation in profile-coated KB mirrors. To overcome this plastic deformation, we need to optimize the mirror dimensions to improve mechanical stability and to decrease the film stress.
2. Recent Results of Au- and Pt-Coated KB Mirrors Using Flat Si Substrates
Precision elliptical KB mirrors with sub-nm figure errors have been fabricated with a predicted focal spot of 38.9 nm (FWHM), compared to the diffraction limit of 37.8 nm for a perfect ellipse . On the 34-ID beamline at the Advanced Photon Source of Argonne National Laboratory, an Au-profile-coated KB pair, with dimensions of 70-mm L × 9-mm W × 4.5-mm H and 40-mm L × 10-mm W × 20-mm H, has produced ~0.60 × 0.40 μm2 focused white beams for several years under normal conditions until it was recently subjected to prolonged X-ray radiation continuously with the slits fully open for several days. After this exposure, the KB pair performance degraded so severely that it could no longer be used for microfocusing.
3. Extended Synchrotron Radiation and Low-Temperature Annealing Tests
One of the damaged mirrors, the 70 mm long one, was remeasured using microstitching interferometry. The mirror was coated with a uniform 15 nm thick Cr underlayer and an Au-profiled layer with thicknesses varying from 100 nm in the center to over 6 μm at the ends. The surface profiles before and after the extended X-ray radiation are shown in Figure 1(a). The profiles overlap with each other, but their height difference shows a clear upward, concaved profile change. The maximum deflection at the center of the mirror is ~140 nm. Another similar profile-coated KB mirror was annealed at 350°C for 15 min and measured before and after annealing, with results shown in Figure 1(b). An upward profile change is also evident after the annealing, with a maximum deflection of ~175 nm.
We repeated the same annealing procedure for a bare Si substrate, an Au- and a Pt-profile-coated mirror, with the same dimensions of 70-mm L × 9-mm W × 4.5-mm H. All samples were annealed three times with their surface profiles measured after each annealing and compared to that before each annealing. The maximum deflection results were plotted as shown in Figure 2. After the first annealing, they all had an upward concave profile change, with the Au-coated one changed the most. After the second annealing, the changes were all smaller. For Au-coated and bare Si, the profile change became convex. The third annealing had very little effect for all three samples.
When flat substrates are used for profile coating of KB mirrors the film stress becomes a significant problem. For mirror application, an ultrasmooth, highly reflective coating is needed, which is often achieved using growth conditions with a low Ar pressure and a low substrate temperature. A large film stress is expected under these conditions  and will bend the substrate. For a wafer substrate the curvature change due to film stress is proportional to , where and are the film and the substrate thickness, respectively . When the substrate is relatively thin and narrow, a film stress relaxation  can change the surface profile. A high film stress may also induce defect movements in the underlying Si at low activation energies, leading to plastic deformation in the substrate [13, 14]. The film stress relaxation is believed to be due to a diffusive relief of compressive stresses . A film with a lower stress is expected to have a lower stress relaxation. Pt has a relatively smaller thermal expansion coefficient than Au and thus a smaller thermal stress, which may attribute to the observed differences in a smaller stress relaxation (Figure 2). The bare Si substrate also has a surface stress due to a compression of the surface layer during polishing [15, 16]. For chemical-mechanical polished substrates, the surface stress is relatively small and decreases rapidly with annealing. This smaller stress explains the smaller deflection for the bare Si substrate as shown in Figure 2.
The plastic deformation of the profile-coated KB mirrors under prolonged X-ray irradiation may also be due to film stress relaxation. It is known that the dominant absorption mechanism of the X-ray energy is photoionization in a thin surface layer . This surface effect may be sufficient to cause a stress relaxation in the Au film without a noticeable increase in the mirror temperature. The surface photoionization under extended X-ray radiation may cause the same effect in the coated film as observed in low-temperature annealing. To make the mirror more stable, we need to use thicker substrates and decrease the film stress. One may choose coating materials with a smaller film stress, or coat only a strip on the mirror instead of coating the whole surface. Low-temperature annealing before the final corrective coating should also be helpful, even though the annealing temperature is limited by crystallization in the thick film. One may use spherical substrates so that less coating is needed. However, only a small region close to the center line can be coated precisely according to the design parameters due to the spherical shape of the substrate. In this case, a profile-figured substrate would be a much better choice. Currently, a profile-etching technique is under development to make such substrates using a broad beam ion source .
The authors would like to thank M. Wieczorek and J. Attig from Argonne National Laboratory for technical assistance. Work at Argonne was supported by the US Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract no. DE-AC02-06CH11357. G. E. Ice and J. Z. Tischler were supported by the DOE Office ofBasic Energy Sciences, Department of Materials Sciences and Engineering. R. Conley and C. M. Kewish were at Argonne and J. Z. Tischler was at Oak Ridge National Laboratory when this work was done.
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