The present invention relates generally to thin-film diamond mounting apparatus, and more particularly, relates to a method and mechanical design for thin-film diamond crystal mounting apparatus for coherence preservation x-ray optics with optimized thermal contact and minimized crystal strain.
Thin-film type-IIa high-pressure high-temperature (HPHT) synthetic diamond-crystals have widespread applications in the field of x-ray optics, such as x-ray optics cavities for hard x-ray free-electron laser oscillators (XFELOs), self-seeding monochromators for hard x-ray free-electron laser (XFEL), ultra-high resolution diamond crystal monochromators/analyzers, beam-sharing, and beam-split-and-delay devices for XFEL and synchrotron radiation facilities. In many cases, the required thickness of the diamond crystals could be in the range of 30-120 micron.
For instance, the diamond crystal for hard x-ray self-seeding monochromator at the Linac Coherent Light Source (LCLS) at SLAC National Accelerator Laboratory is using a 100-micron to 150-micron-thick, very high quality thin diamond-crystal plate with (001) orientation. To minimize the strain in the diamond crystal induced by the holder structure, the diamond-crystal holder was designed to have a precision slot machined on the main body with a trapezoid shape, which is matched with the diamond-crystal shape to prevent the crystal sliding out of the holder. With an optimized sliding fit, the diamond-crystal is held in the holder with a stable and near strain-free condition. The results of LCLS hard x-ray self-seeding project clearly demonstrate self-seeding at Angstrom wavelengths with a factor of 40-50 bandwidth reduction observed with respect to SASE operation.
To overcome the heat transfer limitations of the sliding-fit-type diamond-crystal holder design described above, known diamond optical assemblies have been developed for a beam-multiplexing x-ray monochromator at the LCLS. Manufactured by Technological Institute for Superhard and Novel Carbon Materials (TISNCM), a dedicated crystal mounting method was developed with perforated or nonperforated CVD diamond springs to provide a gentle clamping force between the Type IIa HPHT thin-film diamond (111) crystal and the thick CVD diamond holder base in the range of ˜2.4×10−3 N to ˜1.2×10−2 N. With these assemblies installed in the double-crystal monochromator at the LCLS, the capability of splitting the XFEL beam into a pink and a monochromatic branch was demonstrated.
Both the sliding fit mounting method and CVD diamond springs mounting method only provide fixed clamping forces.
A need exist for a mounting apparatus to enable changing the contact force remotely and dynamically to optimize the thermal contact condition with minimized crystal strain in-situ.
It is desirable to provide an enhanced thin-film diamond crystal mounting apparatus.
Principal aspects of the present invention are to provide a method and mechanical design for thin-film diamond crystal mounting apparatus for coherence preservation x-ray optics with optimized thermal contact and minimized crystal strain. Other important aspects of the present invention are to provide such method and thin-film diamond crystal mounting apparatus substantially without negative effect and that overcome some of the disadvantages of prior art arrangements.
In brief, a method and mechanical design for a thin-film diamond crystal mounting apparatus for coherence preservation x-ray optics with optimized thermal contact and minimized crystal strain are provided. The novel thin-film diamond crystal mounting apparatus mounts a thin-film diamond crystal supported by a chemical vapor deposition (CVD) diamond film spacer, and two groups of thin film thermal conductors, such as thin CVD diamond film thermal conductor groups separated by the thick CVD diamond spacer. The two groups of thin CVD film thermal conductors provide thermal conducting interface media with the thin-film diamond crystal. A piezoelectric actuator is integrated into a flexural clamping mechanism generating a clamping force from zero to an optimal level.
In accordance with features of the invention, the novel thin-film diamond crystal mounting apparatus has been designed and constructed at the Advanced Photon Source (APS) at Argonne National Laboratory with clamping force controls from zero to an optimized level.
In accordance with features of the invention, the thin-film diamond crystal includes a thin-film type-IIa high-pressure high-temperature (HPHT) synthetic diamond-crystal.
In accordance with features of the invention, the thick chemical vapor deposition (CVD) diamond film spacer has a thickness slightly thicker than the thin-film diamond crystal.
In accordance with features of the invention, a thermal compound is added to an interface between the thick CVD diamond film spacer and the thin-film diamond crystal to enhance the interface heat transfer coefficient.
In accordance with features of the invention, the flexural clamping mechanism includes a clamping arm which is mounted on a flexural pivot. On the clamping arm, there is an adjusting screw with lock nut to provide initial clamping force manual setup.
In accordance with features of the invention, the dynamic clamping force acting on the thin-film HPHT diamond-crystal is generated by the piezoelectric actuator through a clamping arm.
The present invention together with the above and other objects and advantages may best be understood from the following detailed description of the preferred embodiments of the invention illustrated in the drawings, wherein:
In the following detailed description of embodiments of the invention, reference is made to the accompanying drawings, which illustrate example embodiments by which the invention may be practiced. It is to be understood that other embodiments may be utilized and structural changes may be made without departing from the scope of the invention.
The terminology used herein is for the purpose of describing particular embodiments only and is not intended to be limiting of the invention. As used herein, the singular forms “a”, “an” and “the” are intended to include the plural forms as well, unless the context clearly indicates otherwise. It will be further understood that the terms “comprises” and/or “comprising,” when used in this specification, specify the presence of stated features, integers, steps, operations, elements, and/or components, but do not preclude the presence or addition of one or more other features, integers, steps, operations, elements, components, and/or groups thereof.
In accordance with features of the invention, a method and a mechanical design for thin-film diamond crystal mounting apparatus for coherence preservation x-ray optics with optimized thermal contact and minimized crystal strain. This novel mechanical design can be applied to new development in the field of: x-ray optics cavities for hard x-ray free-electron laser oscillators (XFELOs), self-seeding monochromators for hard x-ray free-electron laser (XFEL) with high average thermal loading, high heat load diamond crystal monochromators and beam-sharing/beam-split-and-delay devices for XFEL facilities and Advanced Photon Source (APS) future upgraded high-brightness coherent x-ray source in the MBA lattice configuration.
Having reference now to the drawings, in
The novel thin-film diamond crystal mounting apparatus 200 provides dynamic clamping force control to optimize the thermal contact condition with minimized crystal strain in-situ in accordance with preferred embodiments. A prototype of the novel thin-film diamond crystal mounting apparatus 200 has been designed and constructed at the Advanced Photon Source (APS) with clamping force controls from zero to an optimized level for coherence preservation hard x-ray optics applications. The thin-film diamond crystal mounting apparatus 200 includes a mounting base 202 and a bottom plate 204.
Referring also to
As best shown in
A novel feature of this new novel thin-film diamond crystal mounting apparatus 200 is its basic crystal mounting mechanism using the two groups of thin film thermal conductors 304, 306 having thicknesses in the range of 10-20 micron, as thermal conducting and interface media with the thin-film type-IIa HPHT synthetic diamond-crystal 201.
Referring also to
A piezoelectric actuator 206 is integrated into a flexural clamping mechanism generally designated by the reference character 208 generating a clamping force from zero to an optimal level. The dynamic clamping force acting on the thin-film type-IIa HPHT synthetic diamond-crystal 201 is generated by the piezoelectric actuator 206 through a clamping arm 210 engaging contact point 211. The flexural clamping mechanism 208 includes the clamping arm 210 mounted on a flexural pivot 212. The clamping arm 210 is coupled to the piezoelectric actuator 206 with an adjusting screw 214 and a lock nut 216 to provide an initial clamping force manual setup. One or more screws 218 are coupled to the thick CVD diamond film spacer 302 clamp the two groups of thin film thermal conductors 304, 306 with the thick CVD diamond film spacer 302 to a thick CVD diamond thermal conductor 222.
As shown on the right side in
As shown in the detailed view 301 in
Other than the thin film type-IIa HPHT synthetic diamond-crystal 201, and two groups of thin film thermal conductors 304, 306, the choice of the materials to construct the other components of the thin-film diamond crystal mounting apparatus 200 are determined by its operation environment conditions with different applications.
For synchrotron radiation applications operating in an ultra-high-vacuum (UHV) environment condition, the mounting base 202 and bottom plate 204 are made of oxygen-free copper (OFHC) with Nickel and Gold coating. The clamping arm 210 and screws 214, 218, 220 are made of aluminum alloy or stainless steel. Gallium-indium eutectic alloy is added on the edge interface 308 between the thin-film type-IIa HPHT synthetic diamond-crystal 201 and thick CVD diamond film spacer 302 to enhance the interface heat transfer coefficient significantly.
For thin-film diamond crystal mounting apparatus 200 with electron beams nearby applications, such as XFEL self-seeding monochromators with high average thermal loading, high strength graphite, such as Highly Ordered Pyrolytic Graphite (HOPG) or CVD diamond could be used to construct the mounting base 202, bottom plate 204, clamping arm 210, and the like. A Molybdenum radiation shielding cover will be added to protect the piezoelectric actuator 206. Vacuum compatible low-Z-material-based thermal compound is needed to apply on the edge interface 308 between the thin-film type-IIa HPHT synthetic diamond-crystal 201 and thick CVD diamond film spacer 302.
In synchrotron radiation applications with ambient or Helium environment conditions, the mounting base 202 could be made of oxygen-free copper (OFHC) or aluminum alloy. Regular thermal compound could be applied on the edge interface 308 between the thin-film type-IIa HPHT synthetic diamond-crystal 201 and the thick CVD diamond film spacer 302.
While the present invention has been described with reference to the details of the embodiments of the invention shown in the drawing, these details are not intended to limit the scope of the invention as claimed in the appended claims.
The United States Government has rights in this invention pursuant to Contract No. DE-AC02-06CH11357 between the United States Government and UChicago Argonne, LLC representing Argonne National Laboratory.
Number | Name | Date | Kind |
---|---|---|---|
4602377 | Schiferl | Jul 1986 | A |
4776223 | Moss | Oct 1988 | A |
4822466 | Rabalais | Apr 1989 | A |
5113661 | Deeks | May 1992 | A |
5295402 | Bovenkerk | Mar 1994 | A |
5509043 | Van Der Sluis | Apr 1996 | A |
5524040 | Alp | Jun 1996 | A |
5693345 | Chen | Dec 1997 | A |
6082200 | Aslam | Jul 2000 | A |
6456688 | Taguchi | Sep 2002 | B1 |
6543295 | Xu | Apr 2003 | B2 |
6574306 | Kikuchi | Jun 2003 | B2 |
6582513 | Linares | Jun 2003 | B1 |
6607840 | Shu et al. | Aug 2003 | B2 |
6807251 | Okanda | Oct 2004 | B2 |
6822733 | Shu et al. | Nov 2004 | B1 |
6858080 | Linares | Feb 2005 | B2 |
6885726 | Uehara | Apr 2005 | B2 |
6917667 | Fujinawa | Jul 2005 | B2 |
6947518 | Itoga | Sep 2005 | B2 |
6984335 | Shu et al. | Jan 2006 | B2 |
7099437 | Pike | Aug 2006 | B2 |
7162888 | Shu et al. | Jan 2007 | B2 |
7314540 | Seki | Jan 2008 | B2 |
7332727 | Kawashima | Feb 2008 | B2 |
7390695 | Meguro | Jun 2008 | B2 |
7396408 | Schreck | Jul 2008 | B2 |
7508912 | Zhong | Mar 2009 | B2 |
7579759 | Lee | Aug 2009 | B2 |
7581403 | Deeks | Sep 2009 | B2 |
7594968 | Hemley | Sep 2009 | B2 |
7597475 | Shu et al. | Oct 2009 | B1 |
7736472 | Kawashima | Jun 2010 | B2 |
7738630 | Burdett, Jr. | Jun 2010 | B2 |
7791291 | Gorrell | Sep 2010 | B2 |
7799599 | Sung | Sep 2010 | B1 |
7820131 | Hemley | Oct 2010 | B2 |
7848489 | He | Dec 2010 | B1 |
7883684 | Hemley | Feb 2011 | B2 |
7892356 | Meguro | Feb 2011 | B2 |
8076034 | Lassila | Dec 2011 | B1 |
8089199 | Shu et al. | Jan 2012 | B2 |
8119241 | Ueda | Feb 2012 | B2 |
8126117 | Verman | Feb 2012 | B2 |
8455048 | Fan | Jun 2013 | B1 |
8559597 | Chen | Oct 2013 | B2 |
8724776 | Haas | May 2014 | B2 |
8810904 | Jacobsen | Aug 2014 | B2 |
8957567 | Shu et al. | Feb 2015 | B2 |
9008272 | Shu et al. | Apr 2015 | B2 |
9133566 | Twitchen | Sep 2015 | B2 |
9180420 | Fan | Nov 2015 | B1 |
9194824 | Qian | Nov 2015 | B1 |
9217207 | Chang | Dec 2015 | B2 |
9269468 | Ryan | Feb 2016 | B2 |
9469918 | Xu | Oct 2016 | B2 |
9484178 | Yamada | Nov 2016 | B2 |
9529098 | Stoupin | Dec 2016 | B2 |
9613729 | Shu | Apr 2017 | B2 |
Entry |
---|
I. Kantor et al., “BX90: A new diamond anvil cell design for X-ray diffraction and optical measurements,” Review of Scientific Instruments 83, 125102 (2012). |
Ronald Miletich, “Types of Diamond-Anvil Cells and how to work with them,” ECM-27 High-P Workshop Methods of high-P single crystal x-ray diffraction. Aug. 2012. |
A. Jayaraman, Review of Modern Physics, vol. 55, No. 1, Jan. 1983, pp. 65-108. |
K.-J. Kim and Y. Shvyd'ko, “Tunable optical cavity for an x-ray free-electron-laser oscillator”, Phys. Rev. ST-AB 12, 030703, 2009. |
J. Amann, et al., “Demonstration of self-seeding in a hard-X-ray free-electron laser”, Nature Photonics DOI:10.1038-180, 2012. |
S. Stoupin, et al., “Hybrid diamond-silicon angular-dispersive x-ray monochromator with 0.25-meV energy bandwidth and high spectral efficiency”, Optics Express vol. 21 Issue 25, pp. 30932-30946, 2013. |
Y. P. Stetsko and et al., “Time-delayed beam splitting with energy separation of x-ray channels”, Appl. Phys. Lett. 103, 173508,2013. |
S. Stoupin, et al., “Diamond crystal optics for self-seeding of hard-X-rays in X-ray free-electron lasers”, Diamond & Related Materials 33, 1-4, 2013. |
D. Shu, et al., “Design of a diamond-crystal monochromator for the LCLS hard x-ray self-seeding project”, J. Phys. Conf. Ser. 425 052004, 2013. |
S. Stoupin, et al., “All-diamond optical assemblies for a beam-multiplexing X-ray monochromator at the Linac Coherent Light Source”, J. Appl. Cryst. 47, 1329-1336, 2014. |
D. Zhu et al., “Performance of beam-multiplexing diamond crystal monochromator at the Linac Coherent Light Source”, Rev. Sci. Instrum. 85, 063106, 2014. |
Number | Date | Country | |
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20170085055 A1 | Mar 2017 | US |