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Parabolic lithium refractive optics for x rays

dc.contributor.authorPereira, N. R.en_US
dc.contributor.authorDufresne, E. M.en_US
dc.contributor.authorClarke, Royen_US
dc.contributor.authorArms, D. A.en_US
dc.date.accessioned2010-05-06T21:45:04Z
dc.date.available2010-05-06T21:45:04Z
dc.date.issued2004-01en_US
dc.identifier.citationPereira, N. R.; Dufresne, E. M.; Clarke, R.; Arms, D. A. (2004). "Parabolic lithium refractive optics for x rays." Review of Scientific Instruments 75(1): 37-41. <http://hdl.handle.net/2027.42/70176>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70176
dc.description.abstractExcellent x-ray optics for photons at around 10 keV can be expected with lithium metal. One of the best compound refractive lens designs [Lengeler et al., J. Appl. Phys. 84, 5855 (1998)] is now produced routinely in aluminum, and more recently has been demonstrated using beryllium [M. Kuhlmann et al. (unpublished)]. Here, we report a similar refractive lens made from lithium. At 10.87 keV, this lens has a ≃2 m focal length, more than 90% peak transmission, and an average transmission of 49%. The lens shows a very useful gain of up to 40. The full widths at half maximum (FWHM) of the focus are blurred by roughly 20 μm, resulting in a horizontal and vertical FWHM of 33 and 17 μm for an image distance of 2.13 m. The lens produces speckle on the x-ray beam, which is likely due to the inhomogeneities of the lens surface: Coherent x-ray scattering is useful in understanding imperfections in x-ray optics, such as mirrors and lenses. Better molding techniques should result in improved performance and enable microbeam techniques with this type of Li lens. © 2004 American Institute of Physics.en_US
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dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleParabolic lithium refractive optics for x raysen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Physics and MHATT-CAT, University of Michigan, Ann Arbor, Michigan 48109-1120en_US
dc.contributor.affiliationotherEcopulse Incorporated, P.O. Box 528, Springfield, Virginia 22150en_US
dc.contributor.affiliationotherAdvanced Photon Source and MHATT-CAT, Argonne, Illinois 60439en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70176/2/RSINAK-75-1-37-1.pdf
dc.identifier.doi10.1063/1.1633007en_US
dc.identifier.sourceReview of Scientific Instrumentsen_US
dc.identifier.citedreferenceA modern account is D. Attwood, Soft X rays and Extreme Ultraviolet Radiation (Cambridge University Press, Cambridge, UK, 2000).en_US
dc.identifier.citedreferenceContemporary accounts with references to the original papers are, e.g., A. E. Lindl in Handbuch der Experimentalphysik, edited by W. Wien and F. Harms (Academic, Berlin, 1930), Vol. 24, Part, 2, p. 114; A. H. Compton and S. K. Allison, X rays in Theory and Experiment (Van Nostrand, New York, 1935); R. W. James, The Optical Principles of the Diffraction of X Rays (Ox Bow Press, Woodbridge, CT, 1948) (reprint).en_US
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dc.identifier.citedreferencePapers on the latter lens types were presented at the Eighth International Conference on Synchrotron Radiation Instrumentation, San Francisco, CA, 25–29 August 2003, AIP Conf. Proc. (to be published).en_US
dc.identifier.citedreferenceN. R. Pereira, D. A. Arms, R. Clarke, S. B. Dierker, E. M. Dufresne, and D. Foster, Proc. SPIE PSISDG4502, 173 (2001).en_US
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dc.identifier.citedreferenceE. M. Dufresne, N. R. Pereira, R. Clarke, and D. A. Arms, Advanced Photon Source Annual Report (2002).en_US
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dc.identifier.citedreferenceAachen’s website www.xray-lens.de has an excellent account of parabolic CRLs and an up to date series of papers.en_US
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dc.identifier.citedreferenceM. Kuhlmann et al., see Ref. 12.en_US
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dc.identifier.citedreferencehttp://www.mhatt.aps.anl.go/dohn/calculators/ gives the APS Undulator A beam properties. The machine currently runs with an horizontal emittance of 2.6 nm rad and a vertical coupling of 2.7%. The betatron parameters on the site are for a straight section. At 10.87 keV, the horizontal and vertical root-mean-square source sizes are, respectively, 203 and 19 μm.en_US
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dc.identifier.citedreferenceThe lower number is from the DABAX data base that is part of XOP (a well-known x-ray propagation code available at http://www.esrf.fr/computing/scientific/xop/), while the higher number is from LBL’s Center for X-Ray Optics’ website www-cxro.lbl.gov.en_US
dc.identifier.citedreferenceE. M. Dufresne, T. S. Nurushev, S. B. Dierker, and R. Clarke, Phys. Rev. E PLEEE865, 061507 (2002).en_US
dc.identifier.citedreferenceM. Krystian and W. Pichl, Mater. Charact. MACHEX46, 1 (2000).en_US
dc.identifier.citedreferenceThe x-ray properties of material properties are conveniently available on the web from Lawrence Berkeley Laboratory’s Center for X-ray Optics at www-cxro.lbl.gov.en_US
dc.owningcollnamePhysics, Department of


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