X-ray surface analysis and measurement apparatus

US2016178540A1 · US · A1

Patent metadata
FieldValue
Publication numberUS-2016178540-A1
Application numberUS-201615060477-A
CountryUS
Kind codeA1
Filing dateMar 3, 2016
Priority dateFeb 28, 2014
Publication dateJun 23, 2016
Grant date

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  5. First independent claim

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Abstract

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This disclosure presents systems for x-ray diffraction/scattering measurements that have x-ray flux and x-ray flux density several orders of magnitude greater than existing x-ray technologies. These may therefore be useful for applications such as structural analysis and crystallography. The higher brightness is achieved in part by using designs for x-ray targets that comprise a number of microstructures of one or more selected x-ray generating materials fabricated in close thermal contact with a substrate having high thermal conductivity. This allows for bombardment of the targets with higher electron density or higher energy electrons, which leads to greater x-ray brightness and therefore greater x-ray flux. The high brightness/high flux source may then be coupled to an x-ray reflecting optical system, which can focus the high flux x-rays to a spots that can be as small as one micron, leading to high flux density.

First claim

Opening claim text (preview).

We claim: 1 . An x-ray system for analyzing a specimen, comprising: at least one x-ray source comprising: a plurality of x-ray generating sub-sources, in which each of the x-ray generating sub-sources has a source size less than 20 micrometers in at least one direction, and is aligned along a predetermined axis so that x-rays generated from at least two of the plurality of x-ray generating sub-sources accumulate within a predetermined divergence angle relative to the predetermined axis; and additionally comprising: an x-ray optical system having an optical axis aligned relative to the predetermined axis, said optical system positioned to collect diverging x-rays accumulated from said at least two of the plurality of the of x-ray generating sub-sources in the x-ray source and to condition and create an x-ray beam with predetermined properties; said optical system additionally comprising a central beam stop positioned to block x-rays propagating parallel to the optical axis; a means to direct the x-ray beam to be incident with a grazing angle of less than 5 degrees onto an area of a surface of a specimen; at least one detector which detects the intensity of the x-rays emerging from the specimen and generates electrical signals; and a signal processor to analyze the electrical signals to obtain information about at least one of: composition, concentration, quantity, and film thickness. 2 . The x-ray system of claim 1 , in which said at least one detector is positioned to detect x-rays that are diffracted by the specimen; and additionally comprising: at least one additional detector to detect x-rays reflected from the surface of the specimen. 3 . The x-ray system of claim 1 , in which said predetermined axis and said optical axis are coincident. 4 . The x-ray system of claim 1 , in which said optical system comprises a total external reflection based x-ray optic, and said predetermined divergence angle is determined in part based on the critical angle of said x-ray optic. 5 . The x-ray system of claim 1 , in which said predetermined divergence angle is determined in part based on the total length along the optical axis of the x-ray generating region. 6 . The x-ray system of claim 1 , in which said x-ray beam with predetermined properties has the property of being focused to a single spot with a spot size smaller than 300 microns; and in which the focused x-ray spot corresponds to a predetermined position on the surface of the specimen. 7 . An x-ray measurement system, comprising: an x-ray source, comprising: one electron beam emitter; and one anode target comprising: a substrate comprising a first selected material, in which said substrate has at least one planar surface; and a plurality of discrete structures aligned along a predetermined axis comprising a second material selected for its x-ray generation properties; in which each of the plurality of discrete structures is in thermal contact with the substrate; and in which at least two of the discrete structures have at least one dimension parallel to said planar surface of less than 20 microns; and additionally comprising: an electron beam control system to direct electrons from the electron beam emitter onto the plurality of discrete structures; an optical train having an optical axis to collect diverging x-rays generated by said at least two of the plurality of discrete structures in the anode target, and that produces an x-ray beam with predetermined beam properties; said optical train additionally comprising a central beam stop positioned to block x-rays propagating parallel to said optical axis; a mount to hold an object to be investigated, positioned such that the x-ray beam will be incident on the object at a grazing angle of less than 5 degrees; and a detector to measure x-rays emerging from the object when x-rays are incident on the object. 8 . The system of claim 7 , in which said detector is positioned to detect x-rays that are diffracted by the specimen; and additionally comprising: an additional detector to measure the intensity of the x-rays reflected from the object. 9 . The system of claim 7 , in which each dimension parallel to said at least one planar surface of said at least two of the discrete structures is less than 50 microns. 10 . The system of claim 7 , in which the plurality of discrete structures are arranged in a linear array along said predetermined axis; and the optical axis of the optical train is also aligned along said predetermined axis. 11 . The system of claim 7 , in which the first selected material is selected from the group consisting of: beryllium, diamond, graphite, silicon, boron nitride, silicon carbide, sapphire and diamond-like carbon. 12 . The system of claim 7 , in which the second material is selected from the group consisting of: aluminum, titanium, vanadium, chromium, manganese, iron, cobalt, nickel, copper, gallium, zinc, yttrium, zirconium, molybdenum, niobium, ruthenium, rhodium, palladium, silver, tin, iridium, tantalum, tungsten, indium, cesium, barium, gold, platinum, lead and combinations and alloys thereof. 13 . The system of claim 7 , additionally comprising: an additional plurality of discrete structures aligned along said predetermined axis comprising a third material selected for its x-ray generation properties, in which each of the additional plurality of discrete structures is in thermal contact with the substrate, and in which at least two of the additional discrete structures have at least one dimension parallel to said planar surface of less than 20 microns. 14 . The system of claim 13 , in which the third material is selected from the group consisting of: aluminum, titanium, vanadium, chromium, manganese, iron, cobalt, nickel, copper, gallium, zinc, yttrium, zirconium, molybdenum, niobium, ruthenium, rhodium, palladium, silver, tin, iridium, tantalum, tungsten, indium, cesium, barium, gold, platinum, lead and combinations and alloys thereof. 15 . The system of claim 7 , in which the plurality of discrete structures are arranged such that x-rays generated by a predetermined number of the plurality of discrete structures when exposed to an electron beam from the electron beam emitter are transmitted through a predetermined one of the discrete structure selected from the plurality of discrete structures. 16 . The system of claim 7 , in which the anode target is mounted such that the anode target may rotate about an axis. 17 . The system of claim 16 , in which the electron beam control system that direct electrons from the electron beam emitter onto the plurality of discrete structures is adjusted to direct electrons only onto a region of the anode target comprising a portion of the plurality of x-ray generating structures that is aligned with the optical train. 18 . The system of claim 7 , comprising an additional number of electron emitters and, an additional number of anode targets, with each anode target corresponding to a single electron emitter, such that each electron emitter is aligned to provide an electron beam to bombard the corresponding anode target to generate x-rays; and the additional number of anode targets are aligned with each other and with said one anode target, such that the positions at which x-rays are generated in said one anode target and said additional number of anode targets are al

Assignees

Inventors

Classifications

  • by measuring small-angle scattering · CPC title

  • G01N23/205Primary

    using diffraction cameras · CPC title

  • for measuring thickness · CPC title

  • for spectrometry, i.e. using an analysing crystal, e.g. for measuring X-ray fluorescence spectrum of a sample with wavelength-dispersion, i.e. WDXFS · CPC title

  • Devices having a multilayer structure · CPC title

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What does patent US2016178540A1 cover?
This disclosure presents systems for x-ray diffraction/scattering measurements that have x-ray flux and x-ray flux density several orders of magnitude greater than existing x-ray technologies. These may therefore be useful for applications such as structural analysis and crystallography. The higher brightness is achieved in part by using designs for x-ray targets that comprise a number of…
Who is the assignee on this patent?
Sigray Inc
What technology area does this patent fall under?
Primary CPC classification G01N23/205. Mapped technology areas include Physics.
When was this patent published?
Publication date Thu Jun 23 2016 00:00:00 GMT+0000 (Coordinated Universal Time) (A1). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 8 related publications on this page (citations in our corpus or others sharing the same primary CPC).