Method for evaluating modulus of repulsion elasticity, hardness and energy loss of polymer material
US-9528950-B2 · Dec 27, 2016 · US
US9874531B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9874531-B2 |
| Application number | US-201514712917-A |
| Country | US |
| Kind code | B2 |
| Filing date | May 15, 2015 |
| Priority date | Oct 31, 2013 |
| Publication date | Jan 23, 2018 |
| Grant date | Jan 23, 2018 |
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Periodic spatial patterns of x-ray illumination are used to gather information about periodic objects. The structured illumination may be created using the interaction of a coherent or partially coherent x-ray source with a beam splitting grating to create a Talbot interference pattern with periodic structure. The object having periodic structures to be measured is then placed into the structured illumination, and the ensemble of signals from the multiple illumination spots is analyzed to determine various properties of the object and its structures. Applications to x-ray absorption/transmission, small angle x-ray scattering, x-ray fluorescence, x-ray reflectance, and x-ray diffraction are all possible using the method of the invention.
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We claim: 1. A method for examining an object with periodic structures, comprising: selecting an object with periodic structures for examination; determining a volume in which a Talbot interference pattern will be formed, said Talbot interference pattern to be formed using a source of x-rays and an x-ray beam splitting grating, and to be matched in dimension and pitch to the object with periodic structures to be examined; placing the object having periodic structures into said volume; establishing the Talbot interference pattern; aligning the periodic structures of the object with the anti-nodes of the Talbot interference pattern; and detecting an x-ray signal resulting from the interaction of the Talbot interference pattern and the periodic structures of the object. 2. The method of claim 1 , in which the x-ray signal is a signal arising from transmission of x-rays through the periodic structures. 3. The method of claim 1 , in which the x-ray signal is a signal arising from small angle x-ray scattering. 4. The method of claim 1 , in which the source of x-rays is a microfocus source. 5. The method of claim 1 , in which the source of x-rays is an extended source used in conjunction with an absorbing grating comprising periodic apertures. 6. The method of claim 1 , in which the source of x-rays comprises: a vacuum chamber; an emitter for an electron beam; and an x-ray target comprising: a substrate comprising a first material and, embedded in the substrate, at least a plurality of discrete structures comprising a second material selected for its x-ray generating properties, and in which said plurality of discrete structures are arranged to form a periodic pattern of sub-sources. 7. The method of claim 6 , 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; and the second material is selected from the group consisting of: 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. 8. The method of claim 1 , in which the x-ray beam splitting grating comprises structures to introduce a phase-shift of approximately radians for a predetermined x-ray wavelength. 9. The method of claim 1 , in which the x-ray beam splitting grating comprises structures to introduce a phase-shift of approximately π/2 radians for a predetermined x-ray wavelength. 10. The method of claim 1 , in which the x-ray beam splitting grating comprises an x-ray phase-shifting grating, in which the period p 1 of the x-ray phase-shifting grating is less than or equal to the lateral coherence length of the x-rays from the x-ray source. 11. The method of claim 1 , in which matching the Talbot interference pattern to the object having periodic structures to be examined comprises selecting the x-ray beam splitting grating so that the anti-nodes of the Talbot interference pattern have the same pitch to overlap the periodic structures of the object. 12. The method of claim 1 , in which matching the Talbot interference pattern to the object having periodic structures to be examined comprises selecting the x-ray beam splitting grating so that the anti-nodes of the Talbot interference pattern have a pitch that is an integer multiple of the periodic structures of the object and will overlap a subset of the periodic structures of the object. 13. The method of claim 12 , in which the object having periodic structures is selected from the group consisting of: a semiconductor wafer, an integrated circuit, and a packaging component for an integrated circuit; and the x-ray signal provides information that leads to a determination of at least one of the properties of the periodic structures of the object selected from the group consisting of: critical dimensions, sidewall angle, pitch, and linewidth roughness.
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