Method And System For Utilizing Radio-Opaque Fillers In Multiple Layers Of Golf Balls
US-2024424351-A1 · Dec 26, 2024 · US
US9360308B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9360308-B2 |
| Application number | US-201414248673-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 9, 2014 |
| Priority date | Jul 3, 2013 |
| Publication date | Jun 7, 2016 |
| Grant date | Jun 7, 2016 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A method for analyzing an object includes measuring a first reflectivity of light from a surface and measuring a second reflectivity of light from the object, after the object is formed on the surface. A variation between the first and second reflectivities is calculated, and the variation is transformed by a predetermined transform. A thickness of the object is determined based on the transformed variation.
Opening claim text (preview).
What is claimed is: 1. A method for analyzing an object, the method comprising: measuring a first X-ray reflectivity from a substrate before formation of the object, measuring the first X-ray reflectivity including measuring a first X-ray reflectivity spectrum; forming the object on the substrate; measuring a second X-ray reflectivity from the substrate after the formation of the object, measuring the second X-ray reflectivity includes measuring a second X-ray reflectivity spectrum; generating a delta spectrum between the first and second X-ray reflectivity spectrums, the delta spectrum corresponding to a variation between the first and second X-ray reflectivities; transforming the variation using a fast-Fourier transform; and determining a thickness of the object based on the transformed variation. 2. The method as claimed in claim 1 , further comprising: irradiating an X-ray for measuring each of the first and second X-ray reflectivities at an angle of about 5 degrees or less with respect to a surface of the substrate. 3. The method as claimed in claim 1 , wherein generating the delta spectrum includes subtracting a raw first X-ray reflectivity spectrum from a raw second X-ray reflectivity spectrum. 4. The method as claimed in claim 1 , wherein the object is a layer or a pattern. 5. The method as claimed in claim 4 , wherein the layer or pattern is included in a semiconductor device. 6. The method as claimed in claim 1 , further comprising: numerically expressing a full width at half maximum (FWMH) of a peak of a result obtained by fast-Fourier transforming the variation. 7. A method for analyzing an object, the method comprising: measuring a first X-ray reflectivity from a substrate before formation of the object; forming the object on the substrate; measuring a second X-ray reflectivity from the substrate after the formation of the object; calculating a variation between the first and second X-ray reflectivities; transforming the calculated variation using a fast-Fourier transform; numerically expressing a signal to noise ratio (S/N ratio) of a result obtained by fast-Fourier transforming the calculated variation; and determining a thickness of the object based on the S/N ratio of the result obtained by fast-Fourier transforming the calculated variation. 8. A method for analyzing an object, the method comprising: measuring a first reflectivity of light from a surface; measuring a second reflectivity of light from the object, after the object is formed on the surface; calculating a variation between the first and second reflectivities; transforming the variation using a predetermined transform; and determining a thickness of the object based on the transformed variation, wherein the method further includes numerically expressing a full width at half maximum (FWMH) of a peak of a result obtained by the predetermined transform. 9. The method as claimed in claim 8 , wherein the light is in an X-ray spectrum. 10. The method as claimed in claim 8 , wherein the predetermined transform is a fast-Fourier transform. 11. The method as claimed in claim 8 , further comprising: irradiating light on the surface at a first angle; and irradiating light on the object at a second angle. 12. The method as claimed in claim 11 , wherein the first angle is substantially equal to the second angle. 13. The method as claimed in claim 11 , wherein the first and second angles are in a range of about 5 degrees or less. 14. The method as claimed in claim 8 , wherein: measuring the first reflectivity includes measuring a first reflectivity spectrum; and measuring the second reflectivity includes measuring a second reflectivity spectrum. 15. The method as claimed in claim 14 , wherein calculating the variation includes subtracting a raw first reflectivity spectrum from a raw second reflectivity spectrum. 16. The method as claimed in claim 8 , wherein: the surface is a surface of a semiconductor substrate; and the object is a formation on the surface of the semiconductor substrate. 17. The method as claimed in claim 8 , further comprising: numerically expressing a signal to noise ratio (S/N ratio) of a result obtained by the predetermined transform.
Testing or measuring during manufacture or treatment of wafers, substrates or devices · CPC title
by using diffraction of the radiation by the materials, e.g. for investigating crystal structure; by using scattering of the radiation by the materials, e.g. for investigating non-crystalline materials; by using reflection of the radiation by the materials · CPC title
for measuring thickness · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.