IP Library Granted Patent US 9,874,531
Granted Patent B2
US 9,874,531 · App. 14/712,917 · Granted Jan 23, 2018

X-ray method for the measurement, characterization, and analysis of periodic structures

Inventors: Wenbing Yun (Walnut Creek, CA); Sylvia Jia Yun Lewis (San Francisco, CA); Janos Kirz (Berkeley, CA)
Assignee: Sigray, Inc.
G01N23/20075A61B6/4007A61B6/4291A61B6/484A61B6/508G01N23/201G21K1/02H01J35/08G21K2207/005H01J2235/086
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Quick Facts
Patent No.
US 9,874,531
App. No.
14/712,917
Granted
Jan 23, 2018
Kind
B2
Abstract

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.

Claims (63)

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.

Assignments (1)
NUNC PRO TUNC ASSIGNMENT Recorded Oct 9, 2015
From: YUN, WENBING; LEWIS, SYLVIA JIA YUN; KIRZ, JANOS
To: SIGRAY, INC.
Reel/Frame 036767/0536 →
Continuity (11)
Continuation In Part 14700137 · Apr 29, 2015
Continuation In Part 14527523 · Oct 29, 2014
Provisional Application 61987106 · May 1, 2014
Provisional Application 61989743 · May 7, 2014
Provisional Application 61991889 · May 12, 2014
Provisional Application 61993811 · May 15, 2014
Provisional Application 61898019 · Oct 31, 2013
Provisional Application 61901361 · Nov 7, 2013
Provisional Application 61981098 · Apr 17, 2014
Provisional Application 61993792 · May 15, 2014
Related Publication 20150260663A1 · Sep 17, 2015