Optical inspection system and method including accounting for variations of optical path length within a sample

• US 10,274,426 B2
• Filed: 09/27/2017
• Issued: 04/30/2019
• Est. Priority Date: 12/23/2014
• Status: Active Grant

• Current Assignee: Apple Inc.
• Original Assignee: Apple Inc.
• Inventors: Arbore, Mark Alan, Terrel, Matthew A.
• Primary Examiner(s): Decenzo, Shawn
• Assistant Examiner(s): Underwood, Jarreas C
• Application Number:
  US15/717,651
• Publication Number:
  US 20180017491A1
• Time in Patent Office: 580 Days
• Field of Search: None
• CPC Class Codes: G01N 2021/1782 In-depth resolution
• CPC Class Codes: G01N 2021/4709 Backscatter
• CPC Class Codes: G01N 2021/4711 Multiangle measurement
• CPC Class Codes: G01N 21/49 within a body or fluid
• CPC Class Codes: G01N 21/59 Transmissivity G01N21/25 takes precedence
• CPC Class Codes: G01N 2201/066 Modifiable path; multiple paths in one sample
• CPC Class Codes: G01N 2201/0691 Modulated (not pulsed supply)
• CPC Class Codes: G01N 2201/0696 Pulsed
• CPC Class Codes: G01N 2201/12 Circuits of general importance; Signal processing

Abstract

An illuminator/collector assembly can deliver incident light to a sample and collect return light returning from the sample. A sensor can measure ray intensities as a function of ray position and ray angle for the collected return light. A ray selector can select a first subset of rays from the collected return light at the sensor that meet a first selection criterion. In some examples, the ray selector can aggregate ray intensities into bins, each bin corresponding to rays in the collected return light that traverse within the sample an estimated optical path length within a respective range of optical path lengths. A characterizer can determine a physical property of the sample, such as absorptivity, based on the ray intensities, ray positions, and ray angles for the first subset of rays. Accounting for variations in optical path length traversed within the sample can improve accuracy.

Claims

1. An optical inspection system for optically characterizing a sample, comprising:

an illuminator/collector assembly configured to deliver multiple incident light rays to the sample and collect multiple return light rays returning from the sample;

a sensor that includes a plurality of zones, each zone measuring ray intensity as a function of ray position and ray angle for the respective collected return light rays;

a ray selector configured to select a first subset of light rays from the collected multiple return light rays at the sensor that meet a first selection criterion, wherein the first selection criterion is associated with a single scattering event; and

a computer including a characterizer configured to determine a physical property of the sample based on the ray intensities, ray positions, and ray angles for the first subset of light rays.

2. The optical inspection system of claim 1, wherein the first selection criterion comprises a first range of estimated path lengths traversed within the sample, a first range of path length distributions traversed within the sample, or a first range of estimated ray penetration depths traversed within the sample.

3. The optical inspection system of claim 1, wherein the ray selector is further configured to select a second subset of light rays from the collected return light rays that meet a second selection criterion;

and

wherein the characterizer is configured to determine the physical property based on the ray intensities, ray positions, and ray angles for the first subset of light rays and the second subset of light rays.

4. The optical inspection system of claim 3, wherein the first selection criterion comprises a first range of estimated path lengths or path length distributions, and the second selection criterion comprises a second range of estimated path lengths or path length distributions.

5. The optical inspection system of claim 3,

wherein the first selection criterion comprises traversing within the sample an estimated optical path length within a first range of optical path lengths,

wherein the second selection criterion comprises traversing within the sample an estimated optical path length within a second range of optical path lengths, and

wherein the second range of optical path lengths does not overlap the first range of optical path lengths.

6. The optical inspection system of claim 5,

wherein the ray intensities for the first subset of light rays are aggregated into a first binned signal,

wherein the ray intensities for the second subset of light rays are aggregated into a second binned signal, and

wherein the characterizer determines the physical property of the sample based on the first binned signal and second binned signal.

7. The optical inspection system of claim 6, wherein the ray selector includes first pixels of the sensor and second pixels of the sensor, the first pixels and the second pixels each having a shape and size configured for measuring the ray intensities for light rays within the first subset of light rays and the second subsets of light rays, respectively,

wherein the first pixels and the second pixels are configured to respectively output the first binned signal and the second binned signal.

8. The optical inspection system of claim 6, wherein the ray selector is further configured to:

receive signals from corresponding pixels of the sensor,

average a first subset of the signals to form the first binned signal, and

average a second subset of the signals to form the second binned signal.

9. The optical inspection system of claim 8, wherein the first and second subsets of the signals are averaged in hardware.

10. The optical inspection system of claim 8, wherein the first and second subsets of the signals are averaged in software.

11. The optical inspection system of claim 6, wherein the characterizer is further configured to:

fit the first and second binned signals to a Beer'"'"'s Law calculation, and

determine an absorptivity of the sample based on the Beer'"'"'s Law calculation.

12. The optical inspection system of claim 11, wherein the characterizer weights the first and second binned signals differently when determining the absorptivity of the sample.

13. The optical inspection system of claim 3, wherein the computer is configured to perform a first operation set using the first subset of light rays and perform a second operation set using the second subset of light rays in determining the physical property of the sample.

14. The optical inspection system of claim 1, wherein the sensor includes a plurality of microlenses and a detector positioned at a focal plane of the plurality of microlenses.

15. The optical inspection system of claim 14, further comprising a mask disposed between the plurality of microlenses and the detector, the mask including at least one blocking portion configured to block specified light rays in the collected return light rays.

16. The optical inspection system of claim 1, wherein the computer is configured to:

aggregate the ray intensities into binned signals, each binned signal corresponding to light rays in the collected return light rays that traverse within the sample an estimated optical path length within a respective range of optical path lengths,

wherein the characterizer is further configured to determine the physical property of the sample based on the binned signals.

17. The optical inspection system of claim 16, wherein the computer is further configured to:

fit the binned signals to a Beer'"'"'s Law calculation; and

determine an absorptivity of the sample based on the Beer'"'"'s Law calculation.

18. A method for optically characterizing a sample, comprising:

illuminating the sample with incident light using an illuminator;

collecting multiple return light rays returning from the sample;

measuring ray intensities as a function of ray position and ray angle for the respective collected return light rays using a sensor;

aggregating at least some of the ray intensities into a plurality of binned signals; and

determining a physical property of the sample based on the plurality of binned signals.

19. The method of claim 18, wherein each binned signal corresponds to the collected return light rays that traverse within the sample an estimated optical path length within a respective range of optical path lengths.

20. The method of claim 18, further comprising:

fitting the plurality of binned signals to a Beer'"'"'s Law calculation; and

determining an absorptivity of the sample based on the Beer'"'"'s Law calculation.