IP Library Granted Patent US 12,332,510
Granted Patent B2
US 12,332,510 · App. 17/271,135 · Granted Jun 17, 2025

Wavefront shaping with a 1D spatial light modulator

Inventors: Rafael Piestun (Boulder, CO); Omer Tzang (Boulder, CO); Eyal Niv (Boulder, CO)
Assignee: The Regents of the University of Colorado, a body corporate
G02F1/0121G02B27/48
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Quick Facts
Patent No.
US 12,332,510
App. No.
17/271,135
Granted
Jun 17, 2025
Kind
B2
Abstract

Controlling the propagation and interaction of light in complex media has sparked major interest. Unfortunately, spatial light modulation devices suffer from limited speed precluding real-time applications (e.g., imaging in live tissue). To address this problem, various embodiments use a phase-control technique to characterize complex media based on use of fast 1D spatial modulators and 1D-to-2D transformation performed by the same medium being analyzed. Some embodiments use a micro-electro-mechanical grating light valve (GLV) with 1088 degrees of freedom modulated at 350 KHz, enabling unprecedented high-speed wavefront measurements. Some embodiments continuously measure the transmission matrix, calculate the optimal wavefront and project a focus through various dynamic scattering samples in real-time, (e.g., within 2.4 ms per cycle). As such, some embodiments improve, by more than an order of magnitude, prior wavefront shaping modulation speed and open new opportunities for optical processing using 1D-to-2D transformations.

Claims (38)

1. A method comprising:

illuminating a light on a one-dimensional spatial light modulator along a line;

projecting, from the one-dimensional spatial light modulator, the light through a medium; and

generating a higher-dimensional field from the light transmitted through the medium.

2. The method of claim 1 , wherein the higher-dimensional field is a speckle field.

3. The method of claim 1 , wherein the higher-dimensional field is a two-dimensional field.

4. The method of claim 1 , wherein the higher-dimensional field is a spatio-temporal field.

5. The method of claim 1 , wherein the higher-dimensional field is a light pulse.

6. The method of claim 1 , further comprising:

capturing measurements of at least one property of the light transmitted through or back-scattered from the medium; and

instructing, based on the measurements of the at least one property of the light, the one-dimensional spatial light modulator to change a state to modulate the light.

7. The method of claim 6 , wherein the modulated light generates a wavefront that compensates some of the scattering or enhances energy delivery at a selected area or areas.

8. The method of claim 6 , wherein the modulated light generates a wavefront that generates a light distribution or pattern at a selected area or areas on either side of the medium.

9. The method of claim 8 , further comprising optimizing the wavefront for focusing through, inside, or back from the medium.

10. The method of claim 6 , wherein the measurements provide a transmission matrix of the medium.

11. The method of claim 6 , further comprising adaptively changing a phase or amplitude mask in response to changes in the medium identified via the measurements.

12. The method of claim 6 , wherein the measurements provide an optical phase to implement phase conjugation.

13. The method of claim 1 , further comprising transforming a one-dimensional optical field of the one-dimensional spatial light modulator into a two-dimensional optical field by imaging each pixel or segment of a one-dimensional field vector onto a pixel or segment of a two-dimensional field matrix.

14. The method of claim 13 , wherein the imaging is controlled via a lens system array, a micro lens system array, a diffractive optical element, or a computer generated hologram.

15. The method of claim 1 , wherein the medium is an optical fiber, tissue, a biological sample, a photosensitive material, turbulent air, smog, or a turbid material.

16. A method comprising:

illuminating, with a light source, a one-dimensional spatial light modulator along an illumination pattern;

capturing a measurement of at least one property of the illumination pattern transmitted through, reflected or backscattered from a medium;

transforming a one-dimensional optical field of the one-dimensional spatial light modulator into a higher-dimensional optical field;

calculating, based on the higher-dimensional optical field, an optimal wavefront that compensates for part of the scattering or enhances energy delivery at a selected area or areas; and

instructing, based on the at least one property, the one-dimensional spatial light modulator to apply a phase mask to the light and generate the optimal wavefront.

17. The method of claim 16 , wherein transforming the one-dimensional optical field of the one-dimensional spatial light modulator into a higher-dimensional optical field includes controlling a lens system array, controlling a micro lens system array, or generating a hologram.

18. The method of claim 16 , further comprising adaptively changing the phase mask in response to changes in the measurement of the at least one property of the light.

19. The method of claim 16 , further comprising implementing phase conjugation according to an optical phase provided by the measurement.

20. The method of claim 16 , further comprising displaying calculated patterns on the one-dimensional spatial light modulator.

21. The method of claim 16 , wherein the medium is an optical fiber, tissue, a biological sample, a photosensitive material, turbulent air, smog, or a turbid material.

22. The method of claim 16 , wherein the higher-dimensional optical field is a speckle field.

23. The method of claim 16 , wherein the higher-dimensional optical field is a two-dimensional field.

24. The method of claim 16 , wherein higher-dimensional optical field is a spatio-temporal field.

25. The method of claim 16 , wherein the higher-dimensional optical field is a light pulse.

26. The method of claim 16 , wherein the transforming comprises imaging each pixel or segment of a one-dimensional field vector onto a pixel or segment of a two-dimensional field matrix.

27. The method of claim 26 , further comprising controlling the imaging via a lens system array, a micro lens system array, a diffractive optical element, or a computer generated hologram.

28. The method of claim 16 , further comprising performing an optical transformation to rearrange one-dimensional degrees of freedom in a higher dimensional spatial configuration.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 2, 2024
From: PIESTUN, RAFAEL; TZANG, OMER; NIV, EYAL
To: THE REGENTS OF THE UNIVERSITY OF COLORADO, A BODY CORPORATE
Reel/Frame 065995/0626 →
CONFIRMATORY LICENSE Recorded Oct 4, 2021
From: UNIVERSITY OF COLORADO
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 057697/0733 →
Continuity (2)
Provisional Application 62722369 · Aug 24, 2018
Related Publication 20210255488A1 · Aug 19, 2021
References Cited (7)
US 8243355B2 · Kroll et al. · 2012 [cited by applicant]
US 20050147135A1 · Kurtz et al. · 2005 [cited by applicant]
US 20070070302A1 · Govorkov et al. · 2007 [cited by applicant]
US 20180107157A1 · Park · 2018 [cited by examiner]
WO 2017149064A1 · 2017 [cited by applicant]
Frostig, Hadas et al., “Focusing Light By Wavefront Shaping Through Disorder And Nonlinearity,” Optica, vol. 4, No. 9, pp. 1073-1079, Sep. 2017. [cited by applicant]
International Application No. PCT/US2019/048173, International Search Report & Written Opinion, 11 pages, Dec. 19, 2019. [cited by applicant]