Imaging through scattering media with high signal to noise ratio and resolution

Patent metadata

Field	Value
Publication number	US-2016356746-A1
Application number	US-201414913958-A
Country	US
Kind code	A1
Filing date	Aug 26, 2014
Priority date	Aug 26, 2013
Publication date	Dec 8, 2016
Grant date	—

Abstract

Systems and methods are disclosed to enhance three-dimensional photoacoustic imaging behind, through, or inside a scattering material. Embodiments of the invention can increase the optical fluence in an ultrasound transducer focus and/or enhance the optical intensity using wavefront shaping before the scatterer. The photoacoustic signal induced by an object placed behind the scattering medium can serve as feedback to optimize the wavefront, enabling one order of magnitude enhancement of the photoacoustic amplitude. Using the enhanced optical intensity, the object can be scanned in two dimensions and/or a spot can be scanned by re-optimizing the wavefront before post-processing of the data to reconstruct the image. The temporal photoacoustic signal provides information to reconstruct the third-dimensional information.

First claim

That which is claimed:

1 . A method comprising:
illuminating a sample through a scatterer using a light source and at least one spatial light modulator; receiving a photoacoustic signal from a transducer; determining an optimized wavefront from the photoacoustic signal; modifying a configuration of the spatial light modulator based on the optimized wavefront; and illuminating the sample through the scatterer using the light source and the spatial light modulator with the modified configuration.

2 . The method according to claim 1 , wherein the modified configuration produces an optical focus that is smaller than the acoustic focus.

3 . The method according to claim 1 , wherein the spatial light modulator is an optical element selected from the group consisting of one or more spatial light modulators, phase-only spatial light modulators, intensity-only spatial light modulators, prism arrays, diffractive elements, diffusers, holograms, Dammann gratings, liquid crystal spatial light modulators, phase masks, amplitude masks, acousto-optic modulator, acousto-optic deflector, and phase/amplitude masks.

4 . The method according to claim 1 , wherein the determining the optimized wavefront includes using an optimization algorithm to determine the optimized wavefront.

5 . The method according to claim 1 , further comprising scanning the sample, moving the sample with fluid, scanning a focus of the transducer, and/or scanning a focus of the light source.

6 . An imaging system comprising:
a pulsed light source; an optical system configured to direct light from the light source toward a sample through a scatterer; one or more acoustic transducers configured to record acoustic signals from the sample; and a controller coupled with at least a portion of the optical system and the one or more acoustic transducers, wherein the controller is configured to modify the phase and/or amplitude of the light directed by the optical system through the wall using data from the one or more acoustic transducers.

7 . The imaging system according to claim 6 , wherein the one or more acoustic transducers is disposed outside the wall such that the acoustic signals pass through the wall.

8 . The imaging system according to claim 6 , wherein the optical system comprises a spatial light modulator, one or more lenses and/or an objective lens.

9 . The imaging system according to claim 6 , wherein the optical system includes an optical element selected from the group consisting of one or more spatial light modulators, phase-only spatial light modulators, intensity-only spatial light modulators, prism arrays, diffractive elements, diffusers, holograms, Dammann gratings, liquid crystal spatial light modulators, phase masks, amplitude masks, acousto-optic modulator, acousto-optic deflector, and phase/amplitude masks.

10 . The imaging system according to claim 6 , wherein the controller is configured to use a optimization algorithm based on data from the one or more acoustic transducers modify the phase and/or amplitude of the light.

11 . The imaging system according to claim 6 , wherein the controller is configured to use spatially varying feedback to optimize an optical wavefront from the optical system such that light is enhanced and focused to a single speckle behind the wall.

12 . The imaging system according to claim 6 , wherein the controller is configured to increase the depth of optical resolution photoacoustic microscopy by providing high intensity optical focus.

13 . The imaging system according to claim 6 , wherein the controller is configured to scan the sample, scan a focus of the transducer, and/or scan a focus of the light source.

14 . A method comprising:
illuminating a sample inside a scatterer with a plurality of optical wavefronts modulated by a spatial light modulator, each of the plurality of optical wavefronts produced modulated by the spatial light modulator using one of a plurality SLM matrices selected from a population of SLM matrices; receiving a plurality of electric signals from a transducer, wherein each of the plurality of electric signals correspond with a photoacoustic signal received at the transducer for each of the plurality of illuminations; determining an optimum SLM matrix from the population of SLM matrices based on the plurality of electric signals; and returning an image of the sample corresponding with illumination of the sample with the optimum SLM matrix.

15 . The method according to claim 14 , wherein the determining an optimum SLM matrix from the population of SLM matrices comprises determining an optimum SLM matrix from the population of SLM matrices using a genetic algorithm.

16 . The method according to claim 14 , wherein the determining an optimum SLM matrix from the population of SLM matrices based on the plurality of electric signals comprises determining an optimum SLM matrix from the population of SLM matrices based on the peak-to-peak voltage of the plurality of electric signals.

17 . The method according to claim 14 , wherein the optimum SLM matrix produces an optical focus at or near the sample that is smaller than the acoustic focus.

18 . The method according to claim 14 , further comprising:
scanning the sample in the x-y plane; and repeating the method.

19 . The method according to claim 14 , further comprising:
moving the focus of the transducer; repeating the method.

20 . The method according to claim 14 , wherein the image is a three-dimensional image of the sample.

21 . The method according to claim 14 , wherein the plurality of electric signals comprise a plurality of acoustic signals, wherein the acoustic signals are enhanced by nonlinear effects in the sample.

Assignees

• Univ Colorado Regents

Inventors

• Piestun Rafael
• Ju Hengyi
• Dove Jacob
• Caravacca-Aguirre Antonio Miguel
• Murray Todd
• Conkey Donald

Classifications

• G01N2201/0675

  SLM · CPC title

• G01N2021/1706

  in solids · CPC title

• G01N21/1702

  with opto-acoustic detection, e.g. for gases or analysing solids · CPC title

• A61B5/0095

  by applying light and detecting acoustic waves, i.e. photoacoustic measurements · CPC title

• G01N29/2418 Primary

  using optoacoustic interaction with the material, e.g. laser radiation, photoacoustics (photoacoustic cells G01N21/1702; measuring characteristics of vibrations by using radiation-sensitive means G01H9/00; acousto-optical conversion techniques for short-range imaging G01S15/8965; sound-producing devices using laser bundle G10K15/046) · CPC title