IP Library Granted Patent US 8,695,109
Granted Patent B2
US 8,695,109 · App. 13/270,700 · Granted Apr 8, 2014

Method and system for near-field optical imaging

Inventors: John C. Schotland (Ann Arbor, MI); Alexander A. Govyadinov (Warrington, PA); George Y. Panasyuk (Fairborn, OH)
Assignee: The Trustees Of The University Of Pennsylvania
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Quick Facts
Patent No.
US 8,695,109
App. No.
13/270,700
Granted
Apr 8, 2014
Kind
B2
Abstract

A system and method for optically imaging a sample. The method and system uses a controlled scatterer of light positioned in the near field of a sample. The extinguished power from an incident field, which illuminates both the sample and the controlled scatterer, is then measured as a function of the controlled scatterer position and is used to mathematically reconstruct an image of the sample.

Claims (34)

1. A method for optical imaging comprising:

providing a sample;

introducing a controlled scatterer into a near field of the sample whereby changing a position of the controlled scatterer changes a pattern of illumination of said sample;

providing an incident field to illuminate said sample;

measuring extinguished power from the incident field as a function of a position of the controlled scatterer; and

imaging the sample by using the measured extinguished power.

2. The method of claim 1 , further comprising controlling the position of the controlled scatterer.

3. The method of claim 1 , wherein the controlled scatterer is a nano-particle, a scanning near-field tip, an atomic force microscope tip, a near-field scanning optical microscopy tip, or a bow-tie antenna.

4. The method of claim 1 , wherein providing the incident field comprises providing incident light from a monochromatic illumination source having a wavelength λ or a non-monochromatic light source that outputs non-monochromatic light through a filter to obtain wavelength λ.

5. The method of claim 4 , wherein measuring the power comprises measuring electromagnetic power at wavelength λ.

6. The method of claim 1 , further comprising oscillating the controlled scatterer.

7. The method of claim 1 , wherein the step of imaging comprises reconstructing a complex valued susceptibility of the sample with sub-wavelength resolution in three dimensions from the measured extinguished power obtained for different positions of the controlled scatterer distributed on a three-dimensional grid.

8. The method of claim 1 , wherein the step of imaging obtains a sub-wavelength resolution.

9. A system for optical imaging comprising:

a controlled scatterer that is introduced into a near field of a sample and adapted such that changing a position of the controlled scatterer changes a pattern of illumination of said sample;

incident light providing means for providing an incident field that illuminates said sample;

power measuring means for measuring power extinguished from the incident field as a function of a position of the controlled scatterer; and

imaging means for imaging the sample using the measured extinguished power extinguished from the incident field.

10. The system of claim 9 , further comprising means for controlling the position of the controlled scatterer.

11. The system of claim 9 , wherein the controlled scatterer is a nano-particle, an atomic force microscope tip, or a bow-tie antenna.

12. The system of claim 9 , wherein the controlled scatterer is a near-field microscope tip or a near-field scanning optical microscopy tip.

13. The system of claim 9 , wherein the incident light providing means is a monochromatic illumination source having a wavelength λ or a non-monochromatic light source that outputs non-monochromatic light through a filter to obtain wavelength λ.

14. The system of claim 13 , wherein the power measuring means is a photodiode or an avalanche photodiode adapted to measure electromagnetic power at wavelength λ.

15. The system of claim 9 , wherein the controlled scatterer is an oscillating controlled scatterer.

16. The system of claim 9 , wherein the imaging means reconstructs a complex valued susceptibility of the sample with sub-wavelength resolution in three dimensions from measured extinguished power obtained for different positions of the controlled scatterer distributed on a three-dimensional grid.

17. The system of claim 9 , wherein the imaging means obtains a sub-wavelength resolution.

18. A method of optical imaging comprising:

providing a sample;

introducing a controlled scatterer into a near field of the sample whereby changing a position of the controlled scatterer changes a pattern of illumination of said sample;

oscillating the controlled scatterer;

measuring extinguished power obtained for different positions of the controlled scatterer; and

reconstructing a complex valued susceptibility of the sample with sub-wavelength resolution in three dimensions from the measured extinguished power obtained for different positions of the controlled scatterer distributed on a three-dimensional grid outside a region of the sample.

19. The method of claim 18 , wherein the controlled scatterer is a nano-particle, an atomic force microscope tip, or a bow-tie antenna.

20. The method of claim 18 , wherein the controlled scatterer is a near-field microscope tip or a scanning near-field optical microscope tip.

Assignments (2)
CONFIRMATORY LICENSE Recorded Jun 17, 2015
From: UNIVERSITY OF PENNSYLVANIA
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 035938/0306 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 6, 2012
From: SCHOTLAND, JOHN C.; GOVYADINOV, ALEXANDER A.; PANASYUK, GEORGE Y.
To: THE TRUSTEES OF THE UNIVERSITY OF PENNSYLVANIA
Reel/Frame 027494/0421 →
Continuity (2)
Provisional Application 61392619 · Oct 13, 2010
Related Publication 20120096601A1 · Apr 19, 2012