Localization of an object in a turbid medium using radiation of different wavelengths

• US 5,941,827 A
• Filed: 12/01/1997
• Issued: 08/24/1999
• Est. Priority Date: 04/02/1996
• Status: Expired due to Fees

• Current Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Original Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Inventors: Papaioannou, Dimitrius
• Primary Examiner(s): Kamm, William E.
• Assistant Examiner(s): SHAW, SHAWNA JEANNINE
• Application Number:
  US08/973,135
• Time in Patent Office: 631 Days
• Field of Search: 600/473, 600/476, 600/310, 600/475, 600/477, 356/432, 356/433, 356/434, 356/435, 356/345, 356/349, 250/330, 250/332, 250/339.01
• US Class Current: 600/473
• CPC Class Codes: A61B 5/0091 for mammography
• CPC Class Codes: A61B 5/4312 Breast evaluation or disorder diagnosis A61B5/0091 takes precedence

Abstract

A system for detecting an object (1) in a turbid medium (2) comprises a radiation source (3) for irradiating the turbid medium with radiation components of different wavelengths, preferably in the range between 600 nm and 1 μm. The radiation components are amplitude modulated, preferably in anti-phase. The radiation form the turbid medium is received by a photodetector (4) which is sensitive for the different wavelengths. Inhomogeneities in the turbid medium influence the superposition of the amplitude modulations at the photodetector, so that the photodetector outputs a signal that contains information on the presence and/or location of an object in the turbid medium.

Claims

1. A system for detecting an object present in a turbid medium comprising:

a radiation source for irradiating a turbid medium with radiation comprising radiation components of a first and a second wavelength, wherein the radiation components of the first and second wavelength are modulated with amplitude modulation at substantially equal modulation frequencies, the amplitude modulation of the radiation components of the first and second wavelength having a predetermined and fixed phase difference, and

a photodetector arranged to detect an intensity signal of radiation emerging from the turbid medium.

2. A system as claimed in claim 1, wherein the predetermined phase difference is substantially equal to 180°

.

3. A system as claimed in claim 1, wherein the photodetector has a sensitivity wavelength range encompassing the first and second wavelength.

4. A system as claimed in claim 1, wherein the amplitude modulation is substantially a square wave modulation.

5. A system as claimed in claim 1, further comprising

a compression mechanism for compressing the turbid medium, and

a displacement device for moving a radiation emitting face with respect to the turbid medium, and wherein the photodetector has a radiation receiving portion which is arranged opposite said radiation emitting face.

6. A system as claimed in claim 1, comprising a source fiber arranged for guiding radiation from the radiation source to the turbid medium, and a plurality of detector fibers arranged for guiding radiation to the photodetector from respective positions of the turbid medium.

7. A system as claimed in claim 6, wherein the photodetector is a charge-coupled device (CCD).

8. A system as claimed in claim 1, wherein the photodetector comprises a read-out circuit that is arranged to operate synchronously with the amplitude modulation.

9. A system as claimed in claim 8, wherein the read-out circuit comprises a subtraction unit.

11. A system as claimed in claim 2, wherein the photodetector has a sensitivity wavelength range encompassing the first and second wavelength.

12. A system as claimed in claim 2, wherein the amplitude modulation is substantially a square wave modulation.

13. A system as claimed in claim 3, wherein the amplitude modulation is substantially a square wave modulation.

14. The system of claim 1 wherein the amplitude modulation and the predetermined phase difference are such that (I) in the case no object is present in the turbid medium the total of the detected intensities has practically only a DC component, and (ii) in the case an object is present in the turbid medium the total of the detected intensities comprises an AC component at the amplitude modulation frequency.

15. The system of claim 1 wherein both radiation components are incident on the turbid medium at a same position.

16. The system of claim 1 further comprising a signal processing unit for processing the detected intensity signal and its deviation from a predetermined intensity signal into an image signal.

17. The system of claim 16 wherein the amplitude modulation and the predetermined phase difference are such that the predetermined intensity signal has practically only a DC component.

10. A method for detecting an object in a turbid medium comprising:

irradiating a turbid medium with radiation components having a first and a second wavelength, respectively, wherein the radiation components of the first and second wavelength are modulated with amplitude modulation at substantially equal modulation frequencies, the amplitude modulation of the radiation components of the first and second wavelength having a predetermined and fixed phase difference, and

detecting an intensity signal of radiation emerging from the turbid medium,

determining the presence of an object when the detected intensity signal deviates from a predetermined intensity signal.

18. The method of claim 10 further comprising a step of selecting the amplitude modulation and the predetermined phase difference so that the predetermined intensity signal has practically only a DC component, and wherein the step of determining determines the presence of an object in the turbid medium when the detected intensity signal comprises an AC component at the amplitude modulation frequency.

19. The method of claim 10 wherein both radiation components are incident on the turbid medium at a same position.

20. The method of claim 10 wherein the predetermined phase difference is substantially equal to 180°

.

21. The method of claim 10 wherein the amplitude modulation is substantially a square wave modulation.