IP Library Granted Patent US 7,960,707
Granted Patent B2
US 7,960,707 · App. 10/577,527 · Granted Jun 14, 2011

Time-domain method and apparatus for determining the depth and concentration of a fluorophore in a turbid medium

View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 7,960,707
App. No.
10/577,527
Granted
Jun 14, 2011
Kind
B2
Abstract

Methods and apparatuses for determining the depth and concentration of fluorophores in a turbid medium are disclosed. The method advantageously provides for a rapid estimation of the depth of the fluorophore using characteristics of a temporal point spread function. The concentration of the fluorophore can be determined using the method of the present invention by combining a calculated depth of the fluorophore with a measurement of the intensity of the emitted fluorescence. The intensity can be accurately measured by the apparatus disclosed herein which combine back-reflection and trans-illumination geometries for the source of light injecting and detection.

Claims (48)

1. An apparatus for determining depth and concentration of a fluorophore in a turbid medium comprised within an object, said apparatus comprising:

a light source, optically coupled to a source channel and said object, to inject light in said object at a desired point and excitation wavelength;

at least one detector channel, optically coupled to a photon detector and said object, in a back reflection geometry relative to said source channel, to acquire at least one temporal point spread function from a desired point of said object;

a means for spatially positioning said object relative to said channels;

a depth calculator for calculating the depth of the fluorophore on the basis of a time t max corresponding to a maximum of the temporal point spread function; and

a concentration calculator for calculating the concentration of the fluorophore based on the depth and on an intensity of the temporal point spread function.

2. The apparatus as claimed in claim 1 wherein said source and detector channels are in a configuration selected from contact and free-space optic.

3. The apparatus as claimed in claim 1 wherein said channels comprise optical coupling means selected from, mirrors, optic fibers.

4. The apparatus as claimed in claim 1 wherein said channels are mounted in a fixed position relative to one another.

5. The apparatus as claimed in claim 1 wherein said channels are mounted on a gantry that is moveable relative to said object.

6. The apparatus as claimed in claim 1 wherein said channels are independently moveable.

7. The apparatus as claimed in claim 1 wherein said object is placed on a platform transparent to an emission wavelength.

8. The apparatus as claimed in claim 7 wherein said platform is moveable relative to said channels.

9. The apparatus as claimed in claim 1 wherein said light source is a multiwavelength light source.

10. The apparatus as claimed in claim 1 wherein detection is effected using a plurality of source/detector configurations.

11. The apparatus as claimed in claim 1 comprising a plurality of detector channels.

12. The apparatus as claimed in claim 1 comprising a plurality of source channels.

13. The apparatus as claimed in claim 1 further comprising wavelength selection means between said source and said object for selecting one or more excitation wavelength.

14. The apparatus as claimed in claim 1 further comprising wavelength selection means between said object and said detector for selecting one or more emission wavelengths.

15. The apparatus as claimed in claim 1 wherein said detector in a trans-illumination geometry operates in time domain, frequency domain or continuous wave mode.

16. The apparatus as claimed in claim 1 further including a second detector channel in a trans-illumination geometry relative to said source channel, to measure an emission intensity of said fluorophore.

17. The apparatus as claimed in claim 1 , wherein a relative concentration of the fluorophore is calculated as:

Conc

.

Re

lative

=

Id

2

2

d

μ

α

/

D

where:

Conc. Relatlive is the relative concentration of the fluorophore;

I is the intensity of the temporal point spread function;

d is the depth of the fluorophore;

μ a is an optical absorption coefficient of the turbid medium; and

D is an optical diffusion coefficient of the turbid medium.

Assignments (5)
CHANGE OF NAME Recorded Jun 21, 2011
From: DORSKY WORLDWIDE CORP.
To: SOFTSCAN HEALTHCARE GROUP LTD.
Reel/Frame 026469/0916 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jun 20, 2011
From: ART ADVANCED RESEARCH TECHNOLOGIES INC.
To: DORSKY WORLDWIDE CORP.
Reel/Frame 026466/0001 →
CHANGE OF NAME Recorded Jun 20, 2011
From: NEW ART ADVANCED RESEARCH TECHNOLOGIES INC.
To: ART ADVANCED RESEARCH TECHNOLOGIES INC.
Reel/Frame 026479/0052 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 8, 2006
From: ART ADVANCED RESEARCH TECHNOLOGIES INC.
To: NEW ART ADVANCED RESEARCH TECHNOLOGIES INC.
Reel/Frame 018597/0320 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Apr 28, 2006
From: HALL, DAVID; MA, GUOBIN; LESAGE, FREDERIC; GALLANT, PASCAL
To: ART, ADVANCED RESEARCH TECHNOLOGIES, INC.
Reel/Frame 017878/0059 →