Optical coherence tomography systems and methods with dispersion compensation

1. A system, comprising:

a swept laser light source configured to generate laser light having a frequency swept across a frequency bandwidth as a function of time;

a sample path configured to direct a first portion of the laser light to an eye as a probe beam and to receive a returned portion of the probe beam from the eye, returned by at least one of reflection and scattering;

a reference path for passing therethrough a second portion of the laser light, the reference path having a defined optical path length;

a wavefront aberrometer;

a corneal topographer;

an iris imaging system;

a structure having an aperture therethrough; and

a detector configured to receive the returned portion of the probe beam from the eye and the second portion of the laser light from the swept laser light source which passed through the reference path, and in response thereto to output an optical coherence tomography (OCT) signal having peaks whose relative timing represents the depths of various reflection and scattered surfaces within the eye,

wherein the reference path includes a first optical fiber of a first type having a first length, in series with a second optical fiber of a second type which is different than the first type and having a second length, wherein dispersion characteristics of the first optical fiber and the second optical fiber are significantly different than each other,

wherein the sample path directs the probe beam to the eye through the aperture, and

wherein all of the wavefront aberrometer, the corneal topographer, and the iris imaging system direct light to the eye through the aperture.

2. The system of claim 1 , wherein the sample path includes a Z-axis telescope configured to focus the probe beam at a desired depth within the eye.

3. The system of claim 1 , wherein the sample path includes a scanner configured to scan the probe beam in X and Y directions to span an X-Y OCT measurement space in the eye.

4. A system, comprising:

a swept laser light source configured to generate laser light having a frequency swept across a frequency bandwidth as a function of time;

a sample path configured to direct a first portion of the laser light to an eye as a probe beam and to receive a returned portion of the probe beam from the eye, returned by at least one of reflection and scattering;

a reference path for passing therethrough a second portion of the laser light, the reference path having a defined optical path length; and

a detector configured to receive the returned portion of the probe beam from the eye and the second portion of the laser light from the swept laser light source which passed through the reference path, and in response thereto to output an optical coherence tomography (OCT) signal having peaks whose relative timing represents the depths of various reflection and scattered surfaces within the eye,

wherein the reference path includes a first optical fiber of a first type having a first length, in series with a second optical fiber of a second type which is different than the first type and having a second length, wherein dispersion characteristics of the first optical fiber and the second optical fiber are significantly different than each other, and a third optical fiber of a third type having a third length, in series with the first and second optical fibers, and wherein dispersion characteristics of the third optical fiber are significantly different than the dispersion characteristics of the first optical fiber and than the second optical fiber.

5. The system of claim 4 , wherein the first optical fiber and the second optical fiber have substantially different group velocity dispersion constants than each other for at least one frequency within the bandwidth of the swept laser light source.

6. The system of claim 4 , wherein a total group delay dispersion of a first portion of the laser light passing through the sample path and a total group delay dispersion of the second portion of the laser light passing through the reference path offset each other at the detector.

7. The system of claim 4 , wherein the first optical fiber is an HI-1060 type optical fiber and the second optical fiber is an SM-980 type optical fiber.

8. The system of claim 4 , wherein the first optical fiber, the second optical fiber and the third optical fiber all have substantially different group velocity dispersion constants than each other for at least one frequency within the bandwidth of the swept laser light source.

9. The system of claim 8 , wherein a total group delay dispersion of a first portion of the laser light passing through the sample path and a total group delay dispersion of the second portion of the laser light passing through the reference path offset each other at the detector.

10. A method, comprising:

sweeping a frequency of a laser light source across a frequency bandwidth as a function of time to generate laser light whose frequency varies as a function of time;

directing a first portion of the laser light to an eye as a probe beam, and receiving a returned portion of the probe beam from the eye, returned by at least one of reflection and scattering via a sample path of an optical coherence tomography (OCT) interferometer;

passing a second portion of the laser light through a reference path of the OCT interferometer, the reference path having a defined optical path length; and

receiving at a detector the returned portion of the probe beam from the eye and the second portion of the laser light from the swept laser light source which passed through the reference path, and in response thereto outputting an OCT signal having peaks whose relative timing represents the depths of various reflection and scattered surfaces within the eye,

wherein the reference path includes a first optical fiber of a first type having a first length, in series with a second optical fiber of a second type which is different than the first type and having a second length, and a third optical fiber of a third type having a third length, in series with the first and second optical fibers, wherein dispersion characteristics of the first optical fiber and the second optical fiber are significantly different than each other, and wherein dispersion characteristics of the third optical fiber are significantly different than the dispersion characteristics of the first optical fiber and than the second optical fiber.

11. The method of claim 10 , wherein the first optical fiber and the second optical fiber have substantially different group velocity dispersion constants than each other for at least one frequency within the bandwidth of the swept laser light source.

12. The method of claim 10 , wherein a total group delay dispersion of a first portion of the laser light passing through the sample path and a total group delay dispersion of the second portion of the laser light passing through the reference path offset each other at the detector.

13. The method of claim 10 , wherein the first optical fiber is an HI-1060 type optical fiber and the second optical fiber is an SM-980 type optical fiber.

14. The method of claim 10 , wherein the first optical fiber, the second optical fiber and the third optical fiber all have substantially different group velocity dispersion constants than each other for at least one frequency within the bandwidth of the swept laser light source.

15. The method of claim 14 , wherein a total group delay dispersion of a first portion of the laser light passing through the sample path and a total group delay dispersion of the second portion of the laser light passing through the reference path offset each other at the detector.

16. The method of claim 10 , further comprising focusing the probe beam at a desired depth within the eye via a Z-axis telescope.

17. The method of claim 10 , scanning the probe beam in X and Y directions to span an X-Y OCT measurement space in the eye.