Conoscopic system for real-time corneal topography

• US 5,909,270 A
• Filed: 05/09/1997
• Issued: 06/01/1999
• Est. Priority Date: 05/10/1996
• Status: Expired due to Fees

• Current Assignee: California Institute of Technology
• Original Assignee: California Institute of Technology
• Inventors: Barbastathis, George, Psaltis, Demetri, Moser, Christophe
• Primary Examiner(s): MANUEL, GEORGE C
• Application Number:
  US08/854,212
• Time in Patent Office: 753 Days
• Field of Search: 351/208, 351/211, 351/212, 606/4, 606/5, 606/12, 606/10, 606/11
• US Class Current: 351/212
• CPC Class Codes: A61B 18/20 using laser
• CPC Class Codes: A61B 2018/00636 Sensing and controlling the application of energy
• CPC Class Codes: A61B 3/107 for determining the shape or measuring the curvature of the cornea
• CPC Class Codes: A61F 2009/00844 Feedback systems
• CPC Class Codes: A61F 2009/00855 Calibration of the laser system
• CPC Class Codes: A61F 2009/00872 Cornea
• CPC Class Codes: A61F 2009/00882 based on topography
• CPC Class Codes: A61F 2009/00897 Scanning mechanisms or algorithms
• CPC Class Codes: A61F 9/00804 Refractive treatments
• CPC Class Codes: G01B 11/255 for measuring radius of curvature measuring diameter G01B11/08
• CPC Class Codes: G03H 1/0493 Special holograms not otherwise provided for, e.g. conoscopic, referenceless holography

Abstract

A corneal topographer based on conoscopic holography with partially coherent illumination. Corneal topographic measurements can be accomplished at a processing rate higher than the standard video rate of 30 Hz. The conoscopic measurements can be used in an opto-electronic servo to control a photorefractive keratectomy system in real time for an improved accuracy in laser ablation of a corneal surface.

Claims

1. A conoscopic topographer for obtaining topographic measurements of a substantially spherical target surface at a fixed position, comprising:

an illuminating device, producing a collimated probe beam to said target surface, said probe beam being of a probe wavelength to which said target surface is reflective;

a collecting lens disposed relative to said target surface at a predetermined distance, for receiving a reflected probe beam including said target surface, said reflected probe beam encoded with surface phase information indicative of said target surface;

an optical birefringent medium having a single optic axis, positioned relative to said collecting lens and oriented to form a tilted angle between a direction of said reflected probe beam and said optic axis, said birefringent medium splitting said reflected probe beam into an ordinary probe beam and an extraordinary probe beam which interfere with each other to form a conoscopic interference pattern;

a first polarizer, located in an optical path of said probe beam between said light source and said birefringent medium, operating to polarize said reflected probe beam in a first polarization direction;

an imager, receiving said conoscopic interference pattern and producing an electrical representation of said interference pattern; and

a microprocessor, processing said electrical representation of said interference pattern to extract a topographic shape of said target surface.

2. A conoscopic topographer as in claim 1, wherein said illuminating device has a partially coherent light source.

3. A conoscopic topographer as in claim 1, wherein said illuminating device has an incoherent light source which has a pin hole at an output thereof.

4. A conoscopic topographer as in claim 1, wherein a ratio of an spectral linewidth of said probe beam to said probe wavelength is in a range from about 0.1% to about 1%.

5. A conoscopic topographer as in claim 1, wherein said collecting lens is so located relative to said target surface that a spacing between two adjacent fringes in said conoscopic interference pattern captured by said imager is maximized.

6. A conoscopic topographer as in claim 1, wherein said first polarization is selected relative to said optic axis of said birefringent medium so that said ordinary and extraordinary beams have a substantially identical power with respect to each other.

7. A conoscopic topographer as in claim 1, wherein said birefringent medium is a calcite crystal.

8. A conoscopic topographer as in claim 1, wherein said microprocessor extracts a direct phase information of said target surface from said interference pattern by using a Hermite polynomial expansion.

9. A photorefractive keratectomy surgical system, comprising:

a pulsed laser with a pulse repetition rate, producing an ablating laser beam at a wavelength at which a cornea is absorptive, said ablating laser beam having a fluence sufficient to ablate cornea tissue;

a beam steering system, located relative to said laser and guiding said ablating laser beam to a target eye which is at a fixed location;

a conoscopic topographer disposed relative to said fixed location, producing a probe beam to illuminate said target eye and receiving a reflected probe beam from said target eye, said topographer operable to measure a corneal shape of said target eye based on a conoscopic interference of said reflected probe beam; and

a system controller having a microprocessor, electrically connected to said laser, said beam steering system, and said topographer, said controller controlling said topographer to achieve a corneal topographic measurement of said target eye at a processing rate higher than said pulse repetition rate.

10. A system as in claim 9, wherein said ablating laser beam is controlled by said controller based on said corneal topographic measurement of said target eye.

11. A system as in claim 10, wherein said control of said ablating laser beam affects said fluence.

12. A system as in claim 10, wherein said control of said ablating laser beam affects a beam impact position on said target eye.

13. A system as in claim 9, wherein said topographer comprises:

a light source, producing said probe beam;

a collimator, displaced relative to said light source, operating to collimate said probe beam;

a collecting lens disposed relative to said target eye at a predetermined distance for receiving said reflected probe beam whose wavefront is encoded with corneal surface phase information;

an optical birefringent crystal having a single optic axis, positioned relative to said collecting lens and orientated to form a tilted angle between a direction of said reflected probe beam and said optic axis, said crystal splitting said reflected probe beam into an ordinary probe beam and an extraordinary probe beam which interfere with each other to form a conoscopic interference pattern;

a first polarizer, located in an optical path of said probe beam between said light source and said crystal, operating to make said reflected probe beam polarize in a first polarization direction;

an imager, receiving said conoscopic interference pattern and producing an electrical representation of said interference pattern; and

a second polarizer having a second polarization direction substantially orthogonal to said first polarization direction, located between said crystal and said imager, said second polarizer optimizing a detection of said imager.

14. A method for performing a topographic measurement of a spherical surface that is illuminated with a collimated probe beam, comprising:

imprinting a phase information of said spherical surface onto a reflected probe beam produced by said illumination of said probe beam;

generating a conoscopic interference pattern by using a uniaxial birefringent crystal to produce an ordinary beam and an extraordinary beam from said reflected probe beam;

determining a phase difference between said ordinary and extraordinary beams;

detecting a two-dimensional positioning representation of said spherical surface according to positioning coordinates in said conoscopic interference pattern;

extracting said phase information of said spherical surface based on said phase difference; and

determining a three-dimensional representation of said spherical surface.

15. A method as in claim 14, wherein said phase difference is determined by performing a phase shifting process which comprises:

obtaining a first intensity distribution of said conoscopic interference pattern at a first orientation of said crystal to produce a first phase difference between said ordinary and extraordinary beams;

obtaining a second intensity distribution of said conoscopic interference pattern at a second orientation of said crystal to produce a second phase difference between said ordinary and extraordinary beams, said second orientation being chosen so that said second phase difference is shifted by about π

/2 relative to said first phase difference;

obtaining a third intensity distribution of said conoscopic interference pattern at a third orientation of said crystal to produce a third phase difference between said ordinary and extraordinary beams, said third orientation being chosen so that said third phase difference is shifted by about n relative to said first phase difference; and

obtaining a fourth intensity distribution of said conoscopic interference pattern at a fourth orientation of said crystal to produce a fourth phase difference between said ordinary and extraordinary beams, said fourth orientation being chosen so that said fourth phase difference is shifted by about 3π

/2 relative to said first phase difference.

16. A method as in claim 14, wherein said extracting of said phase information from said phase difference comprises:

representing said phase difference by a first polynomial expansion of Hermite polynomials to a first number of terms;

representing said phase difference by a second polynomial expansion of Hermite polynomials to a second number of terms, said second number being smaller than said first number by one;

determining a second set of expansion coefficients of said second polynomial expansion by projecting said phase difference in a vector space formed by said Hermite polynomials; and

determining a first set of expansion coefficients of said first polynomial expansion based on said second set of expansion coefficients.