Optical filter polarizer combination and laser apparatus incorporating this combination

• US 4,575,849 A
• Filed: 08/20/1984
• Issued: 03/11/1986
• Est. Priority Date: 12/20/1982
• Status: Expired due to Fees

• Current Assignee: General Electric Company
• Original Assignee: General Electric Company
• Inventors: Chun, Myung K.
• Primary Examiner(s): Scott, Jr., Leon
• Application Number:
  US06/642,571
• Time in Patent Office: 568 Days
• Field of Search: 372/98, 372/9, 372/106, 372/108, 372/105, 372/19, 372/20, 372/101, 350/403, 350/400, 350/416, 350/311, 350/317, 350/480, 350/380, 350/247, 350/505, 350/481, 353/20
• US Class Current: 372/9
• CPC Class Codes: H01S 2301/206 Top hat profile
• CPC Class Codes: H01S 3/08045 Single-mode emission
• CPC Class Codes: H01S 3/0805 by apertures, e.g. pin-holes or knife-edges
• CPC Class Codes: H01S 3/08054 Passive cavity elements acting on the polarization, e.g. a polarizer for branching or walk-off compensation quarter-wave plates in a Q-switch laser H01S3/1124, H01S3/115
• CPC Class Codes: H01S 3/08081 Unstable resonators
• CPC Class Codes: H01S 3/106 by controlling devices placed within the cavity H01S3/10076, H01S3/13 take precedence
• CPC Class Codes: H01S 3/115 using intracavity electro-optic devices

Abstract

The present invention deals with an optical filter polarizer combination providing a spacial transmission function to polarized incident light. When the light is in the form of a beam the combination may be used to reject extraneous light, or to modify the intensity profile of the beam as a radial or as a linear spacial function (orthogonal to the axis of the beam). The filter employs two lens elements of birefringent materials, with their crystal optical axes mutually orthogonal, and at 45° to the plane of polarization. Spherical lenses are employed for a radial spacial function and cylindrical lenses are employed for a linear spacial function. The combination is useful for mode selection in a stable laser oscillator, for beam quality improvement in a stable/unstable oscillator, and for fill factor enhancement in coupling energy from a laser oscillator to a laser amplifier.

Claims

1. A laser apparatus comprising:

first and second reflector means disposed in optical alignment for defining a resonant cavity therebetween;

an active laser medium for producing a beam of coherent electromagnetic radiation disposed between and in optical alignment with said first and second reflector means, and

optical mode control means disposed within said resonant cavity in optical alignment with said laser medium for shaping the optical transmission characteristics of said resonant cavity to maximize transmission of a desired transverse electromagnetic mode of electromagnetic radiation, said control means comprising;

first and second matching phase plates disposed in optical alignment with said laser medium;

said first phase plate comprising a bifringent crystal having a first flat major surface and a second concave major surface with a predetermined radius of curvature and a predetermined center thickness;

said second phase plate comprising a birefringent crystal having a first flat major surface and a second spherically convex major surface with a predetermined radius of curvature equal to the radius of curvature of said concave surface of said first phase plate and a predetermined center thickness equal to the center thickness of said first phase plate; and

a polarizing means disposed in optical alignment with said phase plates for ejecting radiation having a first polarization from said cavity and transmitting radiation having a second polarization orthogonal to said first polarization.

2. The invention of claim 1 wherein:

said laser medium comprises a face-pumped laser.

3. The invention of claim 2 wherein:

said first reflector means comprises a mirror being 100 percent reflective of radiation at the wavelength of said beam of electromagnetic radiation; and

said second reflector means comprises a mirror being partly reflective of radiation at the wavelength of said beam of electromagnetic radiation.

4. The invention of claim 3 wherein said matching phase plates comprise:

birefringent crystals having their primary optical axes disposed at a predetermined angular orientation.

5. The invention of claim 4 wherein:

said first and second birefringent crystal phase plates are so disposed that the concave surface of said first plate is in mating relationship with said convex surface of said second plate.

6. The invention of claim 5 wherein:

said first and second birefringent crystals comprise quartz.

7. The invention of claim 6 wherein:

said optical axes of said crystals are disposed in orthogonal relationship.

8. The invention of claim 7 further comprising:

Q-switch means comprising a Pockel'"'"'s cell disposed in optical alignment with said laser medium for controlling the build-up of a population inversion in said laser medium; and

an aperture plate disposed in optical alignment with said lasing medium.

9. The invention of claim 8 further comprising voltage control means for controlling the optical transmission of said Pockel'"'"'s cell;

said voltage control means comprising;

first switch means for causing the voltage applied to said Pockel'"'"'s cell to change with a first time constant to allow generation of a seed beam within said resonant cavity; and

second switch means for causing the voltage applied to said Pockel'"'"'s cell to change with a second time constant;

said second time constant being substantially shorter than said first time constant to produce a rapid depletion of the population inversion in the laser medium to produce an oscillating pulse within said resonant cavity.

10. The invention of claim 1 wherein said optical mode control means comprises:

first and second matching phase plates disposed in optical alignment with said laser medium;

said first phase plate comprising a birefringent crystal having a first flat major surface and a second cylindrically concave major surface with a predetermined center thickness;

said second phase plate comprising a birefringent crystal having a first flat major surface and a second cylindrically convex major surface with a predetermined radius of curvature equal to the radius of curvature of said concave surface of said first phase plate and a predetermined center thickness equal to the center thickness of said first phase plate; and

a polarizing means disposed in optical alignment with said phase plates for ejecting radiation having a first polarization from said cavity and transmitting radiation having a second polarization orthogonal to said first polarization.

11. The invention of claim 10 wherein said matching phase plates comprise:

birefringent crystals having their primary optical axes disposed at a predetermined angular orientation.

12. The invention of claim 11 wherein:

said phase plates are so disposed that the concave surface of said first plate is in mating relationship with said convex surface of said second plate; and

said optical axes of said crystals are disposed in orthogonal relationship.

13. The invention of claim 9 wherein:

said first time constant is on the order of 1.0 to 3.0 microseconds; and

said second time constant is on the order of 2.0 to 4.0 nanoseconds.

14. A method for controlling the generation of a laser beam in a laser resonant cavity comprising the steps of:

exciting a laser medium to build up a population inversion in said laser medium;

activating a Q-switch disposed in said laser resonant cavity a first time to produce a seed beam of coherent electromagnetic radiation in said cavity;

passing said seed beam through a zero order phase retardation unit to produce a beam in which the transverse electromagnetic TEM₀₀ mode has a first polarization and the higher order TEM modes have a second polarization orthogonal to said first polarization;

impinging said beam on a polarizing means to transmit said TEM₀₀ mode and to reject said higher order TEM modes from said cavity;

activating said Q-switch a second time to cause rapid depletion of population inversion to produce a pulse of coherent electromagnetic radiation within said laser cavity;

passing said pulse through said zero order phase retardation unit to produce a polarized pulse;

impinging said polarized pulse upon said polarizing means to transmit a single TEM₀₀ mode pulse of oscillating coherent electromagnetic radiation within said cavity; and

outputting a portion of said single TEM₀₀ mode pulse from said cavity during each oscillation of said pulse within said cavity.

15. The invention of claim 14 wherein:

said step of activating said Q-switch a first time comprises partially discharging a precharged voltage from a Pockel'"'"'s cell through a discharge circuit having a time constant on the order of 1.0 to 3.0 microseconds; and

said step of activating said Q-switch a second time comprises discharging the remaining voltage from said Pockel'"'"'s cell through a discharge circuit having a time constant on the order of 2.0 to 4.0 nanoseconds.

16. In a combination exhibiting a spacial transmission function for incident light, including a beam polarized in a P dimension,

A. an optical transmission filter for imposing a differential phase delay upon said light as a continuous function of position, said transmission filter having an optical axis which is concentric with the axis of said beam and comprising:

1. a first lens of birefringent material of a first center thickness having a first surface which is flat and a second surface which has a predetermined radius of curvature,

2. a second lens of birefringent material of a second cneter thickness having a first surface which is flat and a second surface which has a radius of curvature equal to the radius of curvature of said first lens but of opposite sign,

the surfaces of said lenses being oriented orthogonal to and concentric with said optical axis;

the crystal optical axes of said materials being oriented in mutually orthogonal positions along said optical axis and at an angle of 45°

to said P dimension, with said second surfaces adjacent,

B. polarizing means aligned with the optical axis of said optical transmission filter for rejecting components of the beam elements having a first polarization, and selecting components of the beam elements having a second polarization, the light derived from said polarizing means exhibiting said modification in intensity.

17. The combination set forth in claim 16 wherein:

one of said polarizations of said polarizing means is oriented parallel to said P dimension.

18. The combination set forth in claim 17 wherein:

the second surface of each of said filter lenses is spherical,

said combination exhibiting a radial transmission function, which is a continuous function of the radial distance of light from the axis of the filter.

19. The combination set forth in claim 18 wherein:

said filter lenses provide a small differential phase delay on-axis and a large differential phase delay near the perimeter of the beam,

said combination exhibiting a radial transmission function which transmits said beam, and attenuates light beyond the perimeter of said beam.

20. The combination set forth in claim 18 wherein:

said filter lenses provide a small differential phase delay on-axis and a large differential phase delay near, but within the perimeter of said beam,

said combination exhibiting a radial transmission function which gradually attenuates the perimeter of said beam.

21. The combination set forth in claim 20 having in addition thereto,

an aperture through which said beam must pass,

the attenuation of said beam exhibited by said filter and polarizer combination being substantial at the margin of said beam impinging on said aperture to avoid fringing effects.

22. The combination set forth in claim 20 wherein:

said filter lenses provide a substantial differential phase delay on-axis, a zero differential phase delay at an intermediate radial distance changing in at this distance, and a substantial differential phase delay at the perimeter of said beam,

said combination broadening the profile of said beam.

23. The combination set forth in claim 17 wherein:

the second surface of each of said filter lenses is cylindrical,

said combination exhibiting a spatial transmission function, which is a continuous function of a coordinate of an element of light referenced to the beam axis in a plane orthogonal to said beam axis and in the plane of said curvature.

24. The combination set forth in claim 17 wherein:

said filter lenses provide a small differential phase delay at a zero coordinate value and a large differential phase delay at a maximum coordinate value at the perimeter of said beam,

said combination exhibiting a spacial transmission function which gradually attenuates the perimeter of said beam at said maximum coordinate value.

25. The combination set forth in claim 24 having in addition thereto,

an aperture set at said maximum coordinate value through which said beam must pass,

the attenuation of said beam exhibited by said filter and polarizer combination being substantial at the margin of said beam impinging on said aperture to avoid fringing effects.

26. The combination set forth in claim 25 wherein:

said filter lenses provide a substantial differential phase delay at a zero coordinate value and a zero differential phase delay at an intermediate coordinate value changing in sign at this value, and a substantial differential phase delay at said maximum coordinate value at the perimeter of said beam,

said combination broadening the profile of said beam along said coordinate.

27. Laser apparatus for forming a beam of electromagnetic radiation propagating within said apparatus along the axis thereof, and polarized in a P dimension orthogonal to said axis, comprising:

A. first and second reflector means concentrically arranged upon said axis and defining a stable optical resonator susceptable of operation in multi modes,

B. an active laser medium for producing said beam disposed between said first and second reflector means, concentrically arranged upon said axis, and

C. optical mode control means disposed within said resonant cavity, concentrically arranged upon said axis, comprising,

1. an optical transmission filter for imposing a differential phase delay and consequent progressive polarization rotation upon elements of said polarized coherent electromagnetic radiation as a continuous spacial function, and

2. polarizing means to which said filtered radiation is applied, oriented to attenuate spacially filtered components of said radiation associated with a mode sought to be suppressed and to transmit spacially filtered components of said radiation associated with a desired mode.

28. Laser apparatus as set forth in claim 27 wherein:

said desired mode is a TEM₀₀ mode, and wherein, said optical mode control means exhibits a radial transmission function, which is a continuous function of the radial distance of an element of radiation from asi axis.

29. Laser apparatus as set forth in claim 28 wherein:

said radial transmission function, has a minimum attenuation on-axis and a maximum attenuation at a radial distance corresponding to the perimeter of a beam formed by said TEM₀₀ mode to suppress higher order modes whose energy distribution is beyond the perimeter of said TEM₀₀ formed beam.

30. Laser apparatus as set forth in claim 27 wherein said optical transmission filter comprises:

A. a first lens of birefringent material of a first center thickness having a first surface which is flat and a second surface which has a predetermined radius of curvature,

B. a second lens of birefringent material of a second center thickness having a first surface which is flat and a second surface which has a radius of curvature of said first lens but of opposite sign,

the surfaces of said lenses being oriented orthogonal to and concentric with said axis, the crystal optical axes of the materials of said lenses being oriented in mutually orthogonal positions along said axis and at an angle of 45°

to said P dimension, with said second surfaces adjacent.

31. Laser apparatus as set forth in claim 30 wherein:

the second surface of said filter lenses is spherical to effect a differential phase delay and consequent progressive polarization rotation which is a continuous function of the radial distance of each element of light of radiation from the axis to the filter.

32. Laser apparatus for forming a beam of electromagnetic radiation propagating within said apparatus along the axis thereof, and polarized in a P dimension orthogonal to said axis, comprising:

A. first and second reflector means concentrically arranged upon said axis and defining a stable/unstable optical resonator, stable operation occurring along an S dimension, orthogonal to said axis, to the dimension of stable operation, and to said P dimension,

B. an active laser medium for producing said beam disposed between said first and second reflector means, concentrically arranged upon said axis,

said laser apparatus having an effective aperture at an S coordinate value referred to said axis, and

C. beam enhancement means disposed within said optical resonator concentrically arranged upon said axis comprising;

34. Laser apparatus as set forth in claim 32 wherein said optical transmission filter comprises:

A. a first lens of birefringent material of a first center thickness having a first surface which is flat and a second surface which has a preterermined radius of curvature,

B. a second lens of birefringent material of a second center thickness having a first surface which is flat and a second surface which has a radius of curvature equal to the radius of curvature equal to the radius of curvature of said first lens but of opposite sign,

the surfaces of said lenses being oriented orthogonal to and concentric with said axis, the crystal opitcal axes of the materials of said lenses being oriented in mutually orthogonal positions along said axis and at an angle of 45°

to said P dimension, with said second surfaces adjacent.

33. an optical transmission filter for imposing a differential phase delay and consequent progressive polarization rotation of elements of said P polarized coherent electromagnetic radiation as a continuous function of their S coordinate values, andpolarizing means to which said filtered radiation is applied oriented to attenuate spacially filtered elements of said radiation as a continuous function of said S coordinate value, said function producing a zero attenuation on-axis, which increases to a miximum attenuation at the maximum S coordinate value of said aperture to enchance said beam.

35. Laser apparatus as set forth in claim 33 wherein:

the second surface of each of said filter lenses is cylindrical to effect a differential phase dalay and consequent progressive polarization rotation which is a continuous function of an S coordinate of each element of radiation.

37. In combination as set forth in claim 35 wherein:

said beam has a circular cross-section and a profile which is invarient with rotation about said beam axis, and wherein,

said optical transmission filter exhibits a radial transmission function.

38. The combination set forth in claim 35 wherein said optical transmission filter is adjustable, comprising,

A. a first lens of birefringent material of a first center thickness having a first surface which is flat and a second surface which has a predetermined radius of curvature, the surfaces of said lens being oriented orthogonal to and concentric with said optical axis;

B. A second, compound lens of birefringent material of an adjustable center thickness, having a first surface which is flat and a second surface which has a radius of curvature equal to the radius of curvature of said first lens but of opposite sign, said second lens consisting of,

a wedge shaped first lens element with flat surfaces, having a cross-section tapered at a first angle, and a second lens element having a cross-section tapered at said first angle, assembled in sliding engagement with said wedge shaped lens element, the external surfaces of said compound lens being oriented orthogonal to and centered on said optical axis,

The crystal optical axes of the materials of said lenses being oriented in mutually orthogonal positions along said optical axis and at an angle of 45°

to said P dimension, with said second surfaces adjacent.

39. The combination set forth in claim 37 wherein a second surface of each of said filter lenses is spherical to effect a beam profile modification which is a continuous function of the radial distance of each beam element from the beam axis.

41. The combination set forth in claim 39 wherein said optical transmission filter is adjustable, comprising,

A. a first lens of birefringent material of a first center thickness having a first surface which is flat and a second surface which has a predetermined radius of curvature, the surfaces of said lens being oriented orthogonal to and cocentric with said optical axis;

B. a second, compound lens of birefringent material of adjustable center thickness, having a first surface which is flat and a second surface which has a radius of curvature equal to the radius of curvature of said first lens but of opposite sign, said second lens consisting of,

a wedge shaped first lens element with flat surfaces, having a cross-section tapered at a first angle, and

a second lens element having a cross-section tapered at said first angle, assembled in sliding engagement with said wedge shaped lens element, the external surfaces of said compound lens being oriented orthogonal to and centered on said optical axis,

the crystal optical axes of the materials of said lenses being oriented in mutually orthogonal positions along said optical axis and at an angle of 45°

to said P dimension with said second surfaces adjacent.

36. In combination:

A. means for supplying a beam of light propagating along a prescribed axis and polarized in a P dimension orthogonal to said axis, said beam exhibiting symmetrical intensity profile peaking on said beam axis and diminishing gradually toward the beam perimeter;

B. optical intensity profile control means having an optical axis coincident with said beam axis for imposing greater rectangularity upon said profile, comprising;

1. an optical transmission filter for imposing a differential phase delay and consequent polarization rotation upon elements of said polarized beam as a continuous spacial function, in which a substantial differential phase delay occurs on said beam axis, a zero differential phase delay occurs at an intermediate distance, changing in sense at this distance, and a substantial delay again occurs at the perimeter of the beam, and

2. polarizing means to which said filtered beam is applied, oriented to provide substantial attenuation on-axis, zero attenuation at said intermediate distance and a substantial attenuation at the beam perimeter, and

C. beam amplification means having an active medium dimensioned to accept said modified intensity profile for enhancing the filling of said medium.

40. In combination:

A. means for supplying a beam of light propagating along a prescribed axis and polarized in a P dimension orthogonal to said axis, said beam exhibiting a symmetrical intensity profile peaking on said beam axis and diminishing gradually toward the beam perimeter along an S dimension orthogonal to said axis and to said P dimension,

B. optical intensity profile control means having an optical axis coincident with said beam axis for imposing greater rectangularity to said S dimension profile, comprising;

1. an optical transmission filter for imposing a differential phase delay and consequent polarization rotation upon elements of said polarized beam as a continuous spacial function in whcih a substantial differential phase delay occurs on said beam axis, a zero differential phase delay occurs at an intermediate S dimension, changing in sense at this intermediate S dimension, and a substantial delay again occurs at a maximum S dimension at the perimeter of the beam, and

2. polarizing means to which said filtered beam is applied, oriented to provide substantial attenuation on-axis, zero attenuation at said intermediate S dimension and a substantial attenuation at said maximum S dimension at the beam perimeter, and

C. a beam amplification means having an aperature dimensioned to accept said modified intensity profile.

42. The combination set forth in claim 40 wherein, the second surface of each of said filter lenses is cylindrical to effect a beam profile modification which is a continuous function of the S dimension of each beam element.