Resonant phase modulator

• US 4,998,255 A
• Filed: 10/11/1989
• Issued: 03/05/1991
• Est. Priority Date: 10/11/1989
• Status: Expired due to Fees

• Current Assignee: Lightwave Electronics Corp. (Lumentum Holdings Inc.)
• Original Assignee: Lightwave Electronics Corp. (Lumentum Holdings Inc.)
• Inventors: Wallace, Richard, Gerstenberger, David C., Kane, Thomas J.
• Primary Examiner(s): Gonzalez, Frank
• Assistant Examiner(s): NOT, DEFINED
• Application Number:
  US07/420,045
• Time in Patent Office: 510 Days
• Field of Search: 372/26, 372/100, 372/28, 372/98, 350/353, 350/355, 350/356
• US Class Current: 372/28
• CPC Class Codes: G02F 1/03 based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect G02F1/061 takes precedence
• CPC Class Codes: G02F 1/21 by interference
• CPC Class Codes: G02F 1/212 Mach-Zehnder type

Abstract

Apparatus and method for modulating the phase or the amplitude of a monochromatic light beam, the apparatus including in one embodiment a Mach-Zehnder interferometer that consists of two beam splitters or beam combiners, a fully reflective mirror and an electro-optical crystal for modulation of one of two beam components. The electro-optical crystal serves as an optical resonator for the portion of the light beam admitted into the crystal material, using total internal reflection of the light beam from two or more of the crystal surfaces. The crystal has a high finesse so that a relatively small change in voltage applied across the crystal produces a large (≈180°) change in the external phase shift associated with the modulated component of the light beam. The modulated and unmodulated light beam components may be recombined for purposes of communication of information, using the mutual extinction of the two beam components when the optical phase shift between the two beam components is approximately 180°. Transverse or longitudinal electro-optical materials can be used for the crystal, and the driving voltages required are less than 50 volts in some configurations. Communications at frequency up to and beyond 1 GHz. are possible.

Claims

1. Light beam modulation apparatus for varying the optical phases of a light beam output signal relative to the optical phase of a light beam input signal, the apparatus comprising:

an optically resonant electro-optical crystal, having a first partially transmissive crystal face to receive a light beam having a frequency-stabilized single frequency and to cause a portion of the light beam to propagate internally within the crystal, and having at least second and third crystal faces positioned to reflect this internally propagating portion of the beam so that this portion follows a closed path within the crystal with a phase shift φ

that varies around a resonant value φ

_r =2Nπ

, where N is a non-zero integer, along this closed path, where a portion of this internally propagating portion of the light beam that arrives at the first crystal face combines with an externally reflected portion of the light beam to form an output beam propagating in a selected direction; and

a voltage source positioned adjacent to the crystal to impress a controllable, time-varying voltage deference across the crystal in a second selected direction to controllably vary the phase shift φ

about the resonant value φ

_r =2Nπ

.

2. The apparatus of claim 1, wherein said electro-optical crystal is drawn from the class consisting of CdTe, GaAs, GaP, ZnS, ZnSe and ZnTe.

3. The apparatus of claim 1, wherein said electro-optical crystal is drawn from the class consisting of LiNbO₃ and LiTaO₃.

4. The apparatus of claim 1, wherein said electro-optical crystal is drawn from the class consisting of AgGaS₂, CsH₂ AsO₄, KH₂ PO₄, KD₂ PO₄, (NH₄)H₂ PO₄, (NH₄)HDPO₄ and (NH₄)D₂ PO₄.

5. The apparatus of claim 4, wherein said electrical field has a direction that has a non-zero component lying in the plane defined by the optical path of said light beam in said crystal.

6. The apparatus of claim 1, wherein said voltage source can change the polarity of said impressed electrical field at a frequency that is greater than 0 Hertz and is no greater than 10⁹ Hertz.

7. The apparatus of claim 1, wherein said crystal has a finesse of at least 4.4.

8. The apparatus of claim 1, wherein said first crystal face has an associated optical reflectivity of at least 50 percent for the wavelength of said light beam.

9. The apparatus of claim 1, wherein the round trip optical path within said crystal has a length L and one of said first, second and third crystal faces is curvilinear and has a curvature R satisfying the relation R>

L/2.

10. The apparatus of claim 1, further comprising a light beam source that produces a frequency-stabilized light beam with a selected polarization direction, where this light beam is received by said electro-optical crystal.

11. The apparatus of claim 1, further comprising voltage control means for impressing a control voltage across said crystal to maintain a time average of said phase shift φ

at said resonant phase shift value φ

_r.

12. The apparatus of claim 1, wherein said internally propagating portion of said light beam is reflected by total internal reflection at at least one of said second crystal face and said third crystal face.

13. The apparatus of claim 12, wherein said voltage source can modulate said voltage difference between said two electrodes at a frequency greater than 0 Hertz and no greater than 10⁹ Hertz.

14. The apparatus of claim 13, wherein said electro-optical crystal is drawn from the class consisting of CdTe, GaAs, GaP, ZnDS, ZnSe and ZnTe.

16. The apparatus of claim 12, wherein said electro-optical crystal is composed of a longitudinal electro-optical material drawn from the class consisting of AgGaS₂, CsH₂ AsO₄, KH₂ PO₄, KD₂ PO₄, (NH₄)H₂ PO₄, (NH₄)HDPO₄ and (NH₄)D₂ PO₄.

17. The apparatus of claim 16, wherein said polarization direction of said light beam is chosen to lie in a plane defined by the optical path of said light beam in said crystal.

18. Light beam modulation apparatus comprising:

a light beam source that produces a single frequency, frequency-stabilized light beam with a selected polarization direction;

beam splitter means for receiving the light beam and for producing first component and second component light beams that issue therefrom in different directions;

phase shift means for receiving the first component light beam from the splitter means, for splitting off a portion of this light beam and shifting the phase of this portion, relative to the remainder portion of the first component light beam, by a time-variable, controllable phase shift φ

about a resonant phase shift value φ

_r =2Nπ

, where N is a non-zero integer, and for combining the split-off portion of the beam with the remainder portion of the beam as a first composite light beam that propagates in a selected direction; and

beam combiner means for combining the first composite light beam with the second component light beam as an overall composite light beam, whereby the amplitude of the overall composite light beam may be controllably modulated.

15. The apparatus of claim 19, wherein said electro-optical crystal is drawn from the class consisting of LiNbO₃ LiTaO₃.

19. The apparatus of claim 18, wherein said phase shift means comprises:

an optically resonant electro-optical crystal, having a first partially transmissive crystal face to receive said first component light beam and to cause a portion of this light beam to propagate internally within the crystal, and having at least second and third crystal faces positioned to reflect this internally propagating portion of this beam so that this portion follows a closed path within the crystal with said phase shift φ

_r along this closed path, where a portion of this internally propagating portion of said first component light beam that arrives at the first crystal face combines with an externally reflected portion of said first component light beam to form said first composite light beam propagating in a selected direction;

two electrodes positioned so that the electro-optical crystal lies between the two electrodes; and

a voltage source positioned adjacent to the crystal to impress a controllable, time-varying voltage difference across the crystal in a second selected direction to controllably vary said phase shift φ

about said resonant value φ

_r =2Nπ

.

20. The apparatus of claim 19, further comprising voltage control means for impressing a control voltage across said crystal to maintain a time average of said phase shift φ

at a said resonant phase shift value φ

_r.

21. The apparatus of claim 19, wherein said internally propagating portion of said light beam is reflected by total internal reflection at at least one of said second crystal face and said third crystal face.

22. The apparatus of claim 18, further comprising:

second phase shift means for receiving said second component light beam from said splitter means, for splitting off a portion of this light beam and shifting the phase of this portion, relative to the remainder portion of said second component light beam, by a time-variable, controllable phase shift ψ

about a resonant phase shift value ψ

_r =2Mπ

, where M is a non-zero integer, and for combining the split-off portion of the beam with the remainder portion of the beam as a second composite light beam that propagates in a selected direction, where said beam combiner means combines the second composite light beam with said first composite light beam.

23. The apparatus of claim 22, wherein said first phase shift means and said second phase shift means together comprise:

a first optically resonant electro-optical crystal, having a first partially transmissive crystal face to receive said first component light beam and to cause a portion of this light beam to propagate internally within the crystal, and having at least second and third crystal faces positioned to reflect this internally propagating portion of this beam so that this portion follows a closed path within the crystal with a phase shift φ

_r =2Nπ

, where N is a non-zero integer, along this closed path, where a portion of this internally propagating portion of said first component light beam that arrives at the first crystal face combines with an externally-reflected portion of said first component light beam to form said first composite light beam propagating in a first selected direction;

a second optically resonant electro-optical crystal, having a first partially transmissive crystal face to receive said second component light beam and to cause a portion of this light beam to propagate internally within the crystal, and having at least second and third crystal faces positioned to reflect this internally propagating portion of the beam so that this portion follows a closed path within the crystal with a phase shift ψ

_r =2Mπ

, where M is a non-zero integer, along this closed path, where a portion of this internally propagating portion of said second component light beam that arrives at the first crystal face combines with an externally reflected portion of said second component light beam to form said second component light beam propagating in a second selected direction;

first and second electrodes, positioned so that the first electro-optical crystal lies between the first and second electrodes;

third and fourth electrodes, positioned so that the second electro-optical crystal lies between the third and fourth electrodes; and

a voltage source having a positive terminal connected to the first and fourth electrodes and having a negative terminal connected to the second and third electrodes to impress controllable, time-varying first and second voltage differences of opposite polarities across the first and second electro-optical crystals.

24. Light beam modulation apparatus for varying the optical phases of a light beam output signal relative to the optical phase of a light beam input signal, the apparatus comprising:

an optically resonant electro-optical crystal, having a first partially transmissive crystal face with optical reflectivity at least 50 percent to receive a light beam having a frequency-stabilized single frequency and to cause a portion of the light beam to propagate internally within the crystal, and having at least second and third crystal faces positioned to reflect this internally propagating portion of the beam so that this portion follows a closed path within the crystal with a phase shift φ

that varies around a resonant value φ

_r =2Nπ

, where N is a non-zero integer, along this closed path, where a portion of this internally propagating portion of the light beam that arrives at the first crystal face combines with an externally reflected portion of the light beam to form an output beam propagating in a selected direction; and

a voltage source positioned adjacent to the crystal to impress a controllable, time-varying voltage difference across the crystal in a second selected direction to controllably vary the phase shift φ

about the resonant value φ

_r =2Nπ

.

25. Light beam modulation apparatus for varying the optical phases of a light beam output signal relative to the optical phase of a light beam input signal, the apparatus comprising:

an optically resonant electro-optical crystal, having a first partially transmissive crystal face to receive a light beam having a frequency-stabilized single frequency and to cause a portion of the light beam to propagate internally within the crystal, and having at least second and third crystal faces positioned to reflect this internally propagating portion of the beam so that this portion follows a closed path within the crystal with a phase shift φ

that varies around a resonant value φ

_r =2Nπ

, where N is a non-zero integer, along this closed path, where a portion of this internally propagating portion of the light beam that arrives at the first crystal face combines with an externally reflected portion of the light beam to form an output beam propagating in a selected direction, and where the round trip optical path within the crystal has a length L and one of the first, second and third crystal faces is curvilinear and has a radius R satisfying the relation R>

L/2; and

a voltage source positioned adjacent to the crystal to impress a controllable, time-varying voltage difference across the crystal in a second selected direction to controllably vary the phase shift φ

about the resonant value φ

_r =2Nπ

.