Picosecond bistable optical switch using two-photon transitions

• US 4,558,923 A
• Filed: 12/22/1983
• Issued: 12/17/1985
• Est. Priority Date: 12/22/1983
• Status: Expired due to Fees

• Current Assignee: the united states of america as represented by the secretary of the navy
• Original Assignee: the united states of america as represented by the secretary of the navy
• Inventors: Hoffman, Craig A., Meyer, Jerry R., Bartoli, Filbert
• Primary Examiner(s): Punter, William H.
• Application Number:
  US06/564,623
• Time in Patent Office: 726 Days
• Field of Search: 350/354, 350/393
• US Class Current: 359/243
• CPC Class Codes: G02F 1/218 using semi-conducting materials
• CPC Class Codes: G02F 1/3526 using two-photon emission or absorption processes
• CPC Class Codes: G02F 3/024 based on non-linear elements, e.g. non-linear Fabry-Perot cavity G02F3/028 takes precedence

Abstract

A bistable optical switch comprising a Fabry-Perot resonator containing a nonlinear semiconductor medium with a desired band structure and whose susceptibility (refractive index) varies with optical energy density. The Fabry-Perot resonator is biased to a point where two stable transmission states are possible. Switching is accomplished by pumping the nonlinear material with an energy hw in the range 1/2Δ_g <hw<Δ_g, where Δ_g is the bandgap between the upper valence band and the conduction band of the nonlinear material, in order to stimulate a two-photon valence-to-conduction band absorption transition at a non-minimum energy and thereby make possible a one-hw photon virtual transition between the heavy hole and split-off valence bands of the nonlinear material. This virtual transition alters the susceptibility thereby switching the resonator to a different stable transmission state. Switching times on the order of picoseconds are obtained because switching-time is not dependent on the carrier recombination time.

Claims

1. A bistable optical device with switching times in the picosecond range comprising:

an optical resonator with an optical resonant cavity therein and including means for extracting a light output beam from said optical resonant cavity,

a nonlinear material which is essentially optically transparent disposed in said optical resonant cavity, said nonlinear material having a conduction band and at least an upper and a lower valence bands with an energy spacing therebetween such that a two-hw photon transition can occur from a non-minimum energy location in said upper valence band to said conduction band, and a one-hw photon virtual transition at a non-minimum energy can occur between said upper and lower valence bands, said nonlinear material having an optical length which depends on the intensity of light in said optical resonant cavity; and

means for pumping photon energy hw in the range 1/2Δ

_g <

hw<

Δ

_g into said optical resonant cavity in order to stimulate said virtual transition via the two-photon transition, where Δ

_g is the bandgap between the upper valence band and the conduction band of said nonlinear material.

2. A bistable optical device as defined in claim 1, wherein said optical resonator is a Fabry-Perot resonator.

3. A bistable optical device as defined in claim 2, wherein said nonlinear material is a semiconductor material.

4. A bistable optical switch as defined in claim 3, wherein said photon pumping means includes means for optically biasing said Fabry-Perot resonator with an input power such that the Fabry-Perot resonator has at least two stable transmission states at the optical bias.

5. A bistable optical device as defined in claim 4, wherein said semiconductor material is a direct bandgap semiconductor material.

6. A bistable optical device as defined in claim 5, wherein the lower and upper valence bands of said semiconductor material are the split-off valence band and the heavy hole valence band, respectively, and at approximately the two-photon absorption transition momentum location said semiconductor material has an energy gap E_s between said split-off valence band and said heavy hole valence band which is less than the bandgap Δ

_g and greater than one-half the bandgap Δ

_g.

7. A bistable optical device as defined in claim 6, wherein said nonlinear semiconductor material is CdTe.

8. A bistable optical device as defined in claim 7, wherein said nonlinear semiconductor material is Hg_1-x Cd_x Te, 0.7<

<

1.0.

9. A bistable optical switch with switching times in the picosecond range comprising:

a Fabry-Perot resonator including an optical resonant cavity;

a nonlinear semiconductor material disposed in said optical resonant cavity of said Fabry-Perot resonator, said semiconductor material having a conduction band, a heavy hole valence band, and at least one other valence band, and having a refractive index which depends on the intensity of light in said optical resonant cavity; and

means for optically biasing said Fabry-Perot resonator with an optical input power such that the Fabry-Perot resonator has at least two stable transmission states, and for pumping photon energy hw in the range 1/2Δ

_g <

hw<

Δ

_g into said optical resonant cavity in order to stimulate a two-photon absorption transition between said heavy hole valence band and said conduction band and thus switch between said two stable transmission states in said Fabry-Perot resonator, where Δ

_g is the bandgap between the heavy hole valence band and the conduction band of said semiconductor material,

wherein said semiconductor material has a band structure with a one-hw photon potential virtual transition between two valence bands thereof at a non-minimum energy.

10. A bistable optical switch as defined in claim 9, wherein said nonlinear semiconductor material is a direct bandgap semiconductor material.

11. A bistable optical switch as defined in claim 10, wherein said semiconductor material has a band structure such that the two-photon transition between the heavy hole valence band and the conduction band and the one-photon virtual transition between said two valence bands line up at approximately but not exactly the same momentum.

12. A bistable optical switch as defined in claim 11, wherein said at least one other valence band in said semiconductor material is the split-off valence band and said virtual transition is a one-hw photon virtual transition between said split-off valence band and said heavy hole valence band.

13. A bistable optical switch as defined in claim 11, wherein said semiconductor material is Hg_1-x Cd_x Te, 0.7<

x<

1.0.

14. A bistable optical switch as defined in claim 12, wherein the photon energy pumped by said pumping means has its energy hw chosen such that Δ

E_h =E_h -E_h '"'"' is a small positive energy, where E_h '"'"' is the energy of a hole created by the two-photon absorption transition in said heavy hole band and E_h is the energy of a heavy hole near in energy to the hole created by the two photon transition and capable of said virtual transition between the heavy hole and split-off valence bands to thereby contribute to the susceptibility of the semiconductor material.

15. A method for switching an optical Fabry-Perot resonator with switching times in the picosecond range, said Fabry-Perot resonator having an optical resonant cavity with a nonlinear semiconductor material disposed therein, said semiconductor material having a conduction band, a heavy hole valence band and at least one other valence band with a band structure such that a two-hw photon transition can occur from a non-minimum energy location in said heavy hole band to said conduction band, and a one-hw photon virtual transition can occur at a non-minimum energy between two of the valence bands, said semiconductor material also having a refractive index which depends on the intensity of light in said optical resonant cavity, said method comprising the steps of:

biasing said optical resonant cavity of said Fabry-Perot resonantor with an optical input power such that said Fabry-Perot resonator has at least two stable transmission states at the bias input power; and

pumping photon energy hw in the range 1/2Δ

_g <

hw<

Δ

_g into said optical resonant cavity in order to stimulate a virtual transition between valence bands via a two-photon absorption transition and thus switch between said at least two stable transmission states in said Fabry-Perot resonator, where Δ

_g is the bandgap between the heavy hole valence band and the conduction band of the semiconductor material.

16. A bistable optical switch with switching times in the picosecond range comprising:

a Fabry-Perot resonator including an optical resonant cavity;

a nonlinear semiconductor material disposed in said optical resonant cavity of said Fabry-Perot resonator, said semiconductor material having a conduction band, a heavy hole valence band, and at least one other valence band and having a band structure with a direct bandgap between said heavy hole valence and conduction bands, and capable of having a 2-hw photon transition occur from a non-minimum energy location in said heavy hole band to said conduction band, and a 1-hw photon virtual transition occur at a non-minimum energy location between two of the valence bands, said semiconductor material also having a refractive index which depends on the intensity of light in said optical resonant cavity;

means for optically biasing said Fabry-Perot resonator with an optical input power such that the Fabry-Perot resonator has at least two stable transmission states at this optical bias; and

means for perturbing the populations of energy states with energies near the valence band energy states with virtual transitions that can give a contribution to the susceptibility to thereby switch between said two stable transmission states in said Fabry-Perot resonator, wherein said energy state perturbing means comprises means for pumping photon energy hw in the range 1/2Δ

_g <

hw<

Δ

_g into said optical resonant cavity in order to stimulate a two-photon absorption transition at said perturbed energy states, where Δ

_g is the bandgap between the heavy hole valence band and the conduction band of said semiconductor material.

17. A bistable optical switch as defined in claim 16, wherein said at least one valence band in said semiconductor material comprises a split-off valence band and at approximately the two-photon absorption transition momentum location said semiconductor material has an energy gap E_s between said split-off valence band and said heavy hole valence band which is less than the bandgap Δ

_g and greater than one-half the bandgap Δ

_g ; and

the photon energy pumped by said pumping means has its energy hw chosen such that Δ

E_h =E_h -E_h '"'"' is a small positive energy, where E_h '"'"' is the energy of the hole created by the two-photon absorption transition, and E_h is the energy of a heavy hole near in energy to the hole created by the two-photon transition and capable of said virtual transition between the heavy hole and split-off valence bands to thereby contribute to the susceptibility of the semiconductor material.