Temporal modes of electromagnetic radiation using nonlinear optical cavities and shaped laser pulses

Patent metadata

Field	Value
Publication number	US-10871699-B2
Application number	US-201916530737-A
Country	US
Kind code	B2
Filing date	Aug 2, 2019
Priority date	Aug 2, 2018
Publication date	Dec 22, 2020
Grant date	Dec 22, 2020

Abstract

Apparatus include an optical cavity including an optical coupling portion situated to couple an optical signal input field to an intracavity optical signal field and an optical control input field to an intracavity optical control field, wherein the optical cavity includes a nonlinear optical medium that mediates a selective exchange of at least one predetermined temporal mode between the intracavity optical signal field and an intracavity optical register field based on a nonlinear phase-matched interaction between the intracavity optical signal, control, and register fields and selectable field characteristics of the optical control input field.

First claim

We claim:

1. An apparatus, comprising:
an optical cavity including an optical coupling portion situated to couple an optical signal input field to an intracavity optical signal field and an optical control input field to an intracavity optical control field, wherein the optical cavity includes a nonlinear optical medium that mediates a selective exchange of a predetermined temporal mode of the optical signal input field and an intracavity optical register field based on a nonlinear phase-matched interaction between the intracavity optical signal, control, and register fields and selectable field characteristics of the optical control input field.

2. The apparatus of claim 1 , wherein a cavity lifetime of the intracavity optical register field is longer than a cavity lifetime of the intracavity optical signal field, and wherein a rate of temporal variation of the optical signal input field is slower than the cavity lifetime of the intracavity optical signal field.

3. The apparatus of claim 2 , wherein the cavity lifetime of the intracavity optical register field is at least ten times longer than a cavity lifetime of the intracavity optical signal field.

4. The apparatus of claim 1 , wherein the field characteristics of the optical control input field are selected to produce the selective exchange corresponding to a unitary shift of the predetermined temporal mode of the optical signal input field to a carrier frequency of the intracavity optical register field so that the intracavity optical register field can be stored in the optical cavity or allowed to leak out of the optical cavity.

5. The apparatus of claim 1 , wherein the field characteristics of the optical control input field are selected to produce the selective exchange corresponding to a unitary shift of the intracavity optical register field to the predetermined temporal mode at a carrier frequency of an optical signal output field that can be read out of the optical cavity.

6. The apparatus of claim 1 , further comprising a pulse controller configured to produce the optical control input field with the selectable field characteristics.

7. The apparatus of claim 1 , further comprising an input optical waveguide optically coupled to the optical cavity through the optical coupling portion and configured to propagate one or both of the optical signal input field and optical control input field; and
an output optical waveguide optically coupled to the optical cavity through the optical coupling portion and configured to propagate one or more of an optical signal output field, an optical control output field, and an optical register output field.

8. The apparatus of claim 7 , wherein the input optical waveguide and the output optical waveguide form a single continuous waveguide.

9. The apparatus of claim 7 , wherein the input optical waveguide is evanescently coupled to the optical cavity through the optical coupling portion to couple the one or both of the of the optical signal input field and optical control input field to the respective intracavity optical signal field and/or intracavity optical control field of the optical cavity;
wherein the output optical waveguide is evanescently coupled to the optical cavity through the optical coupling portion to couple one or more of the intracavity optical signal, control, and register fields out of the optical cavity.

10. The apparatus of claim 1 , further comprising a signal input optical waveguide configured to propagate the optical signal input field and optically coupled to the optical cavity through a first surface of the optical coupling portion; and
a control input optical waveguide configured to propagate the optical control input field and optically coupled to the optical cavity through a second surface of the optical coupling portion spaced apart from the first surface.

11. The apparatus of claim 1 , wherein the optical coupling portion includes one or more dichroic reflective surfaces configured to optically couple the optical signal input field and optical control input field to the optical cavity.

12. The apparatus of claim 11 , wherein the one or more dichroic surfaces or another dichroic surface provides a cavity lifetime of the intracavity optical register field that is at least two orders of magnitude longer than a cavity lifetime of the intracavity optical signal field.

13. The apparatus of claim 1 , wherein the mediated selective exchange corresponds to one of a second-order optical nonlinearity and a third-order optical nonlinearity.

14. The apparatus of claim 1 , wherein the optical cavity comprises a ring resonator.

15. The apparatus of claim 14 , wherein the optical cavity comprises a plurality of planar mirrors.

16. The apparatus of claim 1 , wherein the optical cavity comprises a pair of opposing reflective elements configured to form a Fabry-Perot resonator.

17. The apparatus of claim 1 , wherein the optical cavity corresponds to a first optical cavity and the optical signal input field corresponds to a qudit, wherein the apparatus further comprises:
a second optical cavity situated to receive the qudit as operated on by the first optical cavity and to target a predetermined temporal mode of the operated-on qudit with a second optical control input field coupled to the second optical cavity.

18. The apparatus of claim 1 , further comprising a detector optically coupled to the optical cavity to detect the optical signal, control, or register fields, or a combination thereof.

19. A quantum pulse gate, comprising the apparatus of claim 1 .

20. A method, comprising:
frequency shifting with a non-linear optical cavity a selected temporal mode component of a first field at a first frequency to a second field at a second frequency based on a time-dependence of a third field at a third frequency;
wherein a cavity lifetime of the second field is longer than a cavity lifetime of the first field;
wherein a rate of temporal variation of a first signal input associated with the first field is slower than the cavity lifetime of the first field.

21. An apparatus, comprising:
means for receiving a first optical field in an optical cavity; and
means for selectively converting a predetermined temporal mode component of the first optical field to a second optical field at a disjoint frequency in the optical cavity.

Assignees

• Univ Oregon

Inventors

• Reddy Dileep V
• Raymer Michael G

Classifications

• G02F1/3544 Primary

  Particular phase matching techniques · CPC title

• G02F1/3534

  Three-wave interaction, e.g. sum-difference frequency generation (G02F1/3532 takes precedence) · CPC title

• G02F1/3536

  Four-wave interaction · CPC title

• G02F2203/15

  involving resonance effects, e.g. resonantly enhanced interaction · CPC title