IP Library Granted Patent US 10,871,699
Granted Patent B2
US 10,871,699 · App. 16/530,737 · Granted Dec 22, 2020

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

Inventors: Dileep V. Reddy (Eugene, OR); Michael G. Raymer (Eugene, OR)
Assignee: University of Oregon
G02F1/3544G02F1/3534G02F1/3536
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Quick Facts
Patent No.
US 10,871,699
App. No.
16/530,737
Granted
Dec 22, 2020
Kind
B2
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.

Claims (31)

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.

Assignments (2)
CONFIRMATORY LICENSE Recorded Oct 9, 2019
From: UNIVERSITY OF OREGON
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 050674/0045 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 5, 2019
From: REDDY, DILEEP V.; RAYMER, MICHAEL G.
To: UNIVERSITY OF OREGON
Reel/Frame 049958/0486 →
Continuity (2)
Provisional Application 62713811 · Aug 2, 2018
Related Publication 20200041868A1 · Feb 6, 2020
Cited By (1)
US 12,700,520