IP Library Granted Patent US 12,548,964
Granted Patent B2
US 12,548,964 · App. 18/021,009 · Granted Feb 10, 2026

Self-isolated nanoscale laser

Inventors: Jefferson Dixon (Staten Island, NY); Mark Lawrence (Saint Louis, MO); David Russell Barton, III (Somerville, MA); Jennifer A. Dionne (Menlo Park, CA)
Assignee: The Board of Trustees of the Leland Stanford Junior University
H01S3/08054H01S3/094H01S3/094073H01S3/1628H01S3/30
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Quick Facts
Patent No.
US 12,548,964
App. No.
18/021,009
Granted
Feb 10, 2026
Kind
B2
Abstract

Self-isolated lasers are provided by using a chiral metasurface in combination with a spin-selective gain medium and symmetry-breaking (i.e., not linearly polarized) optical pumping. In preferred embodiments the chiral metasurface is resonant, thereby proving an integrated optical resonator to support lasing. The chiral metasurface can be the spin-selective gain medium, or it can be formed on a surface of the spin-selective gain medium, or it can be distinct from the spin-selective gain medium.

Claims (15)

1 . A self-isolated coherent light source comprising:

a pump source configured to provide pump radiation having a not-linear state of polarization;

a spin-selective gain medium configured to provide gain when excited by the pump radiation;

an optical resonator configured to define a lasing mode when the spin-selective gain medium is excited by the pump radiation; and

a chiral metasurface configured to provide less loss to the lasing mode than to a back-reflection of the lasing mode.

2 . The self-isolated coherent light source of claim 1 , wherein the pump radiation has an ellipticity e of its state of polarization such that 0.5≤|e|≤1.0.

3 . The self-isolated coherent light source of claim 2 , wherein the pump radiation has an ellipticity e of its state of polarization such that 0.9≤|e|≤1.0.

4 . The self-isolated coherent light source of claim 1 , wherein the spin-selective gain medium is a Raman-active medium.

5 . The self-isolated coherent light source of claim 1 , wherein the spin-selective gain medium is an inversion-asymmetric transition metal dichalcogenide.

6 . The self-isolated coherent light source of claim 1 , wherein the chiral metasurface is formed of a surface of the spin-selective gain medium.

7 . The self-isolated coherent light source of claim 1 , wherein the chiral metasurface is the spin-selective gain medium.

8 . The self-isolated coherent light source of claim 1 , wherein the chiral metasurface is distinct from the spin-selective gain medium.

9 . The self-isolated coherent light source of claim 1 , wherein the chiral metasurface is distinct from the optical resonator.

10 . The self-isolated coherent light source of claim 1 , wherein the chiral metasurface has a resonance that serves as the optical resonator.

11 . The self-isolated coherent light source of claim 1 , wherein the chiral metasurface has a quality factor Q of 10 or more.

Assignments (2)
CONFIRMATORY LICENSE Recorded Jan 12, 2024
From: STANFORD UNIVERSITY
To: UNITED STATES DEPARTMENT OF ENERGY
Reel/Frame 066286/0820 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 13, 2023
From: DIXON, JEFFERSON; LAWRENCE, MARK; BARTON III, DAVID RUSSELL; DIONNE, JENNIFER A.
To: THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY
Reel/Frame 062672/0616 →
Continuity (2)
Provisional Application 63065908 · Aug 14, 2020
Related Publication 20230299551A1 · Sep 21, 2023
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