System and method for femtotesla direct magnetic gradiometer using a multipass cell

Patent metadata

Field	Value
Publication number	US-11953569-B2
Application number	US-202117519826-A
Country	US
Kind code	B2
Filing date	Nov 5, 2021
Priority date	Nov 5, 2020
Publication date	Apr 9, 2024
Grant date	Apr 9, 2024

Abstract

According to various embodiments, a direct magnetic gradiometer having intrinsic subtraction of rotation signals from two oppositely polarized atomic ensembles within a single multi-pass cell is disclosed. The gradiometer includes three convex spherical mirrors aligned in a V-shape geometry. The three convex spherical mirrors include a front mirror and two back mirrors. The gradiometer further includes a probe laser beam. The laser beam is configured to be initially focused at a near-zero angle into a hole at a center of the front mirror such that the laser beam expands at the back mirrors and nearly overlaps with itself while undergoing multiple reflections between the front and back mirrors. The laser beam is further configured to be refocused to the front mirror at different spots in a number equal to half of total beam passes before exiting.

First claim

What is claimed is:

1. A direct magnetic gradiometer having intrinsic subtraction of rotation signals from two atomic ensembles within a single multi-pass cell, the gradiometer comprising:
three convex spherical mirrors aligned in a V-shape geometry, the three convex spherical mirrors comprising a front mirror and two back mirrors; and
a probe laser beam configured to:
be initially focused at a near-zero angle into a hole at a center of the front mirror such that the laser beam expands at the back mirrors and nearly overlaps with itself while undergoing multiple reflections between the front and back mirrors; and
be refocused to the front mirror at different spots in a number equal to half of total beam passes before exiting.

2. The gradiometer of claim 1 , wherein the single multi-pass cell encloses the two back mirrors.

3. The gradiometer of claim 1 , wherein the single multi-pass cell has an anti-reflection coated front window.

4. The gradiometer of claim 1 , wherein the laser beam is linearly polarized.

5. The gradiometer of claim 1 , further comprising a collimation lens, a half wave plate, and a polarizing beam splitter.

6. The gradiometer of claim 1 , wherein the single multi-pass cell is filled with 87 Rb.

7. The gradiometer of claim 1 , further comprising two pump lasers configured to polarize atoms in opposite directions to subtract their signals.

8. An optical arrangement comprising:
a laser beam configured to be focused into an arrangement of at least three convex spherical mirrors, the mirrors being pre-aligned to expand the laser beam such that the laser beam nearly overlaps with itself while undergoing multiple reflections between the mirrors and then exits the arrangement of mirrors after a predetermined number of beam passes,
wherein the laser beam is configured to be refocused to a front mirror of the mirrors at different spots in a number equal to half of the predetermined number of beam passes before exiting.

9. The optical arrangement of claim 8 , further comprising a single multi-pass cell that encloses two back mirrors of the mirrors.

10. The optical arrangement of claim 9 , wherein the single multi-pass cell has an anti-reflection coated front window.

11. The optical arrangement of claim 9 , wherein the single multi-pass cell is filled with 87 Rb.

12. The optical arrangement of claim 8 , wherein the laser beam is linearly polarized.

13. The optical arrangement of claim 8 , further comprising a collimation lens, a half wave plate, and a polarizing beam splitter.

14. The optical arrangement of claim 8 , further comprising at least one pump laser configured to polarize atoms in opposite directions to subtract their signals.

15. A method for operating an optical arrangement, the optical arrangement including a laser beam and three convex spherical mirrors aligned in a V-shape geometry, the three convex spherical mirrors including a front mirror and two back mirrors, the method comprising:
initially focusing the laser beam at a near-zero angle into a hole at a center of the front mirror such that the laser beam expands at the back mirrors and nearly overlaps with itself while undergoing multiple reflections between the front and back mirrors; and
refocusing the laser beam to the front mirror at different spots in a number equal to half of total beam passes before exiting.

16. The method of claim 15 , further comprising linearly polarizing the laser beam.

17. The method of claim 15 , further comprising collimating the exited laser beam.

18. The method of claim 15 , further comprising detecting a differential signal from the exited laser beam.

19. The method of claim 15 , further comprising continuously recording a free induction decay.

Assignees

• Univ Princeton

Inventors

• Romalis Michael
• Dural Nezih
• Lucivero Vito-Giovanni
• Lee Wonjae

Classifications

• G01R33/26 Primary

  using optical pumping · CPC title

• G02B17/004

  Systems comprising a plurality of reflections between two or more surfaces, e.g. cells, resonators (multipass arrangements for optical cuvettes G01N21/031; laser resonators H01S3/05) · CPC title

• G02B17/0626

  using three curved mirrors (G02B17/0668, G02B17/0694 take precedence) · CPC title

• G02B5/3083

  Birefringent or phase retarding elements (G02B5/3008, G02B5/3016 take precedence; systems for polarisation control G02B27/286; manufacturing phase modulating patterns by lithographic processes G03F7/001) · CPC title

• G02B27/283

  used for beam splitting or combining · CPC title