Systems and methods for eliminating multi-path errors from atomic inertial sensors

Patent metadata

Field	Value
Publication number	US-9887019-B2
Application number	US-201615016180-A
Country	US
Kind code	B2
Filing date	Feb 4, 2016
Priority date	Feb 4, 2016
Publication date	Feb 6, 2018
Grant date	Feb 6, 2018

Abstract

Systems and methods for eliminating multi-path errors from atomic inertial sensors are provided. In certain embodiments, a system for performing atom interferometry includes a vacuum cell containing multiple atoms and a first plurality of lasers configured to trap the atoms within the vacuum cell. The system further includes a second plurality of lasers configured to impart momentum to the atoms and direct the atoms down multiple paths, wherein a primary path in the multiple paths has a first and second component that converge at a converging point, wherein a diverging part of the primary path in which the first and second components are diverging is asymmetrical with respect to a converging part of the primary path in which the first and second components are converging, such that only the first and second components converge at the converging point wherein other paths do not converge at the converging point.

First claim

What is claimed is:

1. A system for performing atom interferometry, the system comprising:
a vacuum cell, wherein a plurality of atoms are contained therein;
a first plurality of lasers configured to trap at least one of the plurality of atoms within the vacuum cell;
a second plurality of lasers configured to impart momentum to the at least one of the plurality of atoms and direct the at least one of the plurality of atoms down a plurality of paths, wherein a primary path in the plurality of paths has a first component and a second component that converge at a converging point, wherein a diverging part of the primary path in which the first component and the second component are diverging is asymmetrical with respect to a converging part of the primary path in which the first component and second component are converging, such that a diverging time when the first component and the second component are diverging is different than a converging time when the first component and the second component are converging, wherein only the first component and the second component of the primary path converge at the converging point wherein other paths in the plurality of paths do not converge at the converging point.

2. The system of claim 1 , wherein the at least one of the plurality of atoms traveling along the first component and the second component travel for a different duration than other atoms traveling on the other paths before arriving at the converging point.

3. The system of claim 1 , wherein the asymmetry of the diverging time and the converging time is introduced after the formation of the plurality of paths.

4. The system of claim 1 , wherein the first plurality of lasers and the second plurality of lasers are the same plurality of lasers.

5. The system of claim 1 , wherein the at least one of the plurality of atoms that travel along the primary path are measured at the converging point, wherein the measurements are processed to acquire inertial data.

6. The system of claim 1 , wherein the first plurality of lasers are created by a plurality of slave lasers that are locked to a master laser.

7. A method for performing atom interferometry, the method comprising:
trapping a plurality of atoms within a vacuum cell;
imparting momentum to at least one atom in the plurality of atoms;
directing the at least one of the plurality of atoms down a plurality of paths, wherein a primary path in the plurality of paths has a first component and a second component that converge at a converging point, wherein a diverging part of the primary path in which the first component and the second component are diverging is asymmetrical with respect to a converging part of the primary path in which the first component and second component are converging, such that a diverging time when the first component and the second component are diverging is different than a converging time when the first component and the second component are converging, wherein only the first component and the second component of the primary path converge at the converging point wherein other paths in the plurality of paths do not converge at the converging point; and
acquiring a measurement from the atoms that converge at the converging point.

8. The method of claim 7 , wherein the at least one of the plurality of atoms traveling along the first component and the second component travel for a different duration than other atoms traveling on the other paths before arriving at the converging point.

9. The method of claim 7 , wherein the asymmetry of the diverging time and the converging time is introduced after the formation of the plurality of paths.

10. The method of claim 7 , wherein the plurality of atoms are trapped within the vacuum cell and the momentum is imparted to the at least one atom in the plurality of atoms are imparted by a plurality of lasers.

11. The method of claim 10 , wherein the plurality of lasers are created by a plurality of slave lasers that are locked to a master laser.

12. The method of claim 7 , wherein the plurality of atoms are trapped within the vacuum cell by a first plurality of lasers and the momentum is imparted to the at least one atom in the plurality of atoms are imparted by a second plurality of lasers.

13. The method of claim 7 , further comprising calculating inertial data from the measurement.

14. A system for performing atom interferometry, the system comprising: a master laser a plurality of slave lasers, the plurality of slave lasers are locked to the master laser a vacuum cell having a plurality of atoms contained therein, wherein the plurality of slave lasers are directed into the vacuum cell to trap at least one of the plurality of atoms within the vacuum cell; a second plurality of lasers configured to impart momentum to the at least one of the plurality of atoms and direct the at least one of the plurality of atoms down a plurality of paths, wherein a primary path in the plurality of paths has a first component and a second component that converge at a converging point, wherein a diverging part of the primary path in which the first component and the second component are diverging is asymmetrical with respect to a converging part of the primary path in which the first component and second component are converging, such that a diverging time when the first component and the second component are diverging is different than a converging time when the first component and the second component are converging, wherein only the first component and the second component of the primary path converge at the converging point wherein other paths in the plurality of paths do not converge at the converging point; a detector configured to provide a signal from atoms detected at the converging point; and a processor configured to calculate measurements from the signal.

15. The system of claim 14 , wherein the at least one of the plurality of atoms traveling along the first component and the second component travel for a different duration than other atoms traveling on the other paths before arriving at the converging point.

16. The system of claim 14 , wherein the asymmetry of the diverging time and the converging time is introduced after the formation of the plurality of paths.

17. The system of claim 14 , wherein the plurality of slave lasers and the second plurality of lasers are the same plurality of lasers.

Assignees

• Honeywell Int Inc

Inventors

• Compton Robert
• Nelson Karl D
• Fertig Chad

Classifications

• G21K1/30 Primary

  for confining neutral particles or handling confined neutral particles, e.g. atom traps · CPC title

• G01P15/08

  with conversion into electric or magnetic values · CPC title

• G01C19/58

  Turn-sensitive devices without moving masses · CPC title

• G21K1/006 Primary

  Physics · mapped topic