IP Library Granted Patent US 9,355,750
Granted Patent B2
US 9,355,750 · App. 14/474,702 · Granted May 31, 2016

System and method for optical confinement of atomic particles

Inventors: Mark E. Saffman (Madison, WI); Martin T. Lichtman (Madison, WI)
Assignee: Wisconsin Alumni Research Foundation
G21K1/006
View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 9,355,750
App. No.
14/474,702
Granted
May 31, 2016
Kind
B2
Abstract

A system and method for controlling atomic particles using projected light are provided. In some aspects, a method includes providing a plurality of atomic particles, and generating light fields using frequencies shifted from at least one atomic resonance. The method also includes forming a two-dimensional (“2D”) optical array using the generated light fields, wherein the 2D optical array comprises linear segments of light, and projecting the 2D optical array on the plurality of atomic particles to control their respective locations in space.

Claims (29)

1. A method for controlling atomic particles using projected light comprising:

a) providing a plurality of atomic particles;

b) generating light fields using frequencies shifted from at least one atomic resonance;

c) forming a two-dimensional (“2D”) optical array using the generated light fields, wherein the 2D optical array comprises linear segments of light; and

d) projecting the 2D optical array on the plurality of atomic particles to control their respective locations in space.

2. The method of claim 1 , wherein step a) comprises preparing the plurality of atomic particles using a particle system.

3. The method of claim 1 , wherein step a) further comprises cooling the plurality of atomic particles to temperatures in a range between 1 and 100 micro Kelvin.

4. The method of claim 1 , wherein the frequencies are selected to achieve at least one of a blue detuning or a red detuning.

5. The method of claim 1 , wherein the frequencies include at least a first frequency and a second frequency that is distinct from the first frequency.

6. The method of claim 5 , wherein the at least first frequency and second frequency are separated by a frequency separation configured to achieve a target coherence.

7. The method of claim 1 , wherein step c) further comprises polarizing the light fields in one or more directions.

8. The method of claim 1 , wherein step c) further comprises controlling a periodicity of the 2D optical array by modifying a magnification of projecting optical elements.

9. The method of claim 1 , wherein the 2D optical array comprises a grid of intersecting linear segments of light.

10. The method of claim 1 , wherein the linear segments of light extend substantially along a longitudinal direction defined by aspect ratios in a range between 15:1 and 2:1.

11. The method of claim 1 , wherein the linear segments of light are described by a Gaussian intensity profile along at least one transverse direction.

12. A system for controlling atomic particles using projected light, the system comprising:

a particle system including a plurality of atomic particles;

one or more optical sources configured to generate light fields using frequencies shifted from at least one atomic resonance; and

a plurality of optical elements configured to form, using the generated light fields, a two-dimensional (“2D”) optical array projected on the plurality of atomic particles, wherein the projected 2D optical array comprises linear segments of light that define locations for the plurality of atomic particles in space.

13. The system of claim 12 , wherein the particle system is configured to cool the plurality of atomic particles to temperatures in a range between 1 and 100 micro Kelvin.

14. The system of claim 12 , wherein the one or more sources are further configured to generate light fields using frequencies configured to achieve a blue detuning or a red detuning.

15. The system of claim 12 , wherein the frequencies include at least a first and a second frequency.

16. The system of claim 15 , wherein the at least first and second frequency are separated by a frequency separation configured to achieve a target coherence.

17. The system of claim 16 , wherein the detuning is in a range between 10 and 100 nanometers.

18. The system of claim 12 , wherein the plurality of optical elements are further configured to polarize the light fields in one or more directions.

19. The system of claim 12 , wherein the plurality of optical elements are further configured to control a periodicity of the 2D optical array by modifying a magnification of the plurality of optical elements.

20. The system of claim 12 , wherein the 2D optical array comprises a grid of intersecting linear segments of light.

21. The system of claim 12 , wherein the linear segments of light extend substantially along a longitudinal direction defined by aspect ratios in a range between 15:1 and 2:1.

22. The system of claim 12 , wherein the linear segments of light are described by a Gaussian intensity profile along at least one transverse direction.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 30, 2015
From: SAFFMAN, MARK; LICHTMAN, MARTIN
To: WISCONSIN ALUMNI RESEARCH FOUNDATION
Reel/Frame 034856/0608 →
Continuity (1)
Related Publication 20160064108A1 · Mar 3, 2016