Broadband sympathetic electromagnetically-induced transparency (EIT) cooling

Patent metadata

Field	Value
Publication number	US-12317403-B2
Application number	US-202217812035-A
Country	US
Kind code	B2
Filing date	Jul 12, 2022
Priority date	Aug 2, 2021
Publication date	May 27, 2025
Grant date	May 27, 2025

Abstract

An atomic object confined in a particular region of an atomic object confinement apparatus is cooled using an S-to-P-to-D EIT cooling operation. A controller associated with the atomic object confinement apparatus controls first and second manipulation sources to respectively provide first and second manipulation signals to the particular region. The first manipulation signal is characterized by a first wavelength corresponding to a transition between an S manifold and a P manifold of a first component of the atomic object and detuned from the S-to-P transition by a first detuning. The second manipulation signal is characterized by a second wavelength corresponding to a transition between the P manifold and a D manifold of the first component and detuned from the P-to-D transition by a second detuning. The first and second detunings selected to establish a dark state associated with a two-photon transition between the S manifold and the D manifold.

First claim

That which is claimed:

1. A method for cooling an atomic object confined by an atomic object confinement apparatus, the method comprising:
controlling, by a controller associated with the atomic object confinement apparatus, a first manipulation source to provide a first manipulation signal to a particular region of the atomic object confinement apparatus; and
controlling, by the controller, a second manipulation source to provide a second manipulation signal to the particular region of the atomic object confinement apparatus,
wherein:
the atomic object to be cooled is located in the particular region of the atomic object confinement apparatus,
the first manipulation signal is characterized by a first wavelength corresponding to a transition between an S manifold and a P manifold of a first component of the atomic object and detuned from the transition between the S manifold and the P manifold by a first detuning,
the second manipulation signal is characterized by a second wavelength corresponding to a transition between the P manifold and a D manifold of the first component of the atomic object and detuned from the transition between P manifold and the D manifold by a second detuning, and
the first detuning and the second detuning are selected to establish a dark state associated with a two photon transition between the S manifold and the D manifold.

2. The method of claim 1 , wherein the atomic object is an ion crystal comprising two or more ions and the first component of the atomic object is at least one of the two or more ions of a first atomic object type.

3. The method of claim 2 , wherein the first component of the atomic object is configured for use as a coolant ion in a sympathetic cooling scheme for the ion crystal.

4. The method of claim 2 , wherein a second component of the atomic object is at least one of the two or more ions of a second atomic object type, the second atomic object type being different from the first atomic object type, and wherein the at least one of the two or more ions of the second atomic object type is configured for use as a qubit of a quantum computer comprising the atomic object confinement apparatus.

5. The method of claim 1 , wherein the first detuning and the second detuning are substantially equal.

6. The method of claim 1 , wherein a polarization of the first manipulation signal and a polarization of the second manipulation signal correspond to the two photon transition associated with the dark state.

7. The method of claim 1 , further comprising causing generation of a magnetic field having a magnetic field direction in the particular region of the atomic object confinement apparatus, wherein one of the atomic object or the particular region of the atomic object confinement apparatus defines an atomic object axis, and the magnetic field direction is transverse to the atomic object axis.

8. The method of claim 7 , wherein the magnetic field direction and the atomic object axis form an angle in a range of thirty to sixty degrees.

9. The method of claim 7 , wherein the first manipulation signal defines a first propagation direction which is transverse to the atomic object axis and the second manipulation signal defines a second propagation direction which is transverse to the atomic object axis.

10. The method of claim 9 , wherein the first manipulation signal and the second manipulation signal are not co-propagating and the magnetic field direction is transverse to both the first propagation direction and the second propagation direction.

11. The method of claim 10 , wherein both the first propagation direction and the second propagation direction are substantially perpendicular to the magnetic field direction.

12. The method of claim 9 , wherein (a) the polarization of the first manipulation signal is substantially transverse to a plane defined by the atomic object confinement apparatus, (b) the polarization of the second manipulation signal is substantially transverse to the plane defined by the atomic object confinement apparatus, and (c) the first propagation direction, the second propagation direction, and the magnetic field direction are respectively substantially parallel to the plane defined by the atomic object confinement apparatus.

13. An apparatus comprising at least one processor and memory storing computer-executable instructions, the computer-executable instructions configured to, when executed by the at least one processor, cause the apparatus to at least:
control a first manipulation source to provide a first manipulation signal to a particular region of an atomic object confinement apparatus; and
control a second manipulation source to provide a second manipulation signal to the particular region of the atomic object confinement apparatus,
wherein:
an atomic object is located within the particular region of the atomic object confinement apparatus,
the first manipulation signal and the second manipulation signal are configured to collectively cool the atomic object,
the first manipulation signal is characterized by a first wavelength corresponding to a transition between an S manifold and a P manifold of a first component of the atomic object and detuned from the transition between the S manifold and the P manifold by a first detuning,
the second manipulation signal is characterized by a second wavelength corresponding to a transition between the P manifold and a D manifold of the first component of the atomic object and detuned from the transition between P manifold and the D manifold by a second detuning, and
the first detuning and the second detuning are selected to establish a dark state associated with a two photon transition between the S manifold and the D manifold.

14. The apparatus of claim 13 , wherein (a) the apparatus is a controller of a quantum computer comprising the atomic object confinement apparatus, (b) the atomic object is an ion crystal comprising two or more ions and the first component of the atomic object is at least one of the two or more ions of a first atomic object type, and (c) the first component of the atomic object is configured for use as a coolant ion in a sympathetic cooling scheme for the ion crystal.

15. The apparatus of claim 14 , wherein a second component of the atomic object is at least one of the two or more ions of a second atomic object type, the second atomic object type being different from the first atomic object type, and wherein the at least one of the two or more ions of the second atomic object type is configured for use as a qubit of the quantum computer.

16. The apparatus of claim 13 , wherein a polarization of the first manipulation signal and a polarization of the second manipulation signal correspond to the two photon transition associated with the dark state.

17. The apparatus of claim 13 , wherein the computer-executable instructions are further configured to, when executed by the at least one processor, cause the apparatus to at least cause generation of a magnetic field having a magnetic field direction in the particular region of the atomic object confinement apparatus, wherein one of the atomic object or the particular region of the atomic object confinement apparatus defines an atomic object axis, and the magnetic field direction is transverse to the atomic object axis.

18. The apparatus of claim 17 , wherein the first manipulation signal defines a first propagation direction which is transverse to the atomic object axis and the second manipulation signal defines a second propagation direction which is transverse to the atomic obje

Assignees

• Quantinuum Llc

Inventors

• Feig Michael
• Estey Brian
• Gilbreth Christopher

Classifications

• G04F5/145

  using Coherent Population Trapping · CPC title

• G06N10/40

  Physical realisations or architectures of quantum processors or components for manipulating qubits, e.g. qubit coupling or qubit control · CPC title

• H05H3/04 Primary

  Acceleration by electromagnetic wave pressure · CPC title

• F25B23/003 Primary

  using selective radiation effect · CPC title