Quantum otto engine

Patent metadata

Field	Value
Publication number	US-9909460-B2
Application number	US-201615008263-A
Country	US
Kind code	B2
Filing date	Jan 27, 2016
Priority date	Jan 29, 2015
Publication date	Mar 6, 2018
Grant date	Mar 6, 2018

Abstract

Systems and methods for operating a quantum Otto cycle, including a superconducting LC resonator circuit electrically coupled to an input control unit with a reservoir source and a waveform generator configured to generate a bias current. A superconducting flux qubit is coupled to the LC resonator via a superconducting quantum interference device (“SQUID”). The SQUID generates a flux in the presence of the bias current, and the flux generated by the SQUID mediates a coupling rate between the flux qubit and the LC resonator. The waveform generator alternates the bias current to adiabatically change the coupling rate between the flux qubit and the LC resonator during adiabatic stages of the quantum Otto cycle. The reservoir source sends pulses to thermalize the flux qubit and the LC resonator system during isochoric stages of the quantum Otto cycle.

First claim

What is claimed is:

1. A system for operating a quantum Otto cycle, comprising:
a superconducting LC resonator circuit electrically coupled to an input control unit, the input control unit including a reservoir source and a waveform generator configured to generate a bias current;
a superconducting flux qubit having at least two states tunably coupled to the LC resonator via a superconducting quantum interference device (“SQUID”), wherein the SQUID generates a flux in the presence of the bias current, and wherein the flux generated by the SQUID mediates a coupling rate between the superconducting flux qubit and the superconducting LC resonator;
a seed coherence control unit inductively coupled to the superconducting flux qubit and adapted to produce a DC flux bias to couple the at least two qubit states; and
a dilution refrigerator chamber for housing the superconducting flux qubit and the superconducting LC resonator;
wherein the waveform generator is configured to alternate the bias current to adiabatically change the coupling rate between the superconducting flux qubit and the superconducting LC resonator during adiabatic stages of the quantum Otto cycle; and
wherein the reservoir source is configured to send pulses to thermalize the superconducting flux qubit and the superconducting LC resonator system during isochoric stages of the quantum Otto cycle.

2. The quantum heat engine of claim 1 , wherein the reservoir source comprises a quasi thermal field source.

3. The quantum heat engine of claim 2 , wherein the quasi thermal field source is thermally coupled to a first thermal reservoir having temperature TL and a second thermal reservoir having temperature TH, and wherein the quasi thermal field source is configured to send a first pulse to thermalize the superconducting flux qubit and the superconducting LC resonator system to temperature TL during a first isochoric stage of the quantum Otto cycle and configured to send a second pulse to thermalize the superconducting flux qubit and the superconducting LC resonator system to temperature TH during a second isochoric stages of the quantum Otto cycle.

4. The quantum heat engine of claim 1 , wherein the reservoir source comprises at least one quantum reservoir characterized by a physical temperature parameter and a quantum parameter.

5. The quantum heat engine of claim 4 , wherein the quantum reservoir is further characterized by an effective temperature, wherein the effective temperature is based on the physical temperature and the quantum parameter, and wherein the effective temperature is higher than the physical temperature.

6. The quantum heat engine of claim 4 , wherein the quantum reservoir comprises one or more of an ensemble of thermal squeezed photons or coherent photons, or a single qubit or qutrit with quantum coherence.

7. The quantum heat engine of claim 4 , wherein the quantum reservoir is adapted to thermalize the superconducting flux qubit and the superconducting LC resonator system by injecting coherence using the seed coherence control unit and coupling the quantum reservoir to the superconducting flux qubit and the superconducting LC resonator system.

8. A method for operating a quantum Otto cycle using a qubit-resonator system comprising a superconducting flux qubit having at least two qubit states tunably coupled to a superconducting LC resonator via a superconducting quantum interference device (“SQUID”), comprising:
cooling the qubit-resonator system to its ground state using a dilution refrigerator chamber;
applying a DC flux bias using a seed coherence control unit to couple the at least two qubit states of the superconducting flux qubit;
thermalizing the qubit-resonator system to a first temperature such that a plurality of first energy levels of the qubit-resonator system have first occupation probabilities;
adiabatically shifting the first energy levels of the qubit-resonator system to a second plurality of second energy levels by applying a bias current to the SQUID to vary the coupling rate between the superconducting flux qubit and the superconducting LC resonator from a first coupling rate to a second coupling rate;
thermalizing the qubit-resonator system to a second temperature such that the second energy levels have second occupation probabilities;
adiabatically shifting the second energy levels of the qubit-resonator system back to the first energy levels by altering the bias current to the SQUID to vary the coupling rate between the superconducting flux qubit and the superconducting LC resonator from the second coupling rate to the first coupling rate.

9. The method of claim 8 , wherein thermalizing the qubit-resonator system to the first temperature includes thermally coupling the qubit-resonator system to a thermal reservoir having a temperature equal to the first temperature.

10. The method of claim 8 , wherein thermalizing the qubit-resonator system to the second temperature includes thermally coupling the qubit-resonator system to a thermal reservoir having a temperature equal to the second temperature.

11. The method of claim 8 , wherein at least one of thermalizing the qubit-resonator system to the first temperature and thermalizing the qubit-resonator system to the second temperature includes coupling the qubit-resonator system to a quantum reservoir characterized by a physical temperature parameter and a quantum parameter.

12. The method of claim 11 , wherein the quantum reservoir is further characterized by an effective temperature, wherein the effective temperature is based on the physical temperature and the quantum parameter, and wherein the effective temperature is higher than the physical temperature.

13. The method of claim 11 , wherein the quantum reservoir comprises one or more of an ensemble of thermal squeezed photons or coherent photons, or a single qubit or qutrit with quantum coherence.

14. The method of claim 11 , wherein the quantum reservoir is adapted to thermalize the qubit-resonator system by injecting coherence using the seed coherence control unit and coupling the quantum reservoir to the superconducting flux qubit and the superconducting LC resonator system.

15. A method for operating a quantum Otto cycle using a qubit-resonator system comprising a superconducting flux qubit having at least two qubit states tunably coupled to a superconducting LC resonator, comprising:
cooling the qubit-resonator system to its ground state using a dilution refrigerator chamber;
applying a DC flux bias using a seed coherence control unit to couple the at least two qubit states of the superconducting flux qubit;
thermalizing the qubit-resonator system to a first temperature such that a plurality of first energy levels of the qubit-resonator system have first occupation probabilities;
adiabatically shifting the first energy levels of the qubit-resonator system to a plurality of second energy levels by applying an external magnetic flux to vary the excitation frequency of the superconducting LC resonator from a first excitation frequency to a second excitation frequency;
thermalizing the qubit-resonator system to a second temperature such that the second energy levels have second occupation probabilities;
adiabatically shifting the second energy levels of the qubit-resonator system back to the first energy levels by altering the external magnetic flux to vary the excitation frequency of the superconducting LC resonator from the second excitation frequency to the first excitation frequency.

16. The method of claim 15 , wherein thermalizing the qubit-resonator system to the first temperature i

Assignees

• Lockheed Corp
• Univ Koc

Inventors

• Allen Edward Henry
• Altintas Ferdi
• Hardal Ali U Cemal
• Muestecaplioglu Oezguer

Classifications

• B82Y99/00

  Subject matter not provided for in other groups of this subclass · CPC title

• F01K13/00 Primary

  General layout or general methods of operation of complete plants · CPC title

• G01R33/035 Primary

  using superconductive devices · CPC title

• G01R33/1284

  Spin resolved measurements; Influencing spins during measurements, e.g. in spintronics devices · CPC title

• G01R33/0354

  SQUIDS · CPC title