GLOBAL CONTROL FOR QUANTUM COMPUTING SYSTEMS
Systems and methods for controlling one or more qubits in a quantum processor are disclosed. The system comprises a quantum processor comprising one or more spin-based qubits; and a dielectric resonator positioned in proximity to the quantum processor. The dielectric resonator provides a magnetic field. The quantum processor is positioned in a portion of the magnetic field provided by the resonator such that the portion of the magnetic field controls the spin transitions of the one or more spin-based qubits of the quantum processor.
1 . A system for controlling one or more qubits in a quantum processor, the system comprising:
a quantum processor comprising one or more spin-based qubits; and
a dielectric resonator positioned in proximity to the quantum processor, the dielectric resonator providing a magnetic field, and
the quantum processor being positioned in a portion of the magnetic field provided by the dielectric resonator such that the portion of the magnetic field controls the spin transitions of the one or more spin-based qubits of the quantum processor.
2 . The system of claim 1 , wherein the multiple spin-based qubits of the quantum processor are operated and controlled by the portion of the magnetic field provided by the dielectric resonator at a cryogenic temperature.
3 . The system of claim 2 , wherein the cryogenic temperature is less than or equal to 4 Kelvin.
4 . The system of any one of claims 1 - 3 , wherein the dielectric resonator is made of a dielectric material having a dielectric constant that increases at a cryogenic temperature relative to at room temperature.
5 . The system of claim 4 , wherein the dielectric constant of the resonator is in a range of 1000 to 40,000 at the cryogenic temperature.
6 . The system of any one of claims 1 - 5 , wherein the portion of the magnetic field controlling the one or more spin-based qubits is a uniform AC magnetic field.
7 . The system of any one of claims 1 - 6 , wherein the portion of the magnetic field acts as a global magnetic field for simultaneously controlling a plurality of spin-based qubits of the quantum processor.
8 . The system of any one of claims 1 - 7 , wherein the dielectric resonator produces an electric field spatially separated from the magnetic field.
9 . The system of any one of claims 1 - 8 , wherein the magnetic field of the dielectric resonator is perpendicular to a surface of the resonator and is directed outwardly of the surface of the dielectric resonator.
10 . The system of claim 8 , wherein the electric field is confined away from the position of the quantum processor for minimising the interaction of the electric field with the one or more spin-based qubits, and on-chip measurement and control electronics of the quantum processor.
11 . The system of any one of claim 8 or 10 , wherein the electric field circulates within the resonator.
12 . The system of any one of claims 1 - 9 , wherein the dielectric resonator is made of a material from a class of compounds having a perovskite structure ( XII A 2+VI B 4+ X 2− 3 ).
13 . The system of claim 10 , wherein the dielectric resonator is made of potassium tantalate (KTaO 3 ) or strontium titanate (SrTiO 3 ).
14 . The system of any one of claims 1 - 13 , wherein the dielectric resonator provides a resonant mode volume of approximately 5×10 −7 m 3 .
15 . The system of any one of claims 1 - 14 , wherein the quantum processor is a solid-state semiconducting or superconducting quantum processor.
16 . The system of any one of claims 1 - 15 , wherein the dielectric resonator is in the form of a solid block of a dielectric material and the quantum processor is placed either above or below the dielectric resonator such that the one or more spin-based qubits of the quantum processor face towards the dielectric resonator to interact with the portion of the magnetic field provided by the dielectric resonator.
17 . The system of any one of claims 1 - 16 , wherein the system further comprises a tuneable coupling element to provide a microwave input signal to the dielectric resonator for generating the magnetic field.
18 . The system of any one of claims 1 - 17 , wherein the resonator has a quality factor Q having a value greater than 100 at cryogenic temperatures.
19 . The system of any one of claims 1 - 18 , wherein the frequency of the magnetic field produced by the resonator is in radio frequency range from 1.0 MHz to 1.0 GHz for controlling nuclear spins.
20 . The system of any one of claims 1 - 18 , wherein the frequency of the magnetic field produced by the resonator is in microwave frequency range which is in a range of 1.0 GHz to 100.0 GHz for controlling electron spins.
21 . A method for controlling one or more spin-based qubits in a quantum processor using the system of any one of claims 1 - 20 .