Constructing and programming quantum hardware for robust quantum annealing processes
US-10346760-B2 · Jul 9, 2019 · US
US10789541B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10789541-B2 |
| Application number | US-202016853463-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 20, 2020 |
| Priority date | Jan 6, 2014 |
| Publication date | Sep 29, 2020 |
| Grant date | Sep 29, 2020 |
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Methods, systems, and apparatus, including computer programs encoded on computer storage media, for constructing and programming quantum hardware for quantum annealing processes.
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What is claimed is: 1. A method comprising: configuring a first logical superconducting unit and a second logical superconducting unit that form a first pair of logical superconducting units for use in computation to each have quantum states that can be spanned over Pauli operator σ sj i , where i=x, y, or z; configuring a first control superconducting unit and a second control superconducting unit that form a first pair of control superconducting units for use in assisting the computation without being a computational unit to each have quantum states that can be spanned over Pauli operator σ ck i , where i=x, y, or z; coupling the first logical superconducting unit and the second control superconducting unit by applying a magnetic field along the z direction; and coupling the second logical superconducting unit and the first control superconducting unit by applying a magnetic field along the z direction. 2. The method of claim 1 , wherein: when applying the magnetic field to the first logical superconducting unit and the second control superconducting unit, a quantum operator σ s1 z of the first logical superconducting unit is coupled with a quantum operator σ c2 z of the second control superconducting unit in a first coupling represented by σ s1 x σ s2 z ; and when applying the magnetic field to the second logical superconducting unit and the first control superconducting unit, the magnetic field couples a quantum operator σ s2 z of the first control superconducting unit with a quantum operator σ c1 z of the second logical superconducting unit in a second coupling represented by σ s2 x σ c1 z . 3. The method of claim 1 , wherein the first and second logical superconducting units and first and second control superconducting units comprise superconducting qubits having binary quantum states. 4. The method of claim 1 , wherein the logical superconducting units have the same precision as the control superconducting units. 5. The method of claim 1 , wherein the control superconducting units have less precision than the logical superconducting units. 6. The method of claim 1 , wherein the superconducting units and the couplings are configured such that a quantum Hamiltonian characterizing the superconducting units and the couplers is: H tot = I ( t ) ∑ i N σ i x + G ( t ) ( ∑ i = 1 N G h i G σ i z + ∑ i , j = 1 N G J ij G σ i z σ j z + ∑ i = 1 N G ∑ j = 1 N A J ij GA σ i z σ j z ) + P ( t ) ( - ∑ i N h i σ i z
Probabilistic graphical models, e.g. probabilistic networks · CPC title
having three or more electrodes, e.g. transistor-like structures · CPC title
Josephson-effect devices · CPC title
Physical realisations or architectures of quantum processors or components for manipulating qubits, e.g. qubit coupling or qubit control · CPC title
Quantum error correction, detection or prevention, e.g. surface codes or magic state distillation · CPC title
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