Systems and methods for implementing finite element modelling
A system and method of implementing finite element modeling on a quantum processor is discussed. A representation of a computational problem including a boundary value problem and problem grid points is received by one or more processors. The problem grid points are mapped to a Hilbert space of the qubits of the quantum processor. The boundary value problem is transformed into a problem Hamiltonian. Instructions are transmitted to the quantum processor to cause the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian. The wavefunction amplitudes of the final state are measured, and the wavefunction amplitudes of the final state are mapped onto the problem grid points based on the Hilbert space of the qubits.
1. A method of operation of a hybrid computing system comprising a digital processor and a quantum processor, the quantum processor comprising qubits, the method being performed by the digital processor, the method implementing a finite element model, the method comprising:
receiving a representation of a computational problem, the computational problem comprising a boundary value problem and problem grid points;
mapping the problem grid points to a Hilbert space of the qubits;
transforming the boundary value problem into a problem Hamiltonian;
causing the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian;
measuring the wavefunction amplitudes of the final state; and
mapping the wavefunction amplitudes of the final state onto the problem grid points based on the Hilbert space of the qubits.
2. The method of claim 1 , wherein transforming the boundary value problem into a problem Hamiltonian comprises generating qubit bias and coupler values.
3. The method of claim 2 , wherein causing the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian further comprises causing the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian and the qubit bias and coupler values.
4. The method of claim 1 , wherein measuring the wavefunction amplitudes of the final state comprises performing quantum process tomography.
5. The method of claim 1 , wherein causing the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian comprises causing the quantum processor to evolve piecewise over a Feynman path integral from the initial state to the final state.
6. The method of claim 1 , wherein causing the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian comprises causing the quantum processor to evolve through quantum annealing from an initial Hamiltonian to the problem Hamiltonian.
7. The method of claim 1 , wherein mapping the problem grid points to a Hilbert space of the qubits comprises:
determining all possible states of the qubits;
defining a set of vectors, wherein each vector in the set of vectors represents one of the possible states of the qubits; and
assigning each of the problem grid points to one of the vectors in the set of vectors.
8. A hybrid computing system for implementing finite element modeling on a quantum processor, comprising:
a quantum processor comprising qubits;
at least one non-transitory processor-readable medium that stores at least one of processor executable instructions and data; and
at least one digital processor communicatively coupled to the least one non-transitory processor-readable medium and the quantum processor, wherein the at least one digital processor, in response to execution of the at least one of processor executable instructions and data:
receives a representation of a computational problem, the computational problem comprising a boundary value problem and problem grid points;
maps the problem grid points to a Hilbert space of the qubits;
transforms the boundary value problem into a problem Hamiltonian;
causes the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian;
measures the wavefunction amplitudes of the final state over the Hilbert space of the qubits; and
maps the wavefunction amplitudes of the final state onto the problem grid points based on the Hilbert space of the qubits.
9. The system of claim 8 , wherein the at least one digital processor transforms the boundary value problem into a problem Hamiltonian and generates qubit bias and coupler values.
10. The system of claim 9 , wherein the at least one digital processor causes the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian and the qubit bias and coupler values.
11. The system of claim 8 , wherein the at least one digital processor measures the wavefunction amplitudes of the final state using quantum process tomography.
12. The system of claim 8 , wherein the at least one digital processor causes the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian by evolving piecewise over a Feynman path integral from the initial state to the final state.
13. The system of claim 8 , wherein the at least one digital processor causes the quantum processor to evolve from an initial state to a final state based on the problem Hamiltonian by performing quantum annealing from an initial Hamiltonian to the problem Hamiltonian.
14. The system of claim 8 , wherein to map the problem grid points to a Hilbert space of the qubits the at least one digital processor:
determines all possible states of the qubits;
defines a set of vectors, wherein each vector in the set of vectors represents one of the possible states of the qubits; and
assigns each of the problem grid points to one of the vectors in the set of vectors.