Estimation of an expected energy value of a Hamiltonian
Systems, computer-implemented methods, and computer program products to facilitate estimation of an expected energy value of a Hamiltonian based on data of the Hamiltonian, the quantum state produced by a quantum device and/or entangled measurements are provided. According to an embodiment, a system can comprise a memory that stores computer executable components and a processor that executes the computer executable components stored in the memory. The computer executable components can comprise a selection component that selects a quantum state measurement basis having a probability defined based on a ratio of a Pauli operator in a Hamiltonian of a quantum system. The computer executable components can further comprise a measurement component that captures a quantum state measurement of a qubit in the quantum system based on the quantum state measurement basis.
1. A quantum system, comprising:
a memory;
a quantum processor that generates quantum states; and
a processor operably coupled to the memory, wherein the processor:
obtains a Hamiltonian of the quantum system;
selects a quantum state measurement basis having a probability defined based on a ratio of a Pauli operator in the Hamiltonian of the quantum system; and
determines a quantum state measurement of a qubit in the quantum system based on the quantum state measurement basis.
2. The quantum system of claim 1 , wherein the quantum state measurement basis comprises a basis state of at least one of a stabilizer state, a single qubit stabilizer state, or multiqubit quantum states that span quantum states comprising a defined number of nonidentity Pauli matrices, and wherein the Hamiltonian comprises a sum of weighted Pauli strings comprising the defined number of the nonidentity Pauli matrices.
3. The quantum system of claim 1 , wherein processor determines the quantum state measurement of the qubit based on the quantum state measurement basis to reduce at least one of: a number of quantum state measurements of the qubit used to compute an expected energy value of the Hamiltonian; or execution time of the quantum system to execute a variational quantum eigensolver algorithm.
4. The quantum system of claim 1 , wherein the processor also generates a product quantum state based on quantum state measurements of the qubit determined based on multiple quantum state measurement bases.
5. The quantum system of claim 1 , wherein the processor also computes an expected energy value of the Hamiltonian based on a product quantum state generated based on quantum state measurements of the qubit determined based on multiple quantum state measurement bases.
6. A computer-implemented method, comprising:
obtaining, by a quantum system operatively coupled to a processor, a Hamiltonian of the quantum system;
selecting, by the quantum system, a quantum state measurement basis having a probability defined based on a ratio of a Pauli operator in the Hamiltonian of the quantum system; and
determining, by the quantum system, a quantum state measurement of a qubit in the quantum system based on the quantum state measurement basis.
7. The computer-implemented method of claim 6 , wherein the quantum state measurement basis comprises a basis state of at least one of a stabilizer state, a single qubit stabilizer state, or multiqubit quantum states that span quantum states comprising a defined number of nonidentity Pauli matrices, and wherein the Hamiltonian comprises a sum of weighted Pauli strings comprising the defined number of the nonidentity Pauli matrices.
8. The computer-implemented method of claim 6 , wherein the determining comprises:
determining, by the quantum system, the quantum state measurement of the qubit in the quantum system based on the quantum state measurement basis to reduce at least one of: a number of quantum state measurements of the qubit used to compute an expected energy value of the Hamiltonian; or execution time of the quantum system to execute a variational quantum eigensolver algorithm.
9. The computer-implemented method of claim 6 , further comprising:
generating, by the quantum system, a product quantum state based on quantum state measurements of the qubit determined based on multiple quantum state measurement bases.
10. The computer-implemented method of claim 6 , further comprising:
computing, by the quantum system, an expected energy value of the Hamiltonian based on a product quantum state generated based on quantum state measurements of the qubit determined based on multiple quantum state measurement bases.
11. A computer program product facilitating a process to estimate an expected energy value of a Hamiltonian, the computer program product comprising a computer readable storage medium having program instructions embodied therewith, the program instructions executable by a processor to cause the processor to:
obtain, by the processor, the Hamiltonian of a quantum system;
select, by the processor, a quantum state measurement basis having a probability defined based on a ratio of a Pauli operator in the Hamiltonian of the quantum system; and
determine, by the processor, a quantum state measurement of a qubit in the quantum system based on the quantum state measurement basis.
12. The computer program product of claim 11 , wherein the quantum state measurement basis comprises a basis state of at least one of a stabilizer state, a single qubit stabilizer state, or multiqubit quantum states that span quantum states comprising a defined number of nonidentity Pauli matrices, and wherein the Hamiltonian comprises a sum of weighted Pauli strings comprising the defined number of the nonidentity Pauli matrices.
13. The computer program product of claim 11 , wherein the program instructions are further executable by the processor to cause the processor to:
determine, by the processor, the quantum state measurement of the qubit in the quantum system based on the quantum state measurement basis to reduce at least one of: a number of quantum state measurements of the qubit used to compute an expected energy value of the Hamiltonian; or execution time of the quantum system to execute a variational quantum eigensolver algorithm.
14. The computer program product of claim 11 , wherein the program instructions are further executable by the processor to cause the processor to:
generate, by the processor, a product quantum state based on quantum state measurements of the qubit determined based on multiple quantum state measurement bases.
15. The computer program product of claim 11 , wherein the program instructions are further executable by the processor to cause the processor to:
compute, by the processor, an expected energy value of the Hamiltonian based on a product quantum state generated based on quantum state measurements of the qubit determined based on multiple quantum state measurement bases.