Systems and methods for enhanced eigenvalue inversion using quantum conditional logic
Embodiments use quantum conditional logic in the Quantum Phase Estimation Algorithm (QPEA) to compute eigenvalues prior to inversion. Embodiments estimate the eigenvalues of a unitary, U=e iÂt , generated by a N×N Hermitian matrix Â. The binary representations of the n-bit estimations of eigenvalues of  may be encoded in these states: |λ i =|b 1 b 2 . . . b n ; λ i is an estimation of the i-th eigenvalue, excluding degeneracy, and .b 1 b 2 . . . b n is its binary representation. To perform the eigenvalue inversion, an n-qubit controlled Ry rotation with angle λ i /2 (n−1) conditioned on seeing |b 1 b 2 . . . b n is applied for each possible n-bit binary string b 1 b 2 . . . b n (2 n values). The overall unitary is called a “uniformly controlled Ry rotation” in literature.
1. A classical computer, comprising:
a computer processor; and
a memory storing a classical computer program;
wherein the classical computer program is configured to generate a quantum computer program comprising instructions to:
initialize a register to an initial state;
initialize an ancilla qubit and apply a Hadamard gate to the ancilla qubit;
determine a number of iterations n to estimate n-bit eigenvalues;
perform a first unitary gate raised to 2 n−1 and controlled by the ancilla qubit;
perform a Hadamard gate on the ancilla qubit;
measure the ancilla qubit and save in a classical register C 0 ;
clear the ancilla qubit;
initialize a counter i to n−2;
perform a second unitary gate raised to 2 i and controlled by the ancilla qubit;
perform a phase gate on the ancilla qubit conditioned on a value in a classical register C (n−1)−i−1 and apply a Hadamard gate on the ancilla qubit;
measure the ancilla qubit and save in a classical register C (n−1)−i ;
clear the ancilla qubit; and
decrease i by 1 and repeating the performing of the second unitary gate, the performing of the phase gate, the applying of the Hadamard gate,
the measuring of the ancilla qubit, the saving of the ancilla qubit, and the decreasing of i by 1 until i is equal to zero;
wherein the classical computer program sends the quantum computer program to a quantum computer, the quantum computer executes the quantum computer program, receives results from the quantum computer in the classical registers C 0 , C 1 , . . . C n−1 , and outputs the results.
2. The classical computer of claim 1 , wherein the results from the quantum computer in the classical registers C 0 , C 1 , . . . C n−1 are binaries of the n-bit eigenvalues.
3. A method for n-bit eigenvalue estimation, comprising:
receiving, by a quantum computer, a quantum computer program from a classical computer;
initializing, by the quantum computer program, a register on the quantum computer to an initial state;
initializing, by a quantum computer program, an ancilla qubit and apply a Hadamard gate to the ancilla qubit;
determining, by a quantum computer program, a number of iterations n to estimate n-bit eigenvalues;
performing, by a quantum computer program, a first unitary gate raised to 2 n−1 and controlled by the ancilla qubit;
performing, by a quantum computer program, a Hadamard gate on the ancilla qubit;
measuring, by a quantum computer program, the ancilla qubit and save in a classical register C 0 ;
clearing, by a quantum computer program, the ancilla qubit;
initializing, by a quantum computer program, a counter i to n−2;
performing, by a quantum computer program, a second unitary gate raised to 2 i and controlled by the ancilla qubit;
performing, by a quantum computer program, a phase gate on the ancilla qubit conditioned on a value in a classical register C (n−1)−i−1 and apply a Hadamard gate on the ancilla qubit;
measuring the ancilla qubit and save in a classical register C (n−1)−i ;
clearing the ancilla qubit;
decreasing i by 1 and repeating the performing of the second unitary gate, the performing of the phase gate, the applying of the Hadamard gate, the measuring of the ancilla qubit, the saving of the ancilla qubit, and the decreasing of i by 1 until i is equal to zero; and
outputting the classical registers C 0 , C 1 , . . . C n−1 to the classical computer, wherein the classical registers C 0 , C 1 , . . . C n−1 comprise the n-bit eigenvalues.
4. A system, comprising:
a classical computer comprising a memory storing a classical computer program, wherein the classical computer program is configured to generate a quantum computer program comprising instructions to:
initialize a register in the quantum computer to an initial state;
initialize an ancilla qubit and apply a Hadamard gate to the ancilla qubit;
determine a number of iterations n to estimate n-bit eigenvalues;
perform a first unitary gate raised to 2 n−1 and controlled by the ancilla qubit;
perform a Hadamard gate on the ancilla qubit;
measure the ancilla qubit and save in a classical register C 0 ;
clear the ancilla qubit;
initialize a counter i to n−2;
perform a second unitary gate raised to 2 i and controlled by the ancilla qubit;
perform a phase gate on the ancilla qubit conditioned on a value in a classical register C (n−1)−i−1 and apply a Hadamard gate on the ancilla qubit;
measure the ancilla qubit and save in a classical register C (n−1)−i ;
clear the ancilla qubit; and
decrease i by 1 and repeating the performing of the second unitary gate, the performing of the phase gate, the applying of the Hadamard gate, the measuring of the ancilla qubit, the saving of the ancilla qubit, and the decreasing of i by 1 until i is equal to zero;
a quantum computer that is configured to receive the quantum computer program from the classical computer, to execute the quantum computer program, and to output the classical registers C 0 , C 1 , . . . C n−1 to the classical computer program, wherein the classical registers C 0 , C 1 , . . . C n−1 comprise the n-bit eigenvalues.