Randomized Quantum Phase Estimation With Single-Ancilla Sampling

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Solution Overview

Problem

Existing quantum computing methods for phase and energy level estimation are inefficient and require high gate complexity and qubit costs, especially for complex Hamiltonians, and suffer from biased errors that cannot be statistically suppressed.

Innovation Solution

A randomized quantum algorithm that combines statistical phase estimation with random compilation of quantum circuits, using a single ancilla and random gate sequences to suppress compilation errors through increased data sampling, optimizing gate complexity and qubit usage.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If existing quantum computing methods are used for phase and energy level estimation, then estimation capability is achieved, but gate complexity and qubit costs are high

Engineering Contradiction:
Improvephase and energy level estimation accuracyVSAvoidgate complexity and qubit costs
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The algorithm segments the Hamiltonian into multiple terms and processes them separately through random sampling. Instead of handling the entire complex Hamiltonian at once, the method divides it into manageable components that can be estimated individually and combined, reducing the gate complexity required for each measurement step.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The algorithm performs partial phase estimation by randomly sampling subsets of Hamiltonian terms rather than completing full estimation for all terms. This partial action approach achieves sufficient estimation accuracy with fewer quantum gates and qubits than traditional complete estimation methods.

Inventive Principle:
Principle #16Partial or excessive action

2Measurement precision

If existing quantum computing methods are used for phase and energy level estimation, then estimation capability is achieved, but biased errors cannot be suppressed

Engineering Contradiction:
Improveestimation accuracyVSAvoiderror suppression capability
Core Design Contradiction:
Measurement precisionVSReliability

Solution Approach 1:

The algorithm incorporates feedback through random sampling and statistical analysis. By repeatedly sampling different Hamiltonian term combinations and using statistical methods to aggregate results, the system identifies and suppresses biased errors, improving the reliability of phase and energy level estimates.

Inventive Principle:
Principle #23Feedback

Solution Approach 2:

The method changes the parameters of the quantum algorithm by using random sampling distributions and varying the number of samples. This parameter variation allows statistical error suppression techniques to be applied, transforming systematic biased errors into reducible statistical fluctuations.

Inventive Principle:
Principle #35Parameter changes

3Measurement precision

If more qubits and gates are used for complex Hamiltonians, then estimation accuracy may improve, but computational efficiency decreases

Engineering Contradiction:
Improveestimation accuracyVSAvoidcomputational efficiency
Core Design Contradiction:
Measurement precisionVSProductivity

Solution Approach 1:

The algorithm performs sufficient but not excessive phase estimation by randomly sampling Hamiltonian terms. It achieves the necessary accuracy threshold without performing complete estimation on all terms, thereby maintaining computational efficiency while ensuring adequate measurement precision for complex Hamiltonians.

Inventive Principle:
Principle #16Partial or excessive action

Data Source

PatentUS12541566B1Randomized quantum algorithm for statistical phase estimation
Publication Date: 2026.02.03 AMAZON TECH INC
  • US12541566B1 patent drawing
  • US12541566B1 patent drawing
  • US12541566B1 patent drawing

AI summary

A system and method for estimating values of an operator, such as energy levels of a Hamiltonian, is disclosed. The estimation is performed in a way such that the runtime of performing the estimation is independent of a complexity of the operator, e.g., a number of terms in the Hamiltonian. Also, errors can be statistically suppressed by performing additional sampling, due to a lack of biased error in the estimator. Additionally, samples may be tested using only a single ancilla qubit.