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Simulation and analysis of quantum phase estimation algorithm in the presence of incoherent quantum noise channels
Quantum Physics · Submitted 28 Jul 2023
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The simulation results indicate that the standard deviation of the eigenvalue of the unitary operator has strong exponential dependence upon the error probability of individual qubits.
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The abstract, sentence by sentence
The quantum phase estimation (QPE) is one of the fundamental algorithms based on the quantum Fourier transform. It has applications in order-finding, factoring, and finding the eigenvalues of unitary operators. The major challenge in running QPE and other quantum algorithms is the noise in quantum computers. In the present work, we study the impact of incoherent noise on QPE, modeled as trace-preserving and completely positive quantum channels. Different noise models such as depolarizing, phase flip, bit flip, and bit-phase flip are taken to understand the performance of the QPE in the presence of noise. The simulation results indicate that the standard deviation of the eigenvalue of the unitary operator has strong exponential dependence upon the error probability of individual qubits. However, the standard deviation increases only linearly with the number of qubits for fixed error probability when that error probability is small.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The quantum phase estimation (QPE) is one of the fundamental algorithms based on the quantum Fourier transform. | background 1.00 | 0.03 | 0.02 | asserted 1.00 |
| s1 | It has applications in order-finding, factoring, and finding the eigenvalues of unitary operators. | background 1.00 | 0.04 | 0.02 | asserted 1.00 |
| s2 | The major challenge in running QPE and other quantum algorithms is the noise in quantum computers. | background 0.98 | 0.04 | 0.02 | asserted 1.00 |
| s3 | In the present work, we study the impact of incoherent noise on QPE, modeled as trace-preserving and completely positive quantum channels. | contribution 0.82 | 0.88 | 0.04 | asserted 0.95 |
| s4 | Different noise models such as depolarizing, phase flip, bit flip, and bit-phase flip are taken to understand the performance of the QPE in the presence of noise. | method 0.97 | 0.80 | 0.03 | asserted 0.90 |
| s5 | The simulation results indicate that the standard deviation of the eigenvalue of the unitary operator has strong exponential dependence upon the error probability of individual qubits. | result 1.00 | 0.93 | 0.67 | hedged possibility 0.80 |
| s6 | However, the standard deviation increases only linearly with the number of qubits for fixed error probability when that error probability is small. | result 0.99 | 0.91 | 0.27 | asserted 0.99 |
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Original abstract
The quantum phase estimation (QPE) is one of the fundamental algorithms based on the quantum Fourier transform. It has applications in order-finding, factoring, and finding the eigenvalues of unitary operators. The major challenge in running QPE and other quantum algorithms is the noise in quantum computers. In the present work, we study the impact of incoherent noise on QPE, modeled as trace-preserving and completely positive quantum channels. Different noise models such as depolarizing, phase flip, bit flip, and bit-phase flip are taken to understand the performance of the QPE in the presence of noise. The simulation results indicate that the standard deviation of the eigenvalue of the unitary operator has strong exponential dependence upon the error probability of individual qubits. However, the standard deviation increases only linearly with the number of qubits for fixed error probability when that error probability is small.
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This quantity is evaluated by rerunning the same experiment as in Fig. [ref] but with additional random noise: the ground state energies of the $H'_k$'s are now sampled according to normal distributions extracted from Table 1 and Fig. 2 of [ref] .
Algorithmic error mitigation for quantum eigenvalues estimation · $p$-th order mitigation of Trotter errors · 0.99
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