Quantum Error-Corrected Computation of Molecular Energies

Fuente: arXiv
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Main Authors: Yamamoto, Kentaro, Kikuchi, Yuta, Amaro, David, Criger, Ben, Dilkes, Silas, Ryan-Anderson, Ciarán, Tranter, Andrew, Dreiling, Joan M., Gresh, Dan, Foltz, Cameron, Mills, Michael, Moses, Steven A., Siegfried, Peter E., Urmey, Maxwell D., Burau, Justin J., Hankin, Aaron, Lucchetti, Dominic, Gaebler, John P., Brown, Natalie C., Neyenhuis, Brian, Ramo, David Muñoz
Format: Preprint
Published: 2025
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author Yamamoto, Kentaro
Kikuchi, Yuta
Amaro, David
Criger, Ben
Dilkes, Silas
Ryan-Anderson, Ciarán
Tranter, Andrew
Dreiling, Joan M.
Gresh, Dan
Foltz, Cameron
Mills, Michael
Moses, Steven A.
Siegfried, Peter E.
Urmey, Maxwell D.
Burau, Justin J.
Hankin, Aaron
Lucchetti, Dominic
Gaebler, John P.
Brown, Natalie C.
Neyenhuis, Brian
Ramo, David Muñoz
author_facet Yamamoto, Kentaro
Kikuchi, Yuta
Amaro, David
Criger, Ben
Dilkes, Silas
Ryan-Anderson, Ciarán
Tranter, Andrew
Dreiling, Joan M.
Gresh, Dan
Foltz, Cameron
Mills, Michael
Moses, Steven A.
Siegfried, Peter E.
Urmey, Maxwell D.
Burau, Justin J.
Hankin, Aaron
Lucchetti, Dominic
Gaebler, John P.
Brown, Natalie C.
Neyenhuis, Brian
Ramo, David Muñoz
contents We present the first demonstration of an end-to-end pipeline with quantum error correction (QEC) for a quantum computation of the electronic structure of molecular systems. We calculate the ground-state energy of molecular hydrogen, using quantum phase estimation (QPE) on qubits encoded with the $[[7,1,3]]$ color code on Quantinuum H2-2. We obtain improvements in computational fidelity by (1) introducing several partially fault-tolerant (FT) techniques for the Clifford+$R_{Z}$ (arbitrary-angle single-qubit rotation) gate set, and (2) integrating Steane QEC gadgets for real-time error correction. In particular, the latter enhances the QPE circuits' performance despite the complexity of the extra QEC circuitry. The encoded circuits contain up to 1585 (546) fixed and 7202 (1702) conditional physical two-qubit gates (mid-circuit measurements), and $\sim$3900 ($\sim$760) total operations are applied on average. The energy $E$ is experimentally estimated to within $E - E_{\mathrm{FCI}} = 0.001(13)$ hartree, where $E_{\mathrm{FCI}}$ denotes the exact ground state energy within the given basis set. Additionally, we conduct numerical simulations with tunable noise parameters to identify the dominant sources of noise. We find that orienting the QEC protocols towards higher memory noise protection is the most promising avenue to improve our experimental results.
format Preprint
id arxiv_https___arxiv_org_abs_2505_09133
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Quantum Error-Corrected Computation of Molecular Energies
Yamamoto, Kentaro
Kikuchi, Yuta
Amaro, David
Criger, Ben
Dilkes, Silas
Ryan-Anderson, Ciarán
Tranter, Andrew
Dreiling, Joan M.
Gresh, Dan
Foltz, Cameron
Mills, Michael
Moses, Steven A.
Siegfried, Peter E.
Urmey, Maxwell D.
Burau, Justin J.
Hankin, Aaron
Lucchetti, Dominic
Gaebler, John P.
Brown, Natalie C.
Neyenhuis, Brian
Ramo, David Muñoz
Quantum Physics
We present the first demonstration of an end-to-end pipeline with quantum error correction (QEC) for a quantum computation of the electronic structure of molecular systems. We calculate the ground-state energy of molecular hydrogen, using quantum phase estimation (QPE) on qubits encoded with the $[[7,1,3]]$ color code on Quantinuum H2-2. We obtain improvements in computational fidelity by (1) introducing several partially fault-tolerant (FT) techniques for the Clifford+$R_{Z}$ (arbitrary-angle single-qubit rotation) gate set, and (2) integrating Steane QEC gadgets for real-time error correction. In particular, the latter enhances the QPE circuits' performance despite the complexity of the extra QEC circuitry. The encoded circuits contain up to 1585 (546) fixed and 7202 (1702) conditional physical two-qubit gates (mid-circuit measurements), and $\sim$3900 ($\sim$760) total operations are applied on average. The energy $E$ is experimentally estimated to within $E - E_{\mathrm{FCI}} = 0.001(13)$ hartree, where $E_{\mathrm{FCI}}$ denotes the exact ground state energy within the given basis set. Additionally, we conduct numerical simulations with tunable noise parameters to identify the dominant sources of noise. We find that orienting the QEC protocols towards higher memory noise protection is the most promising avenue to improve our experimental results.
title Quantum Error-Corrected Computation of Molecular Energies
topic Quantum Physics
url https://arxiv.org/abs/2505.09133