Hamiltonian simulation of minimal holographic sparsified SYK model

The circuit complexity for Hamiltonian simulation of the sparsified SYK model with N Majorana fermions and q = 4 (quartic interactions), which retains holographic features (referred to as ‘minimal holographic sparsified SYK’) with k ≪ N 3 / 24 (where k is the total number of interaction terms times 1/ N ) using the second-order Trotter method and Jordan-Wigner encoding is found to be O ˜ ( k α N 3 / 2 log ⁡ N ( J t ) 3 / 2 ε − 1 / 2 ) where t is the simulation time, ε is the desired error in the implementation of the unitary U = exp ⁡ ( − i H t ) measured by the operator norm, J is the disorder strength, and constant α < 1 . This complexity implies that with less than a hundred logical qubits and about 10 6 gates, it might be possible to achieve an advantage in this model and simulate real-time dynamics.

Authors

Institutions

Publication Details

Journal
Nuclear Physics B
Published
2025-02-04
DOI
https://doi.org/10.1016/j.nuclphysb.2025.116815
Citations
3
Primary Topic
Quantum Computing Algorithms and Architecture
Type
article
Field-Weighted Citation Impact
7.44

Funders

Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

Hamiltonian simulation of minimal holographic sparsified SYK model

Raghav G. Jha
3 citations
Nuclear Physics B
Quantum Computing Algorithms and Architecture
7.44
article

Hamiltonian simulation of minimal holographic sparsified SYK model

Raghav G. Jha
article en
3 citations

Abstract

The circuit complexity for Hamiltonian simulation of the sparsified SYK model with N Majorana fermions and q = 4 (quartic interactions), which retains holographic features (referred to as ‘minimal holographic sparsified SYK’) with k ≪ N 3 / 24 (where k is the total number of interaction terms times 1/ N ) using the second-order Trotter method and Jordan-Wigner encoding is found to be O ˜ ( k α N 3 / 2 log ⁡ N ( J t ) 3 / 2 ε − 1 / 2 ) where t is the simulation time, ε is the desired error in the implementation of the unitary U = exp ⁡ ( − i H t ) measured by the operator norm, J is the disorder strength, and constant α < 1 . This complexity implies that with less than a hundred logical qubits and about 10 6 gates, it might be possible to achieve an advantage in this model and simulate real-time dynamics.

Nuclear Physics BVol. 1012
Thomas Jefferson National Accelerator Facility (US)
High Energy Physics
Openalex Percentile: Top 4%
Quantum Computing Algorithms and Architecture
7.44
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.

Hamiltonian simulation of minimal holographic sparsified SYK model — Raghav G. Jha · Nuclear Physics B (2025) | TGRS Research Map | TGRS