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Shadow Hamiltonian Simulation

Quantum Physics · Submitted 31 Jul 2024

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim This evolution can be simulated on a quantum computer efficiently under broad conditions.

how it is stated · asserted 0.92 read the record →

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arXiv ID2407.21775 (version 2)
Pith ID2A2V46S6, Pith's permanent record of this paper and its review
CitationRobbie King, Robin Kothari, Rolando D. Somma, Ryan Babbush, Thomas O'Brien. "Shadow Hamiltonian Simulation." arXiv:2407.21775 (2024). https://pith.science/paper/2A2V46S6
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 6,198 input tokens.

What the abstract itself states, as probabilities: claims first 0.21 · states limitation 0.24 · human participants 0.01 · controlled comparison 0.10 · randomized assignment 0.01 · states quantitative result 0.07 · compares with prior results 0.86 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

Simulating quantum dynamics is one of the most important applications of quantum computers. Traditional approaches for quantum simulation involve preparing the full evolved state of the system and then measuring some physical quantity. Here, we present a different and novel approach to quantum simulation that uses a compressed quantum state that we call the ``shadow state''. The amplitudes of this shadow state are proportional to the time-dependent expectations of a specific set of operators of interest, and it evolves according to its own Schr\"odinger equation. This evolution can be simulated on a quantum computer efficiently under broad conditions. Applications of this approach to quantum simulation problems include simulating the dynamics of exponentially large systems of free fermions or free bosons, the latter example recovering a recent algorithm for simulating exponentially many classical harmonic oscillators. These simulations are hard for classical methods and also for traditional quantum approaches, as preparing the full states would require exponential resources. Shadow Hamiltonian simulation can also be extended to simulate expectations of more complex operators such as two-time correlators or Green's functions, and to study the evolution of operators themselves in the Heisenberg picture.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Simulating quantum dynamics is one of the most important applications of quantum computers. background 1.00 0.04 0.02 asserted 1.00
s1 Traditional approaches for quantum simulation involve preparing the full evolved state of the system and then measuring some physical quantity. background 1.00 0.04 0.02 asserted 1.00
s2 Here, we present a different and novel approach to quantum simulation that uses a compressed quantum state that we call the ``shadow state''. contribution 0.99 0.91 0.30 asserted 1.00
s3 The amplitudes of this shadow state are proportional to the time-dependent expectations of a specific set of operators of interest, and it evolves according to its own Schr\"odinger equation. method 0.73 0.78 0.16 asserted 1.00
s4 This evolution can be simulated on a quantum computer efficiently under broad conditions. result 0.54 0.70 0.24 asserted 0.92
s5 Applications of this approach to quantum simulation problems include simulating the dynamics of exponentially large systems of free fermions or free bosons, the latter example recovering a recent algorithm for simulating exponentially many classical harmonic oscillators. contribution 0.68 0.65 0.16 asserted 0.90
s6 These simulations are hard for classical methods and also for traditional quantum approaches, as preparing the full states would require exponential resources. gap 0.38 0.19 0.10 asserted 1.00
s7 Shadow Hamiltonian simulation can also be extended to simulate expectations of more complex operators such as two-time correlators or Green's functions, and to study the evolution of operators themselves in the Heisenberg picture. contribution 0.89 0.78 0.10 asserted 0.63

What kind of paper the classifier reports this is: method or tool 1.00 · evidence from proof or derivation 0.85.

What was examined, and what was not

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

Simulating quantum dynamics is one of the most important applications of quantum computers. Traditional approaches for quantum simulation involve preparing the full evolved state of the system and then measuring some physical quantity. Here, we present a different and novel approach to quantum simulation that uses a compressed quantum state that we call the ``shadow state''. The amplitudes of this shadow state are proportional to the time-dependent expectations of a specific set of operators of interest, and it evolves according to its own Schr\"odinger equation. This evolution can be simulated on a quantum computer efficiently under broad conditions. Applications of this approach to quantum simulation problems include simulating the dynamics of exponentially large systems of free fermions or free bosons, the latter example recovering a recent algorithm for simulating exponentially many classical harmonic oscillators. These simulations are hard for classical methods and also for traditional quantum approaches, as preparing the full states would require exponential resources. Shadow Hamiltonian simulation can also be extended to simulate expectations of more complex operators such as two-time correlators or Green's functions, and to study the evolution of operators themselves in the Heisenberg picture.

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References
How the literature uses it

4 arXiv papers cite this in 7 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 2 sentences without a confident label

Uses its method or tool 3 papers
Cites it as background 1 paper
  • Classical shadows has recently emerged as a powerful framework for learning the expectation values of a large number of operators from few copies of a state $ρ$ of interest [ref] .

    Real classical shadows · Introduction · 1.00

What it cites · 3 sentences without a confident label

Compares with 1 paper
  • We note that our shadow Hamiltonian simulation approach for this example is clearly different from other approaches aimed at simulating bosonic field theories formulated in the Schrödinger picture approach [ref] .

    Quantum simulations of one dimensional quantum systems · Free bosons · 1.00

Cites as background 4 papers
  • A plethora of Hamiltonian simulation algorithms exist, with various complexities in terms of the relevant problem parameters, including the time $t$, the error $ϵ$ to which the final state is prepared, and intrinsic properties of the Hamiltonian such as the magnitude of interaction strengths (cf. [ref] ).

    Hamiltonian simulation for low-energy states with optimal time dependence · Introduction · 1.00

  • A plethora of Hamiltonian simulation algorithms exist, with various complexities in terms of the relevant problem parameters, including the time $t$, the error $ϵ$ to which the final state is prepared, and intrinsic properties of the Hamiltonian such as the magnitude of interaction strengths (cf. [ref] ).

    A Simple Proof that Toffoli and Hadamard are Quantum Universal · Introduction · 1.00

  • Depending on the choice of operator basis, this unitary may also be called the super-operator [ref] or Pauli transfer matrix [ref] .

    Tensor networks and graphical calculus for open quantum systems · Comparison with the transfer matrix method · 0.94

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