Universal Quantum Simulators
Abstract
Feynman's 1982 conjecture, that quantum computers can be programmed to simulate any local quantum system, is shown to be correct.
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The quantum simulation algorithm runs in time polynomial in the size of the system being simulated and the desired evolution time, giving an exponential speedup over the best general classical algorithms known.
“The algorithm runs in time polynomial in the size of the system being simulated (the number of qubits) and the desired evolution time, giving an exponential speedup over the best general classical algorithms known.”
From Quantum algorithms: an overview (2016) · cites this paper as [44]
A general-purpose quantum computer can efficiently simulate quantum mechanics for many physically realistic cases, such as systems with locality restrictions on their interactions.
“A general-purpose quantum computer can indeed ef fi ciently simulate quantum mechanics in this sense for many physically realistic cases, such as systems with locality restrictions on their interactions. 44”
From Quantum algorithms: an overview (2016) · cites this paper as [44]
We can program quantum computers to simulate localized quantum systems.
“It is noteworthy that we can program quantum computers to simulate localized quantum systems [68].”
From Quantum Computing in the Next-Generation Computational Biology Landscape: From Protein Folding to Molecular Dynamics (2024) · cites this paper as [68]
With a universal approach, a wide range of quantum problems can be simulated to the desired accuracy with a polynomial increase in quantum resources only.
“With this universal approach, a wide range of quantum problems can be simulated to the desired accuracy with a polynomial increase in quantum resources only (Lloyd, 1996).”
From Noisy intermediate-scale quantum algorithms (2022) · cites this paper as Lloyd, 1996
The quantum computational cost of quantum chemistry algorithms has continued to be reduced.
“The quantum computational cost of these algorithms has continued to be reduced 47-50 .”
From Quantum Chemistry in the Age of Quantum Computing (2019) · cites this paper as [50]
It was demonstrated that the Trotter errors depend on the maximum nuclear charge rather than the number of spin-orbitals.
“Later, it was also demonstrated that the Trotter errors depend on the maximum nuclear charge rather than the number of spin-orbitals 50 .”
From Quantum Chemistry in the Age of Quantum Computing (2019) · cites this paper as [50]
The number of gates for the highly nonlocal coupling b†_1 b_10 + b†_10 b_1 can be as small as 10 per Trotter step with the proposed method, whereas in the general case it would require about 10^6 elementary gates.
“In the general case, it would require a number of elementary gates of 2 20 ≃ 10 6 [2]. With our method, the number of gates can be as small as 10 per Trotter step, consisting of Mølmer-Sørensen gates (dark blue and green), local exp( iφ ′ σ y 2 ) gates (red), exp[ ± i ( π/ 4) ∑ i σ y i ] (yellow) and exp[ ± i ( π/ 4) ∑ i σ x i ] (cyan) gates (see Fig. 1b) [35].”
From Quantum Simulation of Interacting Fermion Lattice Models in Trapped Ions (2012) · cites this paper as [2]
The resulting dynamics are decomposed in efficient steps with Trotter methods, yielding an overall protocol that employs only polynomial resources.
“We map products of fermionic operators onto nonlocal spin operators and decompose the resulting dynamics in efficient steps with Trotter methods, yielding an overall protocol that employs only polynomial resources.”
From Quantum Simulation of Interacting Fermion Lattice Models in Trapped Ions (2012) · cites this paper as [2]
For bounded Hamiltonians, the Trotter expansion associated with the exponential of the polynomial sum of efficiently implementable nonlocal terms is efficient, i.e., it only requires polynomial resources.
“Note that for bounded Hamiltonians, the Trotter expansion associated with the exponential of the polynomial sum of efficiently implementable nonlocal terms is also efficient [2, 29, 30], i.e., it only requires polynomial resources [35].”
From Quantum Simulation of Interacting Fermion Lattice Models in Trapped Ions (2012) · cites this paper as [2]
On a fault-tolerant computer, full-CI energy can be measured by preparing a wave function ansatz and applying Quantum Phase Estimation, which projects into an energy eigenstate.
“On a fault-tolerant computer, one may directly measure the full-CI energy by first preparing a wave function ansatz on the quantum hardware (as in VQE) and then applying the Quantum Phase Estimation algorithm, which projects a prepared state into an energy eigenstate of the Hamiltonian.[111,[132][133][134][135][136]”
From Quantum Computing for Molecular Biology** (2023) · cites this paper as [111]
A proposed solution is to use highly controlled laboratory quantum systems themselves to perform such simulations.
“A proposed solution is to use highly controlled laboratory quantum systems themselves to perform such simulations [1-3].”
From Quantum Simulation of the Klein Paradox with Trapped Ions (2011) · cites this paper as [2]
Simulating quantum mechanics using conventional computers rapidly becomes intractable as the physical systems to which it is applied grow larger.
“Simulating quantum mechanics using conventional computers rapidly becomes intractable as the physical systems to which it is applied grow larger.”
From Quantum Simulation of the Klein Paradox with Trapped Ions (2011) · cites this paper as [2]
According to the Lieb-Robinson theorem, after a sufficiently large time, states can become strongly entangled.
“Indeed, this fact is related to correlation and entanglement spreading according to the Lieb-Robinson theorem that states that, after a sufficiently large time, states can become strongly entangled ([91-96], see also [97]).”
From Can one trust quantum simulators? (2012) · cites this paper as [96]
Quantum dynamics is in general computationally hard.
“or that the quantum dynamics is in general computationally hard [96, 97].”
From Can one trust quantum simulators? (2012) · cites this paper as [96]
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“[2] S.”
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“First, one could exploit the natural decoherence of the simulator, as first suggested in (Lloyd, 1996) and investigated experimentally in (Tseng et al., 2000) (see also the discussion in Section V.”
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“itrary subsets, H = P jHj. The criteria for grouping can dier depending on the target Hamiltonian as shown below. The variational ansatz is dened as j#TAB#()i= YS b=1 UH j (b j):::UH 1( b 1) ! j 0i; (37) where j 0ican be chosen to match the desired symmetry properties of the target ground 84 state, UH k (b k) = exp b…”
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“(38)] is simulated by a digital expansion (Lloyd, 1996) by interleaving the different interactions.”
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“[5] Lloyd, S.”
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Ensemble quantum computing by NMR spectroscopy
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Goals and opportunities in quantum simulation
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Power of One Bit of Quantum Information
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Effective Quantum Spin Systems with Trapped Ions
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Atom-chip-based generation of entanglement for quantum metrology
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“With the experimental method presented here but with a more sophisticated analysis [9], the density matrix of arbitrary spin states that spread over the whole Bloch sphere can be reconstructed.”
MethodWeimer, H., Müller, M., Lesanovsky, I., Zoller, P., & Büchler, H. P. (2010) · Nature Physics · doi:10.1038/nphys1614 · Cited by 867 · see citing works
“For purely coherent dynamics governed by the Hamiltonian, this is the familiar‘digital quantum simulato”
MethodHamiltonian Simulation by Qubitization
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“The first explicit quantum algorithms were discovered by Lloyd [31] for local interactions, and then generalized by Aharonov and Ta-Shma [3] to sparse Hamiltonians.”
MethodQuantum Algorithm Providing Exponential Speed Increase for Finding Eigenvalues and Eigenvectors
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Self-citationExponential algorithmic speedup by a quantum walk
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Real-time dynamics of lattice gauge theories with a few-qubit quantum computer
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“This provides the tools for universal digital quantum simulation [16], where the time evolution of a quantum system is approximated as a stroboscopic sequence of quantum gates [17].”
MethodQuantum Algorithms for Quantum Chemistry and Quantum Materials Science
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Scalable Quantum Simulation of Molecular Energies
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“Universal and efficient simulation of physical systems [1] is among the most compelling applications of quantum”
BackgroundProgrammable quantum simulations of spin systems with trapped ions
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Programmable Quantum Simulations of Spin Systems with Trapped Ions
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Towards quantum chemistry on a quantum computer
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“The challenge of first-principles calculations arises because the computational resources required to obtain exact (that is, full configuration interaction) solutions of the Schrodinger equation on a conventional computer generally increase exponentially with the number of atoms involve”
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Entanglement and quantum computation with ions in thermal motion
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Optimal Hamiltonian Simulation by Quantum Signal Processing
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“[11] S. Lloyd, Science 273, 1073 (1996).”
BackgroundSimulation of Many-Body Fermi Systems on a Universal Quantum Computer
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Self-citationElucidating reaction mechanisms on quantum computers
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“[5] Seth Lloyd, “Universal quantum simulators,” Science 273, 1073 (1996).”
MethodQuantum error correction below the surface code threshold
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“Quantum computing promises computational speedups in quantum chemistry [5], quantum simulation [6], cryptography [7], and optimization [8].”
Simulating Hamiltonian Dynamics with a Truncated Taylor Series
Berry, D. W., Childs, A. M., Cleve, R., Kothari, R., & Somma, R. D. (2015) · Physical Review Letters · doi:10.1103/physrevlett.114.090502 · Cited by 742 · see citing works
Photonic quantum information processing: a review
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Matrix product states represent ground states faithfully
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Efficient Quantum Algorithms for Simulating Sparse Hamiltonians
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“Here we apply the higher-order integrators of Suzuki [12, 13] to reduce the temporal scaling from t 3 / 2 [5] or t 2 [4] to the slightly superlinear scaling t 1+1 / 2 k , where k is the order of the integrator and may be an arbitrarily large integer.”
BackgroundMethodInfluentialEfficient Variational Quantum Simulator Incorporating Active Error Minimization
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“However, there are still many problems that cannot be solved using these powerful classical methods, so it is hoped that quantum computers can extend their reach [18,19,32].”
BackgroundPractical quantum advantage in quantum simulation
Daley, A. J., Bloch, I., Kokail, C., Flannigan, S., Pearson, N., Troyer, M., & Zoller, P. (2022) · Nature · doi:10.1038/s41586-022-04940-6 · Cited by 690 · see citing works
“Many of the algorithms used on a classical computer can be modified for use on a fault-tolerant digital quantum computer, and vice versa 16 .”
BackgroundMethodTopological quantum computation
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“In this context, there are three areas where remarkable algorithms have been found: searching a data base [15], abelian groups (factoring and discrete logarithm) [19], [27], and simulating physical systems [5], [ 21 ].”
The quantum technologies roadmap: a European community view
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Quantum optimization using variational algorithms on near-term quantum devices
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Hamiltonian Simulation by Qubitization
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Contextuality supplies the ‘magic’ for quantum computation
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“Quantum information enables dramatic new advantages for computation, such as Shor’s factoring algorithm [1] and quantum simulation algorithms [2].”
Universal Digital Quantum Simulation with Trapped Ions
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Quantum Chemistry Calculations on a Trapped-Ion Quantum Simulator
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“This can be done in a freely programmable way [7] that is amenable to quantum error correction [22, 23].”
BackgroundInfluentialDefining and detecting quantum speedup
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Simulating a quantum magnet with trapped ions
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“Decoherence in the simulator might even mimic the influence of the natural environmen”
BackgroundSelf-verifying variational quantum simulation of lattice models
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A Modular Functor Which is Universal¶for Quantum Computation
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Experimental Quantum Error Correction
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Topological Quantum Computation
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Computational Capacity of the Universe
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Self-citationThe cold atom Hubbard toolboxPreprint
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Hybrid Quantum-Classical Algorithms and Quantum Error Mitigation
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Toward the first quantum simulation with quantum speedup
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“Efficient quantum algorithms for simulating quantum dynamics have been known for over two decades (12).”
BackgroundThe Bravyi-Kitaev transformation for quantum computation of electronic structure
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Quantum computing with neutral atoms
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“For those models, the solution consists in using quantum circuits made of gates [53].”
MethodExperimental Ten-Photon Entanglement
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“[6] Type-II PPKTP, 20mm Pulsed, 160fs 521: 775+1590 ~ 334 ~44% (775 nm) ~7% (1590 nm) 91%”
Ising machines as hardware solvers of combinatorial optimization problems
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“Quantum simulation was in fact one of the early motivations for realizing a quantum computer, based on Feynman’s conjecture that a quantum computer should be able to simulate quantum systems more efficiently than classical computers 14 — proven true later by Lloyd 17 .”
BackgroundTheory of Trotter Error with Commutator Scaling
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Quantum Computation by Adiabatic Evolution
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“In any case, our algorithm can be recast within the conventional quantum computing paradigm using the technique introduced by Lloyd [5].”
MethodHigh-fidelity readout and control of a nuclear spin qubit in silicon
Pla, J. J., Tan, K. Y., Dehollain, J. P., Lim, W. H., Morton, J. J. L., Zwanenburg, F. A., Jamieson, D. N., Dzurak, A. S., & Morello, A. (2013) · Nature · doi:10.1038/nature12011 · Cited by 527 · see citing works
“30(1) MHz is close to, but not identical with, the bulk value of 117.”
Background(2016) · doi:10.1103/physrevlett.117.060505 · Cited by 540 · see citing works
Quantum Algorithms for Quantum Field Theories
Jordan, S. P., Lee, K. S. M., & Preskill, J. P. (2012) · Science · doi:10.1126/science.1217069 · Cited by 511 · see citing works
The physical nature of information
Landauer, R. W. (1996) · Physics Letters A · doi:10.1016/0375-9601(96)00453-7 · Cited by 514 · see citing works
A scalable quantum computer with ions in an array of microtraps
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“Finally, we would like to stress that apart from using it for quantum computations, our scheme can emulate Ising (and similar) model”
MethodDeterministic Preparation of a Tunable Few-Fermion System
Serwane, F., Zürn, G., Lompe, T., Ottenstein, T. B., Wenz, A. N., & Jochim, S. (2011) · Science · doi:10.1126/science.1201351 · Cited by 509 · see citing works
Noise tailoring for scalable quantum computation via randomized compiling
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“The rich complexity of quantum states and processes enables powerful new protocols for processing and communicating quantum information, as illustrated by Shor’s factoring algorithm [1] and quantum simulation algorithms [2].”
Nobel Lecture: Superposition, entanglement, and raising Schrödinger’s cat
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- Authors
- Lloyd, S.
- Affiliations
- Massachusetts Institute of Technology (US)
- Corresponding author
- Lloyd, Seth
- ORCID
- Lloyd, Seth
- Venue
- Science
- Published
- 1996-08-23
- Volume
- 273
- Issue
- 5278
- Pages
- 1073-1078
- ISSN
- 0036-8075 (ISSN-L)
- 1095-9203
- OpenAlex
- W2040792108
- Cited by
- 3,088
- References
- 54
- Citations by year
- 2026: 183 · 2025: 317 · 2024: 287 · 2023: 268 · 2022: 221 · 2021: 251 · 2020: 208 · 2019: 150 · 2018: 117 · 2017: 134 · 2016: 104 · 2015: 82 · 2014: 97 · 2013: 72 · 2012: 75
- FWCI
- 30.78
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- Science (publishedVersion)
- PubMed (publishedVersion)
- Topics
- Physical Sciences › Computer Science › Artificial Intelligence › Quantum Computing Algorithms and Architecture
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum many-body systems
- Physical Sciences › Computer Science › Artificial Intelligence › Quantum Information and Cryptography
- Keywords
- quantum simulation, quantum computing hardware, quantum computing
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