Solving nonlinear differential equations with differentiable quantum circuits
Open accessAbstract
We propose a quantum algorithm to solve systems of nonlinear differential equations. Using a quantum feature map encoding, we define functions as expectation values of parametrized quantum circuits. We use automatic differentiation to represent function derivatives in an analytical form as differentiable quantum circuits (DQCs), thus avoiding inaccurate finite difference procedures for calculating gradients. We describe a hybrid quantum-classical workflow where DQCs are trained to satisfy differential equations and specified boundary conditions. As a particular example setting, we show how this approach can implement a spectral method for solving differential equations in a high-dimensional feature space. From a technical perspective, we design a Chebyshev quantum feature map that offers a powerful basis set of fitting polynomials and possesses rich expressivity. We simulate the algorithm to solve an instance of Navier-Stokes equations and compute density, temperature, and velocity profiles for the fluid flow in a convergent-divergent nozzle.
AI snapshot
Written from the paper’s full text.
TL;DR
The paper introduces differentiable quantum circuits (DQCs) that encode trial functions via quantum feature maps and use automatic differentiation to represent derivatives analytically, then train hybrid quantum-classically to satisfy nonlinear differential equations and boundary conditions. It demonstrates the approach on single ODEs, coupled ODEs, and a quasi-1D Navier-Stokes convergent-divergent nozzle problem.
Key findings
- DQCs can solve nonlinear ODEs in simulation: for \(du/dx + \lambda u(\kappa + \tan(\lambda x))=0\), \(u(0)=u_0\), with \(\lambda=8,20\), \(\kappa=0.1\), \(u_0=1\), a 6-qubit register, HEA depth \(d=5\), 20 grid points, and 250 iterations, the Chebyshev tower feature map (ChebT) converged best; the product feature map failed, and the simpler Chebyshev map also failed for \(\lambda=20\).
- Increasing variational ansatz depth improved convergence for \(\lambda=20\) with ChebT: depths \(d=3,6,12,24\) were tested, and at \(d=24\) the solver had over 400 variational parameters without yet encountering barren plateaus.
- For a highly oscillatory nonperiodic ODE, Eq. (32), with \(u_0=0.75\), 100 training points, evolution time \(\tau=2\), Adam learning rate 0.01, and 200 iterations, an evolution-enhanced Chebyshev tower feature map improved on the ChebT solution after a second training stage.
- For strongly coupled equations with \(\lambda_1=5\), \(\lambda_2=3\), \(u_{1,0}=0.5\), \(u_{2,0}=0\), 6 qubits, HEA depth \(d=5\), Adam learning rate 0.02, and ChebT, floating boundary handling gave a solution close to the true one with reported \(L_Q\) approximately \(10^{-5}\).
- For the quasi-1D Navier-Stokes nozzle problem, DQCs reproduced density, temperature, and velocity profiles across the full nozzle length using a two-stage optimization: first 20 points in \((0,0.4)\) for 200 iterations at learning rate 0.01, then 40 points in \((0,0.4)\) and \((0.6,0.9)\) for 600 iterations at learning rate 0.005, with regularization switched off around iteration 150.
Methods
- Design: functions are represented as expectation values of parametrized quantum circuits, \(f(x)=\langle f_{\phi,\theta}(x)|\hat C|f_{\phi,\theta}(x)\rangle\), with quantum feature maps encoding \(x\), variational ansatze, Hermitian cost operators, and loss functions combining differential-equation residuals and boundary/regularization terms. Derivatives are obtained analytically via automatic differentiation and parameter-shift rules rather than finite differences.
- Data/sample: numerical simulations use a noiseless full quantum state simulator, implemented with YAO.JL in Julia, typically with a 6-qubit register. Test problems include a single ODE, a highly nontrivial ODE, a system of two strongly coupled ODEs, and stationary quasi-1D Navier-Stokes equations for a convergent-divergent nozzle with \(A(x)=1+4.95(2x-1)^2\), \(\gamma=1.4\), and boundary values \(\rho(0)=1\), \(T(0)=1\), \(V(0)=0.1\).
- Main analysis: training minimizes loss functions such as MSE or MAE using Adam stochastic gradient descent; feature maps compared include product, sparse Chebyshev, Chebyshev tower, and evolution-enhanced Chebyshev tower maps; boundary handling strategies include pinned, floating, and optimized boundaries.
Limitations
- Stated: the paper did not consider the impact of noise on algorithm performance; feature maps and variational ansatz choices remain open and problem-specific; evolution-enhanced feature maps increase expressivity but make training harder; boundary handling methods have tradeoffs, e.g., floating boundary requires an exact initial value while pinned/optimized boundaries can introduce competing loss terms; multifunction encoding can cause competition between optimized functions; Chebyshev derivatives diverge at the boundaries of \((-1,1)\).
- Evident from the text: all reported results are noiseless simulations on small qubit registers, not hardware demonstrations, and no quantum advantage is established; classical optimization and trainability issues such as barren plateaus are acknowledged as risks, though not encountered at the tested depths.
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Claims the paper makes
0 of 30 cited sources checked · 0 supported · 0 flagged
- Findingreasoning
Each function at the RHS diverges at the point x such that T(x) = V(x)^2.
“Immediately we observe that each function at the RHS diverges at the point x s.t.T (x) = V (x) 2 .”
Quote in the paperSubstantial claim - Findingown data
The more expressible ChebT feature map continues to perform well for λ = 20.
“The more expressible ChebT feature map continues to perform well (curves 5, 6).”
Quote in the paperSubstantial claim - Findingown data
The full loss for both λ = 8 and λ = 20 cases plateaus rapidly.
“The full loss for both cases plateaus rapidly.”
Quote in the paperNot a substantial claim - Findingreasoning
When trying to solve the steady state system using various classical methods (e.g., MATHEMATICA's NDSOLVE), the calculations do not converge.
“Interestingly, when trying to solve the system for the steady state solution using various classical methods as, for example, implemented in MATHEMATICA's NDSOLVE, the calculations do not converge.”
Quote in the paperSubstantial claim - Findingnone given
As compared to many methods relying on sparse discretization of x, we have found the solution along the full nozzle length.
“Notably, as compared to many methods relying on sparse discretization of x, we have found the solution along the full nozzle length.”
Quote in the paperNot a substantial claim
- Findingreasoning
The method can accurately represent nonlinear solutions using the high-dimensional Hilbert space of a qubit register.
“We showed how our method can accurately represent nonlinear solutions, using the high-dimensional Hilbert space of a qubit register.”
Quote in the paperSubstantial claim - Findingreasoning
By excluding the region around the nozzle throat, (0.4, 0.6), in the training we alleviate this problem.
“However, by excluding the region around the nozzle throat, (0.4, 0.6), in the training we alleviate this problem.”
Quote in the paperSubstantial claim - Findingown data
Analytical circuit differentiation can be used to represent function derivatives appearing in differential equations.
“We also showed how analytical circuit differentiation can be used to represent function derivatives appearing in differential equations, and constructed loss functions which aim to improve the prepared trial solution.”
Quote in the paperSubstantial claim - Findingown data
We find a high-quality solution based on the gradient information in the imposed solution region x < 0.4.
“We find a highquality solution based on the gradient information in the imposed solution region x < 0.4 shown in Fig. 10(a).”
Quote in the paperNot a substantial claim - Findingown data
For λ = 8, both Chebyshev feature maps converge closely to the true solution.
“We observe that for λ = 8 both Chebyshev feature maps converge closely to the true solution [Figs.6(a) and 6(d)].”
Quote in the paperSubstantial claim - Findingown data
Pinned and optimized boundary handlers perform similarly, slowly converging to the analytical solution u1,2(x) within 250 iterations.
“The pinned and optimized boundary handlers perform similarly, slowly converging to the analytical solution u 1,2 (x) within 250 iterations [Fig.8(a)].”
Quote in the paperNot a substantial claim - Findingown data
The circuit trained with the Chebyshev tower feature map manages to come close to the true solution but misses some details for getting a precise solution.
“Being expressive in itself, it manages to come close to the true solution but misses some details for getting a precise solution [Fig.7(a), red dashed curve labeled as 2].”
Quote in the paperSubstantial claim - Findingown data
At d = 24, we had not yet run into barren plateaus with over 400 variational parameters.
“however at d = 24 we had not yet ran into this with over 400 variational parameters.”
Quote in the paperNot a substantial claim - Findingown data
The two approaches have similar convergence in terms of the full loss.
“The two approaches have similar convergence in terms of the full loss [Fig.8(b)].”
Quote in the paperNot a substantial claim - Findingown data
The Chebyshev tower feature map was the most expressible of the three considered for the single ODE example.
“As shown in Fig. 6, the Chebyshev tower feature map was the most expressible of the three considered for that example.”
Quote in the paperNot a substantial claim - Findingown data
The derivative contribution L_D weakly improves during training.
“while the full loss L F improves [Fig.10(c), curve 7] thanks to regularization contribution and weakly improved derivative contribution L D [Fig.10(c), curve 9]”
Quote in the paperNot a substantial claim - Findingown data
The DQC solution matches the known solution for the Navier-Stokes convergent-divergent nozzle problem.
“The DQC solution matches the known solution and also what would be physically expected.”
Quote in the paperSubstantial claim - Findingown data
The full loss L_F improves during training.
“while the full loss L F improves [Fig.10(c), curve 7] thanks to regularization contribution and weakly improved derivative contribution L D [Fig.10(c), curve 9]”
Quote in the paperNot a substantial claim - Premisecitation
Translating quantum oracles that encode differential equations can introduce huge computational overheads, making simulation infeasible even for a fault-tolerant quantum computer.
“Finally, translating quantum oracles that encode DEs (matrix Â) can introduce huge computational overheads, making simulation infeasible even for a faulttolerant quantum computer [36].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [36] source
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- Interpretationreasoning
The DQC approach brings advantage in finding solutions of differential equations by using the large expressive power of quantum feature maps and parametrized quantum circuits.
“This brings advantage in finding solutions of differential equations, as we use the large expressive power of quantum feature maps and parametrized quantum circuits.”
Quote in the paperSubstantial claim - Premisecitation
Chebyshev polynomials form an optimal set of basis functions in the sense of the uniform L∞ norm.
“As shown in the Remez algorithm [161,162], Chebyshev polynomials form an optimal set of basis functions in the sense of the uniform L ∞ norm.”
Quote in the paperSubstantial claim0 of 2 sources checked- cites [161]
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- cites [162]
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- Interpretationnone given
The DQC approach targets near-term quantum devices, where hybrid quantum-classical computing can work with noisy operation and reasonably shallow circuit depth.
“Our approach targets near-term quantum devices, where hybrid quantum-classical computing can work with noisy operation and reasonably shallow circuit depth.”
Quote in the paperSubstantial claim - Premisecitation
Preparation of a generic input state requires sophisticated techniques such as quantum random access memory, leading to a data input problem.
“Second, the preparation of a generic input state |b requires sophisticated techniques such as quantum random access memory (QRAM) [35], thus leading to a so-called data”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [35] source
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- Premisecitation
The redundancy from many qubits forms a basis set for function fitting.
“The redundancy from many qubits thus forms a basis set for function fitting [157].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [157]
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- Interpretationreasoning
The DQC approach can implement a spectral method for solving differential equations in a high-dimensional feature space.
“As a particular example setting, we show how this approach can implement a spectral method for solving differential equations in a high-dimensional feature space.”
Quote in the paperNot a substantial claim - Interpretationcitation
The Chebyshev feature map decomposition corresponds to a unitary operation with matrix elements defined by degree-n Chebyshev polynomials of the first and second kind.
“The resulting decomposition (12) corresponds to a unitary operation with matrix elements defined by degree-n Chebyshev polynomials of first and second kind, denoted as T n (x) and U n (x), respectively [160].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [160]
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- Interpretationreasoning
The proposed quantum algorithm can solve systems of nonlinear differential equations.
“We propose a quantum algorithm to solve systems of nonlinear differential equations.”
Quote in the paperSubstantial claim - Premisecitation
HHL-based algorithms rely on amplitude encoding, which provides exponential memory advantage by compressing large grids into a small qubit register.
“The power of HHL-based algorithms relies on amplitude encoding, where a function is represented as a quantum state |u = 2 N k=1 u k |k encoded in complex u k amplitudes of computational basis states |k for N qubits.This allows for compressing large grids into a small qubit register, providing exponential memory advantage.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [9] source
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- Interpretationreasoning
The DQC approach alleviates the data input problem by not relying on amplitude encoding but using a latent space representation defined in the high-dimensional Hilbert space.
“We alleviate the data input problem, as we do not rely on amplitude encoding, but use a latent space representation defined in the high-dimensional Hilbert space.”
Quote in the paperSubstantial claim - Interpretationnone given
Automatic differentiation represents function derivatives in an analytical form as differentiable quantum circuits, avoiding inaccurate finite difference procedures for calculating gradients.
“We use automatic differentiation to represent function derivatives in an analytical form as differentiable quantum circuits (DQCs), thus avoiding inaccurate finite difference procedures for calculating gradients.”
Quote in the paperSubstantial claim - Interpretationreasoning
The Chebyshev tower feature map allows the representation of generic functions.
“Eq. ( 15) allows the representation of generic functions, and can be improved further by using layers of rotations as in Eq. ( 7).”
Quote in the paperSubstantial claim - Premisecitation
The product feature map encodes the variable as an N-th degree polynomial formed by {1, x, sqrt(1-x^2)} and their products.
“Acting on the initial state |Ø this feature map encodes the variable as an N-th degree polynomial formed by {1, x, √ 1x 2 } and their products [73].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [73] source
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- Interpretationreasoning
The DQC approach alleviates the problem of approximation errors and fine discretization grids in typical quantum ODE solvers.
“This problem is alleviated in our approach.”
Quote in the paperSubstantial claim - Interpretationreasoning
The Chebyshev feature map drastically changes the basis set for function representation.
“Belonging to the product feature map family, it drastically changes the basis set for function representation.”
Quote in the paperSubstantial claim - Premisecitation
Reading out function values from the quantum state in HHL-based algorithms generally requires exponential sampling, representing a data output problem.
“Reading out the function values from the quantum state |u in general requires exponential sampling, representing a so-called data”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [9] source
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- Interpretationreasoning
The DQC approach avoids the data readout problem because the solution is encoded in the observable of an operator, such that expectation can be routinely calculated.
“and (4) avoid the data readout problem, as the solution is encoded in the observable of an operator, such that expectation can be routinely calculated.”
Quote in the paperSubstantial claim - Premisereasoning
Product feature map states are limited to the subspace of product states.
“These states are limited to the subspace of product states.”
Quote in the paperSubstantial claim - Interpretationnone given
Pinned boundary handling's weakness is the necessity of adjusting the boundary value starting from the one represented by initial θinit, typically generated randomly.
“At the same time, the weakness corresponds to the necessity of adjusting the boundary value starting from the one represented by initial θ init , typically generated randomly.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Optimized boundary handling: due to the classical shift, even if random initial angles start far from the initial value, the optimizer can quickly and easily update fc to rectify this.
“One strength of the described method is that, due to the classical shift, even if the random initial angles start such that f ϕ,θ init (x 0 )| Ĉ| f ϕ,θ init (x 0 ) is far from the initial value u 0 , the optimizer can quickly and easily update f c to rectify this.”
Quote in the paperSubstantial claim - Interpretationreasoning
The choice of ansatz is sensitive to the choice of the cost function operator, as dictated by symmetry.
“First, we note that the choice of ansatz is sensitive to the choice of the cost function operator (see the next subsection), as dictated by the symmetry.”
Quote in the paperSubstantial claim - Interpretationnone given
Pinned boundary handling's strength is equivalent treatment of boundary and derivative terms, both encoded in Ĉ.
“The strength of the pinned boundary handling is in equivalent treatment of boundary and derivative terms, both being encoded in Ĉ.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Once close to the optimal solution, MAE and KL can achieve higher accuracy than MSE.
“However, once close to the optimal solution they can achieve higher accuracy than MSE.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The evolution-enhanced feature map joins the Chebyshev and Fourier basis sets, encoded in the full Hilbert space for complex Ĥ.
“The evolution-enhanced feature map then joins the Chebyshev and Fourier basis sets, encoded in the full Hilbert space for complex Ĥ .”
Quote in the paperNot a substantial claim - Premisecitation
Regularization procedure helps the optimizer avoid getting trapped in local minima.
“We can achieve this by introducing a regularization procedure [167,168], also helping the optimizer to avoid getting trapped in local minima.”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [167]
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- cites [168]
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- Premisecitation
Trainability can change depending on the variational ansatz type and cost function choice.
“This can change depending on the variational ansatz type and cost function choice [70].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [70] source
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- Interpretationnone given
By choosing Ĥ as a complex many-body Hamiltonian, exponentially many amplitudes are generated.
“By choosing Ĥ as a complex many-body Hamiltonian we ensure that exponentially many amplitudes are generated.”
Quote in the paperSubstantial claim- Rests on an assumption: Quantum simulation of dynamics leads to a volume-like increase of entanglement.
- Interpretationreasoning
The Chebyshev quantum feature map allows the approximation of highly nonlinear functions.
“Below we describe some possible choices and propose a distinct Chebyshev quantum feature map that allows the approximation of highly nonlinear functions.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The DQC approach uses quantum feature map encoding, thus overcoming the complexity of amplitude encoding for preparing the solution at the boundary.
“we (1) use quantum feature map encoding, thus overcoming the complexity of amplitude encoding for preparing the solution at the boundary;”
Quote in the paperSubstantial claim - Interpretationnone given
Floating boundary handling requires knowledge of an exact initial value, which can be an issue in specific situations.
“However this method does require knowledge of an exact initial value which can be an issue in specific situations.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The Chebyshev tower feature map enriches the basis set by creating a tower-like structure of polynomials with increasing n = j.
“where the encoded degree grows with the number of qubits, creating a tower-like structure of polynomials with increasing n = j.Again, as polynomials chain together and morph between two kinds and their degrees, the basis set is largely enriched.”
Quote in the paperSubstantial claim - Interpretationnone given
DQC constructs the solution valid also beyond (and between) the points at which loss is evaluated originally.
“Notably, this can be done for any point x, as DQC constructs the solution valid also beyond (and between) the points at which loss is evaluated originally.”
Quote in the paperSubstantial claim - Interpretationown data
The system is stiff.
“This proves to be challenging as the system is stiff.”
Quote in the paperSubstantial claim - Interpretationreasoning
Adding quantum evolution helps to represent highly oscillatoric functions.
“This helps to represent highly oscillatoric functions.”
Quote in the paperSubstantial claim - Interpretationreasoning
A feature map with high expressibility is vital for solving Eq. (32).
“Therefore a feature map with high expressibility is vital for this problem.”
Quote in the paperSubstantial claim - Interpretationown data
Choosing a feature map expressible enough for the problem is important.
“This supports the hypothesis that choosing a feature map expressible enough for the problem is important”
Quote in the paperSubstantial claim - Interpretationreasoning
The larger |λ1| compared to |λ2|, the more strongly coupled the two equations will be.
“The larger |λ 1 | is in comparison to |λ 2 | the more strongly coupled the two equations will be.”
Quote in the paperNot a substantial claim - Interpretationnone given
The differential equation (32) has a solution that is hard to represent since it involves both oscillatoric terms with high frequency and nonoscillatoric terms representing growth and decay.
“This differential equation has a solution that is hard to represent since it involves both oscillatoric terms with high frequency and nonoscillatoric terms representing growth and decay.”
Quote in the paperSubstantial claim - Interpretationown data
Solutions may become unstable depending on initial values, specifically the input velocity.
“Solutions may become unstable depending on initial values, and specifically the input velocity.”
Quote in the paperSubstantial claim - Interpretationnone given
Adding a quantum evolution increases expressibility of the circuit.
“We note that by adding a quantum evolution we increase expressibility of the circuit.”
Quote in the paperSubstantial claim - Interpretationreasoning
This method opens up a new way of solving general, complex, (non)linear systems.
“This method opens up a new way of solving general, complex, (non)linear systems; as an example we presented solutions to the Navier-Stokes equations, but the same method can be applied across all disciplines where differential equations arise.”
Quote in the paperNot a substantial claim - Interpretationown data
The DQC solution matches what would be physically expected for the Navier-Stokes convergent-divergent nozzle problem.
“The DQC solution matches the known solution and also what would be physically expected.”
Quote in the paperSubstantial claim- Rests on an assumption: As air flows through the convergent-divergent nozzle, it accelerates and cools down.
- Interpretationreasoning
VQA are highly suitable to problems where traditional methods fail or are inefficient.
“While VQA inherently remains a heuristic, similarly to machine learning-type approaches, they are highly suitable to problems where traditional methods fail or are inefficient.”
Quote in the paperNot a substantial claim - Interpretationreasoning
For differential equations, rich basis sets allow for accurate solution representation in a memory-frugal form.
“For differential equations, rich basis sets allow for accurate solution representation in a memory-frugal form-a saved list of optimal circuit parameters for a given DQC structure.”
Quote in the paperSubstantial claim - Premisecitation
Barren plateaus can be mitigated by a carefully chosen circuit structure, as recently shown for convolutional quantum circuits.
“That can be mitigated by a carefully chosen circuit structure, as recently shown for convolutional quantum circuits [115,175].”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [115] source
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- cites [175]
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- Interpretationown data
The improvement in the full loss L_F is due to the regularization contribution.
“while the full loss L F improves [Fig.10(c), curve 7] thanks to regularization contribution and weakly improved derivative contribution L D [Fig.10(c), curve 9]”
Quote in the paperNot a substantial claim
- May combine two claims. 38
- Classified as probably not a substantial claim. 43
- The quote only partly states this claim. 2
May combine two claims.
Findingnone givenThe authors simulate the algorithm to solve an instance of Navier-Stokes equations and compute density, temperature, and velocity profiles for the fluid flow in a convergent-divergent nozzle.
“We simulate the algorithm to solve an instance of Navier-Stokes equations and compute density, temperature, and velocity profiles for the fluid flow in a convergent-divergent nozzle.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataMSE loss choice is intuitive and performs sufficiently well in numerical simulations.
“While being simple, we find the choice (22) intuitive and performing sufficiently well in numerical simulations.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown dataFor lower depths the solver is slower to converge and does not reach as high accuracy as it does for higher depths.
“We observe that for lower depths the solver is slower to converge and does not reach as high accuracy as it does for higher depths.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown dataAfter second stage training with the evolution-enhanced feature map, we are able to capture the intricate details of the solution, and both the full loss and quality of solution are improved.
“As can be seen, after this second stage of training, we are able to capture the intricate details of the solution [Fig.7(a), blue dashed curve labeled by 3], and both the full loss and quality of solution are improved upon [Fig.7(b)].”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown dataThe consequence of competing terms in the loss function can be seen in the early oscillations of the full loss in Fig. 8(b).
“The consequence of competing terms in the loss function can be seen in the early oscillations of the full loss in Fig. 8(b).”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown dataThe increase of speed for the air flow in the convergent part and decrease of temperature and density is reproduced quantitatively.
“The increase of speed for the air flow in the convergent part and decrease of temperature and density is reproduced quantitatively.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataThe less powerful product feature map fails to converge with the loss quickly plateauing.
“The less powerful product feature map fails to converge with the loss quickly plateauing (curves 1, 2).”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataThe more expressible Chebyshev tower feature map takes longer to converge but reaches a solution closer to the true solution.
“The more expressible Chebyshev tower feature map (curves 5, 6) takes longer to converge but reaches a solution closer to the true solution.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataFull dynamical solution and its t→∞ extrapolation are possible once well-suited initial conditions (45)-(47) are chosen allowing to avoid instability.
“At the same time, full dynamical solution and its t → ∞ extrapolation are possible, shown in Figs.9(b) and 9(c) once the well-suited initial conditions (45)-( 47) are chosen allowing to avoid instability, as usually done in computational fluid dynamics [2,142].”
Quote in the paperSubstantial claim0 of 2 sources checked- cites [2]
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- cites [142]
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Findingown dataFor λ = 20, the product feature map still fails to converge, and the simpler Chebyshev feature map also fails to converge.
“The product feature map still fails to converge (curves 1, 2), but now also failing to converge is the simpler Chebyshev feature map (curves 3, 4).”
Quote in the paperSubstantial claimMay combine two claims. The quote only partly states this claim.
Findingown dataDQCs are efficiently trained to approach the true solution, evidenced by LQ decrease.
“For the region with switched off regularization we observe steady improvement of all metrics, showing that DQCs are efficiently trained to approach true solution, also evidenced by L Q decrease.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataThe full solution converges to the expected long-time behavior for the system, where function derivatives from DQC match the nonlinear contributions.
“It converges to the expected long-time behavior for the system, where function derivatives from DQC match the nonlinear contributions.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataIn the subsonic region, flow velocity grows towards the middle of the nozzle, while temperature and density drop slowly.
“As expected, in the subsonic region flow velocity grows towards the middle of the nozzle, while temperature and density drop slowly [see Fig. 10(a), dashed curves 4, 5, 6].”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based). May combine two claims.
Interpretationnone givenThe Chebyshev quantum feature map offers a powerful basis set of fitting polynomials and possesses rich expressivity.
“we design a Chebyshev quantum feature map that offers a powerful basis set of fitting polynomials and possesses rich expressivity.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationTypical schemes for quantum ODE solvers involve numerical differentiation using Euler's method and finite difference schemes that suffer from approximation errors and often require a fine discretization grid.
“Notably, typical schemes for quantum ODE solvers involve numerical differentiation using Euler's method and finite difference schemes that suffer from approximation errors, and often require a fine discretization grid.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [25][26][27][28][29][30][31][32][33]
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InterpretationreasoningBecause the Fourier map involves unitary operators with phases that are linear functions of x, it is a fully harmonic mapping.
“As it involves unitary operators with phases being linear functions of x, this is a fully harmonic mapping.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Interpretationnone givenShared quantum register encoding is resource-frugal and suitable for certain systems.
“This method is resource-frugal, and is suitable for certain systems.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningFloating boundary handling guarantees exact matching to initial values given and does not require a separate boundary term in the loss function.
“This method of boundary handling guarantees exact matching to initial values given and does not require a separate boundary term in the loss function, thus the derivative loss term does not have to compete with the boundary loss.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S4 (based).
Premisenone givenProduct feature maps induce nonlinear mappings between variable(s) x and quantum states described by tensor products of separate single-qubit wave functions.
“Product feature maps induce nonlinear mappings between variable(s) x and quantum states described by tensor products of separate single-qubit wave functions.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Interpretationnone givenMSE places greater emphasis on larger distances and smaller weight on small distances, strongly discouraging terms with large L.
“MSE places a greater emphasis on larger distances and smaller weight on small distances, strongly discouraging terms with large L.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Interpretationnone givenShared register encoding may exhibit competition between the optimization of different functions.
“However, the choice of suitable cost operators becomes complicated, as in some cases shared register encoding may exhibit competition between the optimization of different functions.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationcitationThe alternating blocks ansatz's motivation is to entangle qubits locally first and gradually form a correlated state by interleaving subblocks, which helps improve trainability while maintaining high expressibility.
“The motivation behind ABA is that we want to entangle qubits locally first, and gradually form a correlated state by interleaving subblocks.This helps to improve trainability of the circuit together while maintaining high expressibility [70,164].”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [70] source
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- cites [164]
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Probably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningEnhancing product feature maps (specifically the layered Chebyshev map) with additional entangling layers represented by Hamiltonian evolution makes feature maps more expressive.
“To make the described feature maps even more expressive, we suggest enhancing product feature maps (and specifically the layered Chebyshev map) with additional entangling layers represented by Hamiltonian evolution.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Interpretationnone givenPaired with expressive variational ansatze, digital feature maps may offer function encoding with memory savings of amplitude encoding while avoiding the input problem.
“Paired with expressive variational ansatze they may offer function encoding with memory savings of the amplitude encoding, while avoiding the input problem.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Interpretationnone givenOptimized boundary handling's weakness is that boundary and differential terms in the loss may compete against one another.
“A weakness however is that the boundary and differential terms in the loss may compete against one another.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningFloating boundary handling simplifies the choice for optimal angles and removes the dependence on initial θinit.
“Furthermore, as we allow the cost function to match to the solution shifted by any amount, this simplifies the choice for optimal angles and removes the dependence on initial θ init .”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningThe DQC approach differs from amplitude encoding in HHL and related methods, where getting the full solution from amplitudes is exponentially costly and requires tomographic measurements.
“For the latter point, it differs from amplitude encoding |u in HHL and related methods, where getting the full solution from amplitudes is exponentially costly and requires tomographic measurements.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationFourier feature maps are based on the evolution operator exp(-i Ĥdata x), applied for some set of qubits.
“This class of quantum feature maps is based on the evolution operator exp(-i Ĥdata x), which is applied for some set of qubits.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [155]
Not checked in the free run.
Probably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing), S4 (based).
Interpretationnone givenDigital quantum feature maps offer a potentially powerful technique when dealing with functions of discrete variables.
“Digital quantum feature maps offer a potentially powerful technique when dealing with functions of discrete variables.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Interpretationnone givenThe simplest cost operator choice, magnetization of a single qubit Ẑj, allows representing functions in the range [-1, 1] and requires rescaling for other intervals.
“Note that this choice allows representing functions in range [-1, 1], and requires rescaling for other intervals.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningOptimized boundary handling removes the need to include boundary information in the cost expectation, but information still needs to be included in the loss function.
“This removes the need to include boundary information in the cost expectation, but information still needs to be included in the loss function.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningUsing two layers of rotations plus evolution makes the embedding difficult to simulate classically, but can be implemented as a unitary evolution on a quantum computer.
“Then using two layers of rotations plus evolution the embedding becomes difficult to simulate classically, but can be implemented as a unitary evolution on a quantum computer.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningIncreased number of controlled parameters can complicate the search for an optimal θ, known as a problem in trainability.
“However, this comes with an increased number of controlled parameters which can complicate the search for an optimal θ opt for the solution, known as a problem in trainability.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationcitationThe DQC approach can work with quantum kernels, an advantageous choice for the loss function that allows for efficient multipoint training.
“We note that our approach also can work with quantum kernels [153], an advantageous choice for the loss function that allows for efficient multipoint training.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [153]
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
InterpretationcitationChoosing an ansatz parametrized by single-qubit rotations allows the application of the parameter shift rule, while overlap measurement opens up options for more general strategies.
“Choosing an ansatz parametrized by single-qubit rotations allows the application of the parameter shift rule, while overlap measurement opens up options for more general strategies [158].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [158]
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe Fourier map lets functions be encoded as Fourier series defined by the differences of the eigenvalues of Ĥdata.
“The Fourier map lets functions be encoded as Fourier series defined by the differences of the eigenvalues of Ĥdata .”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [155]
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
InterpretationreasoningMAE and KL do not place such an emphasis and may have slower convergence.
“Both MAE and KL do not place such an emphasis and may have slower convergence.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premisenone givenAs the number of layers d grows, the circuit's expressive power increases.
“As the number of layers d grows, the circuit's expressive power increases.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
InterpretationreasoningHigher emphasis on regularization at initial stages, diminishing to zero at higher iteration numbers, leads to prior information being used first, setting a rough solution, followed by precise derivative loss optimization at later training stages.
“In general, we require higher emphasis on the regularization-based training at initial stages, which shall diminish to zero at higher iteration numbers.This leads to the prior information being used at first, setting a rough solution or preferred function behavior, followed by precise derivative loss optimization at later training stages.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningAs a consequence of cost function choice, one needs to choose noncommuting generators Ĝj for the variational ansatz such that [Ĉ, Ĝj] = 0, which ensures the solution space can be spanned.
“Namely, as a consequence of cost function choice we need to choose noncommuting generators Ĝ j for the variational ansatz such that [ Ĉ, Ĝ j ] = 0.This ensures that the solution space can be spanned.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationIn many cases generators can be chosen such that only real amplitudes are generated.
“In many cases generators can be chosen such that only real amplitudes are generated, see for instance [70].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [70] source
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing).
Interpretationreasoningλ=20 is a complex case as the resulting solution is highly nonlinear and oscillatoric.
“These problem parameters are chosen to make DQC construction challenging, with λ = 20 being a complex case as the resulting solution is highly nonlinear and oscillatoric.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Interpretationnone givenAs λ and κ grow, the function starts to oscillate and decay more rapidly, and the solution becomes harder to express.
“As λ and κ grow the function starts to oscillate and decay even more rapidly, and the solution becomes harder to express.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
InterpretationreasoningThis causes a major problem to classical solvers, that are unable to find a steady state solution directly.
“This causes a major problem to classical solvers, that are unable to find a steady state solution directly.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
InterpretationreasoningSeparate quantum registers require more resources, but function and derivative evaluation can be done in parallel.
“While requiring more resources we note that function and derivative evaluation can be done in parallel.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe alternating blocks ansatz is designed in a way that vanishing gradients can be avoided for certain conditions.
“We also note that the alternating blocks ansatz is designed in the way that vanishing gradients can be avoided for certain conditions [164].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [164]
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Interpretationnone givenSpin-glass type cost functions allow for high expressibility of the circuit describing the DE's solution.
“These are known to include NP-hard problem instances, and they allow for high expressibility of the circuit describing the DE's solution.”
Quote in the paperNot a substantial claim- Rests on an assumption: Spin-glass type cost functions include NP-hard problem instances.
Probably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing).
Interpretationnone givenQuality of solution gives a useful way to compare how two different training setups perform, especially if they are training to solve the same differential equations.
“Quality of solution gives us a useful way to compare how two different training setups perform, especially if they are training to solve the same differential equations.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningAs depth increases, the number of gate operations needed per iteration and the number of parameters the classical optimizer needs to update increase, raising the time taken per iteration.
“This causes an increase in the number of gate operations needed in each iteration and how many parameters the classical optimizer needs to update, raising the time taken per iteration.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningThe difference in convergence rate is a result of boundary information having an impact on the loss, demanding the matching for pinned and optimized boundary handlers, whereas the floating boundary automatically matches the initial condition and no loss boundary term is needed.
“This difference in convergence rate is a result of boundary information having an impact on the loss, demanding the matching for pinned and optimized boundary handlers, whereas the floating boundary automatically matches the initial condition and no loss boundary term is needed.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductnone givenChoosing maximal time 0.9 avoids the region with diverging derivative of the nonlinear feature function dφ(x)/dx.
“This is chosen such that the region with diverging derivative of the nonlinear feature function dϕ(x)/dx is avoided, and we note that x can be rescaled to match required boundaries.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Premisenone givenThe key problem of the convergent-divergent nozzle in the subsonic-supersonic transition case is the divergence around the middle of the nozzle.
“As we discussed before, the key problem of the convergentdivergent nozzle in the subsonic-supersonic transition case is the divergence around the middle of the nozzle.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
InterpretationreasoningMore simulations with more qubits offers a way to increase the power drastically.
“and more simulations with more qubits offers a way to increase the power drastically.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningDQCs with the evolution-enhanced feature map are more difficult to train, as keeping track of the gradients for oscillatoric function requires a finer training grid and has a slower convergence.
“At the same time, DQCs in this case are more difficult to train, as keeping track of the gradients for oscillatoric function requires a finer training grid and has a slower convergence.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductnone givenResults remain consistent for different J and h generated randomly.
“We check that results remain consistent for different J and h generated randomly.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningDivergent contributions from this region also impact the loss function, and makes training complicated.
“Divergent contributions from this region also impact the loss function, and makes training complicated.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningThis leads to singular behavior and breaks classical solvers, including the ones with stiff handling.
“This leads to singular behavior and breaks classical solvers, including the ones with stiff handling.”
Quote in the paperSubstantial claimMay combine two claims.
Interpretationnone givenThe expressive power of the evolution-enhanced map can be increased for more complex H and larger τ, though at the expense of trainability.
“The expressive power of the evolution-enhanced map can be increased for more complex Ĥ and larger τ , though at the expense of trainability.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationAs the depth of the ansatz continues to increase, eventually the problem of barren plateaus could be encountered.
“As the depth of the ansatz continues to increase eventually the problem of barren plateaus could be encountered [171].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [171]
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
InterpretationreasoningAlthough the method works explicitly for a spectral (global) treatment, the scheme is general and one may instead consider a digital quantum feature map which allows a grid-based (local) treatment.
“Although we showed how the method works explicitly for a spectral (global) treatment, the scheme is general and one may instead consider a digital quantum feature map which allows a grid-based (local) treatment.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningSeparate quantum registers remove the issue of choosing cost operators and avoid direct competition due to independent parametrization.
“This removes the issue of choosing the cost operators, and avoids the related direct competition due to independent parametrization.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
InterpretationreasoningThe same method can be applied across all disciplines where differential equations arise.
“but the same method can be applied across all disciplines where differential equations arise.”
Quote in the paperNot a substantial claimMay combine two claims.
Interpretationown dataFor λ = 20, the true solution is more oscillatoric and has stronger damping, making the solution harder to represent.
“For λ = 20 the true solution is more oscillatoric and has stronger damping, making the solution harder to represent [Figs.6(b) and 6(e)].”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationIn classification tasks, increased representation power leads to increased accuracy even for small networks.
“In classification tasks this leads to increased accuracy even for small networks [174].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [174]
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductnone givenWe did not yet consider the impact of noise on the algorithm performance.
“We did not yet consider the impact of noise on the algorithm performance;”
Quote in the paperNot a substantial claim- Rests on an assumption: Analytical gradients are much less susceptible to noise than numerical gradients evaluated on variational quantum circuits.
Probably not a substantial claim: may not pass S3 (load-bearing).
Interpretationnone givenA good choice of variational ansatz is crucial to loss function convergence success and speed.
“A good choice of variational ansatz is crucial to loss function convergence success and speed.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationClassical neural networks based on Fourier representation were recently shown to outperform traditional PDE solvers by three orders of magnitude.
“For instance, classical neural networks based on Fourier representation were recently shown to outperform traditional PDE solvers by three orders of magnitude [147].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [147]
Not checked in the free run.
Probably not a substantial claim: may not pass S4 (based). The quote only partly states this claim.
InterpretationreasoningAbsolute operation rates require quantum hardware specifications with high sampling rates and a low-latency hybrid operational mode.
“The latter requires quantum hardware specifications with high sampling rates and a low-latency hybrid operational mode.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningThe success of operation depends on trainability of quantum circuits and absolute operation rates.
“Having the expressibility advantage, the success of operation then depends on (1) trainability of quantum circuits and (2) absolute operation rates.”
Quote in the paperSubstantial claim- Rests on an assumption: Trainability of quantum circuits is well-known to suffer from barren plateaus.
Probably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThis was used recently to speed up generative modeling with quantum batch training.
“This was used recently to speed up generative modeling with quantum batch training [124].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [124] source
Not checked in the free run.
Probably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing), S4 (based).
Interpretationnone givenDifferential quantum circuits can enjoy another type of computational advantage related to training.
“Finally, differential quantum circuits can enjoy another type of computational advantage related to training.”
Quote in the paperNot a substantial claim- Rests on an assumption: For expressive feature maps, the representation power of quantum circuits grows superpolynomially with the number of qubits.
Classified as probably not a substantial claim.
PremisecitationVariational quantum machine learning uses quantum circuits as universal function approximators.
“Similarly to classical ML, variational quantum machine learning uses quantum circuits as universal function approximators [173].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [173]
Not checked in the free run.
The paper relies on this without support.
Quantum simulation of dynamics leads to a volume-like increase of entanglement.
“It is known that the quantum simulation of dynamics leads to a volume-like increase of entanglement.”
The paper relies on this without support.
Spin-glass type cost functions include NP-hard problem instances.
“These are known to include NP-hard problem instances, and they allow for high expressibility of the circuit describing the DE's solution.”
The paper relies on this without support.
The type of Hamiltonian used in the evolution-enhanced feature map is not crucial and may depend on hardware implementation.
“Note that the type of Hamiltonian is not crucial, and may depend on hardware implementation.”
The paper relies on this without support.
Analytical gradients are much less susceptible to noise than numerical gradients evaluated on variational quantum circuits.
“it is well-known that the analytical gradients, which are used here, are much less susceptible to noise than numerical gradients evaluated on variational quantum circuits.”
The paper relies on this without support.
For expressive feature maps, the representation power of quantum circuits grows superpolynomially with the number of qubits.
“For expressive feature maps, the representation power of quantum circuits grows superpolynomially with the number of qubits.”
The paper relies on this without support.
Trainability of quantum circuits is well-known to suffer from barren plateaus.
“The former is well-known to suffer from a phenomenon commonly referred to as barren plateaus.”
The paper relies on this without support.
As air flows through the convergent-divergent nozzle, it accelerates and cools down.
“As the air goes through the nozzle it accelerates and cools down.”
Claims other papers make about this one
Each is checked against this paper’s own text: does it say what the citing paper says it does?
Refs [139-141] considered the Hamiltonian H_G = A(I - |b><b|)A†.
“Refs. [139-141] considered the Hamiltonian H G = A ( ✶ -| b 〉 〈 b | ) A † (which was also considered outside of the variational setting [142]).”
From Variational quantum algorithms (2021) · cites this paper as [142]
The Introduction discusses solving for |u⟩ = A⁻¹|b⟩, but does not give the claimed Hamiltonian. The Cost function section describes magnetization and Ising-type operators instead. Searches for the projector |b⟩⟨b| and H_G found no passage showing that this paper considered H_G = A(I − |b⟩⟨b|)A†. (LLM, conf=0.74)
Experimental — accuracy not yet measured
Self-check
Percentages, sums and reported differences re-computed from the paper’s own numbers.
Each contradiction between two passages listed here was confirmed by an independent check.
Odd-degree Chebyshev conversion disagrees with the stated U1 polynomial
MinorApplying the stated odd-degree conversion at n = 1 gives U1(x) = 2[T1(x) − 1] = 2x − 2. The paper separately states U1(x) = 2x.
“U n (x) = 2 n j odd [T j (x) -1] when n is odd.”
“U 0 (x) = 1, U 1 (x) = 2x, U n+1 (x) = 2xU n (x) -U n-1 (x).”
Chebyshev polynomial derivatives are said to diverge at the boundaries
MinorThe paper says these derivatives diverge at the interval boundaries, but its explicit polynomial T2(x) = 2x2 − 1 has derivative 4x, which is finite at both boundaries.
“their derivatives diverge at the boundaries of this interval.”
“T 2 (x) = 2x 2 -1”
Two derivative formulas give different parameter-shift coefficients
MinorFor a single x-dependent rotation with φ(x) = x, Eq. (2) assigns one-half of the difference between the shifted expectations to the derivative. Eqs. (9)-(10) assign one-quarter of that same difference.
“d dx Ø| Ûϕ (x) † Ĉ Ûϕ (x)|Ø = 1 4 d dx ϕ(x) ( Ĉ + -Ĉ -), (9”
“df (x)/dx = 1 2 j f + dϕ, j,θ (x)| Ĉ| f + dϕ, j,θ (x) -f - dϕ, j,θ (x)| Ĉ| f - dϕ, j,θ (x) ,(2)”
Cites
Adam: A Method for Stochastic Optimization
Kingma, D. P., & Ba, J. (2014) · arXiv · doi:10.48550/arxiv.1412.6980 · Cited by 98,946 · see citing works
Raissi, M., Perdikaris, P., & Karniadakis, G. E. (2019) · Journal of Computational Physics · doi:10.1016/j.jcp.2018.10.045 · Cited by 20,384 · see citing works
Handbook of Mathematical Functions with Formulas
Owen, D. B., Abramowitz, M., & Stegun, I. A. (1965) · Technometrics · doi:10.1080/00401706.1965.10490234 · Cited by 19,065 · see citing works
Quantum Computing in the NISQ era and beyond
Preskill, J. (2018) · Quantum · doi:10.22331/q-2018-08-06-79 · Cited by 8,830 · see citing works
Quantum Computation and Quantum Information: 10th Anniversary Edition
Nielsen, M. A., & Chuang, I. L. (2012) · doi:10.1017/cbo9780511976667 · Cited by 8,436 · see citing works
Quantum supremacy using a programmable superconducting processor
Arute, F., Arya, K., Babbush, R., Bacon, D., Bardin, J. C., Barends, R., Biswas, R., Boixo, S., Brandao, F. G. S. L., Buell, D. A., et al. (2019) · Nature · doi:10.1038/s41586-019-1666-5 · Cited by 7,720 · see citing works
Biamonte, J., Wittek, P., Pancotti, N., Rebentrost, P., Wiebe, N., & Lloyd, S. (2017) · Nature · doi:10.1038/nature23474 · Cited by 4,779 · see citing works
A variational eigenvalue solver on a photonic quantum processor
Peruzzo, A., McClean, J., Shadbolt, P., Yung, M.-H., Zhou, X.-Q., Love, P. J., Aspuru-Guzik, A., & O’Brien, J. L. (2014) · Nature Communications · doi:10.1038/ncomms5213 · Cited by 4,552 · see citing works
Solving Ordinary Differential Equations II
Hairer, E., & Wanner, G. (1996) · Springer Series in Computational Mathematics · doi:10.1007/978-3-642-05221-7 · Cited by 4,342 · see citing works
Chebyshev and Fourier Spectral Methods
Boyd, J. P. (2001) · Cited by 4,168 · see citing works
Quantum Algorithm for Linear Systems of Equations
Harrow, A. W., Hassidim, A., & Lloyd, S. (2009) · Physical Review Letters · doi:10.1103/physrevlett.103.150502 · Cited by 3,325 · see citing works
Numerical Methods for Ordinary Differential Equations
Butcher, J. C. (2016) · Wiley eBooks · doi:10.1002/9781119121534 · Cited by 3,020 · see citing works
Hardware-efficient variational quantum eigensolver for small molecules and quantum magnets
Kandala, A., Mezzacapo, A., Temme, K., Takita, M., Brink, M., Chow, J. M., & Gambetta, J. M. (2017) · Nature · doi:10.1038/nature23879 · Cited by 2,982 · see citing works
Supervised learning with quantum-enhanced feature spaces
Havlíček, V., Córcoles, A. D., Temme, K., Harrow, A. W., Kandala, A., Chow, J. M., & Gambetta, J. M. (2019) · Nature · doi:10.1038/s41586-019-0980-2 · Cited by 2,572 · see citing works
Artificial neural networks for solving ordinary and partial differential equations
Lagaris, I. E., Likas, A., & Fotiadis, D. I. (1998) · IEEE Transactions on Neural Networks · doi:10.1109/72.712178 · Cited by 2,440 · see citing works
Barren plateaus in quantum neural network training landscapes
McClean, J. R., Boixo, S., Smelyanskiy, V. N., Babbush, R., & Neven, H. (2018) · Nature Communications · doi:10.1038/s41467-018-07090-4 · Cited by 2,329 · see citing works
The theory of variational hybrid quantum-classical algorithms
McClean, J. R., Romero, J., Babbush, R., & Aspuru-Guzik, A. (2016) · New Journal of Physics · doi:10.1088/1367-2630/18/2/023023 · Cited by 2,227 · see citing works
DGM: A deep learning algorithm for solving partial differential equations
Sirignano, J. A., & Spiliopoulos, K. (2018) · Journal of Computational Physics · doi:10.1016/j.jcp.2018.08.029 · Cited by 2,216 · see citing works
Hidden fluid mechanics: Learning velocity and pressure fields from flow visualizations
Raissi, M., Yazdani, A. Z. K., & Karniadakis, G. E. (2020) · Science · doi:10.1126/science.aaw4741 · Cited by 2,127 · see citing works
Quantum Support Vector Machine for Big Data Classification
Rebentrost, P., Mohseni, M., & Lloyd, S. (2014) · Physical Review Letters · doi:10.1103/physrevlett.113.130503 · Cited by 1,951 · see citing works
Computational fluid dynamics : the basics with applications
Anderson, J. D. (1995) · Cited by 1,879 · see citing works
Quantum Machine Learning in Feature Hilbert Spaces
Schuld, M., & Killoran, N. (2019) · Physical Review Letters · doi:10.1103/physrevlett.122.040504 · Cited by 1,840 · see citing works
Mitarai, K., Negoro, M., Kitagawa, M., & Fujii, K. (2018) · Physical Review A · doi:10.1103/physreva.98.032309 · Cited by 1,639 · see citing works
Numerical Methods for Ordinary Differential Equations
Butcher, J. C. (2008) · Wiley eBooks · doi:10.1002/9780470753767 · Cited by 1,625 · see citing works
Quantum computational chemistry
McArdle, S., Endo, S., Aspuru-Guzik, A., Benjamin, S. C., & Yuan, X. (2020) · Reviews of Modern Physics · doi:10.1103/revmodphys.92.015003 · Cited by 1,621 · see citing works
Quantum Chemistry in the Age of Quantum Computing
Cao, Y., Romero, J., Olson, J. P., Degroote, M., Johnson, P. D., Kieferová, M., Kivlichan, I. D., Menke, T., Peropadre, B., Sawaya, N. P. D., et al. (2019) · Chemical Reviews · doi:10.1021/acs.chemrev.8b00803 · Cited by 1,560 · see citing works
Quantum convolutional neural networks
Cong, I., Choi, S., & Lukin, M. D. (2019) · Nature Physics · doi:10.1038/s41567-019-0648-8 · Cited by 1,517 · see citing works
Quantum principal component analysis
Lloyd, S., Mohseni, M., & Rebentrost, P. (2014) · Nature Physics · doi:10.1038/nphys3029 · Cited by 1,385 · see citing works
An introduction to quantum machine learning
Schuld, M., Sinayskiy, I., & Petruccione, F. (2015) · Contemporary Physics · doi:10.1080/00107514.2014.964942 · Cited by 1,381 · see citing works
Error Mitigation for Short-Depth Quantum Circuits
Temme, K., Bravyi, S., & Gambetta, J. M. (2017) · Physical Review Letters · doi:10.1103/physrevlett.119.180509 · Cited by 1,379 · see citing works
Regularization Theory and Neural Networks Architectures
Girosi, F., Jones, M., & Poggio, T. (1995) · Neural Computation · doi:10.1162/neco.1995.7.2.219 · Cited by 1,345 · see citing works
Parameterized quantum circuits as machine learning models
Benedetti, M., Lloyd, E., Sack, S., & Fiorentini, M. (2019) · Quantum Science and Technology · doi:10.1088/2058-9565/ab4eb5 · Cited by 1,324 · see citing works
Fourier Neural Operator for Parametric Partial Differential EquationsPreprint
Li, Z., Kovachki, N., Azizzadenesheli, K., Liu, B., Bhattacharya, K., Stuart, A. M., & Anandkumar, A. (2020) · arXiv (Cornell University) · doi:10.48550/arxiv.2010.08895 · Cited by 1,296 · see citing works
Quantum Chemistry in the Age of Quantum Computing
Cao, Y., Romero, J., Olson, J., Degroote, M., Johnson, P., Kieferová, M., Kivlichan, I., Menke, T., Peropadre, B., Sawaya, N., et al. (n.d.) · OPUS - Open Publications of UTS Scholars (University of Technology Sydney) · Cited by 1,265 · see citing works
Machine learning & artificial intelligence in the quantum domain: a review of recent progress
Dunjko, V., & Briegel, H. J. (2018) · Reports on Progress in Physics · doi:10.1088/1361-6633/aab406 · Cited by 1,132 · see citing works
Evaluating analytic gradients on quantum hardware
Schuld, M., Bergholm, V., Gogolin, C., Izaac, J., & Killoran, N. (2019) · Physical Review A · doi:10.1103/physreva.99.032331 · Cited by 1,072 · see citing works
Quantum algorithms: an overview
Montanaro, A. (2016) · npj Quantum Information · doi:10.1038/npjqi.2015.23 · Cited by 1,071 · cited 1× · see citing works
“Quantum computers o ff er a fundamentally di ff erent approach to perform computation, and possess algorithmically superior scaling for certain problems that include amplitude amplification and Abelian hidden subgroup problems [7, 8].”
BackgroundScalable Quantum Simulation of Molecular Energies
O’Malley, P. J. J., Babbush, R., Kivlichan, I. D., Romero, J., McClean, J. R., Barends, R., Kelly, J., Roushan, P., Tranter, A., Ding, N., et al. (2016) · Physical Review X · doi:10.1103/physrevx.6.031007 · Cited by 1,059 · see citing works
Circuit-centric quantum classifiers
Schuld, M., Bocharov, A., Svore, K. M., & Wiebe, N. (2020) · Physical Review A · doi:10.1103/physreva.101.032308 · Cited by 1,057 · see citing works
Cost function dependent barren plateaus in shallow parametrized quantum circuits
Cerezo, M., Sone, A., Volkoff, T., Cincio, L., & Coles, P. J. (2021) · Nature Communications · doi:10.1038/s41467-021-21728-w · Cited by 1,047 · see citing works
An adaptive variational algorithm for exact molecular simulations on a quantum computer
Grimsley, H. R., Economou, S. E., Barnes, E., & Mayhall, N. J. (2019) · Nature Communications · doi:10.1038/s41467-019-10988-2 · Cited by 1,033 · see citing works
Artificial Neural Networks for Solving Ordinary and Partial Differential Equations
Lagaris, I. E., Likas, A., & Fotiadis, D. I. (1998) · Cited by 944 · see citing works
Giovannetti, V., Lloyd, S., & Maccone, L. (2008) · Physical Review Letters · doi:10.1103/physrevlett.100.160501 · Cited by 935 · see citing works
Classification with Quantum Neural Networks on Near Term Processors
Farhi, E., & Neven, H. (2020) · doi:10.37686/qrl.v1i2.80 · Cited by 909 · see citing works
Hartree-Fock on a superconducting qubit quantum computer
Collaborators, G. A. Q. A., Arute, F., Arya, K., Babbush, R., Bacon, D., Bardin, J. C., Barends, R., Boixo, S., Broughton, M., Buckley, B. B., et al. (2020) · Science · doi:10.1126/science.abb9811 · Cited by 824 · see citing works
Approximation Theory and Methods
Powell, M. J. D. (1981) · Cambridge University Press eBooks · doi:10.1017/cbo9781139171502 · Cited by 776 · see citing works
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
Effect of data encoding on the expressive power of variational quantum-machine-learning models
Schuld, M., Sweke, R., & Meyer, J. J. (2021) · Physical Review A · doi:10.1103/physreva.103.032430 · Cited by 739 · see citing works
Training deep quantum neural networks
Beer, K., Bondarenko, D., Farrelly, T., Osborne, T. J., Salzmann, R., Scheiermann, D., & Wolf, R. (2020) · Nature Communications · doi:10.1038/s41467-020-14454-2 · Cited by 726 · see citing works
Efficient Variational Quantum Simulator Incorporating Active Error Minimization
Li, Y., & Benjamin, S. C. (2017) · Physical Review X · doi:10.1103/physrevx.7.021050 · Cited by 686 · see citing works
Solving Ill-Conditioned and Singular Linear Systems: A Tutorial on Regularization
Neumaier, A. (1998) · SIAM Review · doi:10.1137/s0036144597321909 · Cited by 646 · see citing works
Childs, A. M., Kothari, R., & Somma, R. D. (2017) · SIAM Journal on Computing · doi:10.1137/16m1087072 · Cited by 646 · see citing works
Universal Differential Equations for Scientific Machine Learning
Rackauckas, C., Ma, Y., Martensen, J., Warner, C., Zubov, K., Supekar, R., Skinner, D., Ramadhan, A., & Edelman, A. (2020) · doi:10.21203/rs.3.rs-55125/v1 · Cited by 643 · see citing works
Self-verifying variational quantum simulation of lattice models
Kokail, C., Maier, C., van Bijnen, R., Brydges, T., Joshi, M. K., Jurcevic, P., Muschik, C. A., Silvi, P., Blatt, R., Roos, C. F., et al. (2019) · Nature · doi:10.1038/s41586-019-1177-4 · Cited by 594 · see citing works
Quantum Generative Adversarial Learning
Lloyd, S., & Weedbrook, C. (2018) · Physical Review Letters · doi:10.1103/physrevlett.121.040502 · Cited by 576 · see citing works
Practical Quantum Error Mitigation for Near-Future Applications
Endo, S., Benjamin, S. C., & Li, Y. (2018) · Physical Review X · doi:10.1103/physrevx.8.031027 · Cited by 562 · see citing works
Variational ansatz-based quantum simulation of imaginary time evolution
McArdle, S., Jones, T., Endo, S., Li, Y., Benjamin, S. C., & Yuan, X. (2019) · npj Quantum Information · doi:10.1038/s41534-019-0187-2 · Cited by 557 · see citing works
Quantum Generative Adversarial Networks for learning and loading random distributions
Zoufal, C., Lucchi, A., & Woerner, S. (2019) · npj Quantum Information · doi:10.1038/s41534-019-0223-2 · Cited by 480 · see citing works
Stokes, J., Izaac, J., Killoran, N., & Carleo, G. (2020) · Quantum · doi:10.22331/q-2020-05-25-269 · Cited by 473 · see citing works
Quantum-Enhanced Machine Learning
Dunjko, V., Taylor, J. M., & Briegel, H. J. (2016) · Physical Review Letters · doi:10.1103/physrevlett.117.130501 · Cited by 460 · see citing works
Computation of Molecular Spectra on a Quantum Processor with an Error-Resilient Algorithm
Colless, J. I., Ramasesh, V. V., Dahlen, D., Blok, M. S., Kimchi-Schwartz, M. E., McClean, J. R., Carter, J., de Jong, W. A., & Siddiqi, I. (2018) · Physical Review X · doi:10.1103/physrevx.8.011021 · Cited by 460 · see citing works
An introduction to quantum machine learningPreprint
Schuld, M., Sinayskiy, I., & Petruccione, F. (2014) · Cited by 435 · see citing works
Quantum Generative Adversarial Networks for learning and loading random distributions
Zoufal, C., Lucchi, A., & Woerner, S. (2019) · Repository for Publications and Research Data (ETH Zurich) · doi:10.3929/ethz-b-000382432 · Cited by 390 · see citing works
A generative modeling approach for benchmarking and training shallow quantum circuits
Benedetti, M., Garcia-Pintos, D., Perdomo, O., Leyton-Ortega, V., Nam, Y., & Perdomo-Ortiz, A. (2019) · npj Quantum Information · doi:10.1038/s41534-019-0157-8 · Cited by 379 · see citing works
Towards quantum machine learning with tensor networks
Huggins, W. J., Patil, P., Mitchell, B., Whaley, K. B., & Stoudenmire, E. M. (2018) · Quantum Science and Technology · doi:10.1088/2058-9565/aaea94 · Cited by 363 · see citing works
Variational Quantum Linear Solver
Bravo-Prieto, C., LaRose, R., Cerezo, M., Subaşı, Y., Cincio, Ł., & Coles, P. J. (2023) · Quantum · doi:10.22331/q-2023-11-22-1188 · Cited by 359 · see citing works
Ground-state energy estimation of the water molecule on a trapped-ion quantum computer
Nam, Y., Chen, J.-S., Pisenti, N. C., Wright, K., Delaney, C. P., Maslov, D., Brown, K. R., Allen, S., Amini, J., Apisdorf, J., et al. (2020) · npj Quantum Information · doi:10.1038/s41534-020-0259-3 · Cited by 346 · see citing works
Absence of Barren Plateaus in Quantum Convolutional Neural Networks
Pesah, A., Cerezo, M., Wang, S., Volkoff, T., Sornborger, A. T., & Coles, P. J. (2021) · Physical Review X · doi:10.1103/physrevx.11.041011 · Cited by 343 · see citing works
Subspace-search variational quantum eigensolver for excited states
Nakanishi, K. M., Mitarai, K., & Fujii, K. (2019) · Physical Review Research · doi:10.1103/physrevresearch.1.033062 · Cited by 337 · see citing works
Variational quantum algorithms for nonlinear problems
Lubasch, M., Joo, J., Moinier, P., Kiffner, M., & Jaksch, D. (2020) · Physical Review A · doi:10.1103/physreva.101.010301 · Cited by 332 · see citing works
Layerwise learning for quantum neural networks
Skolik, A., McClean, J. R., Mohseni, M., van der Smagt, P., & Leib, M. (2021) · Quantum Machine Intelligence · doi:10.1007/s42484-020-00036-4 · Cited by 324 · see citing works
Active learning machine learns to create new quantum experiments
Melnikov, A. A., Nautrup, H. P., Krenn, M., Dunjko, V., Tiersch, M., Zeilinger, A., & Briegel, H. J. (2018) · Proceedings of the National Academy of Sciences · doi:10.1073/pnas.1714936115 · Cited by 290 · see citing works
Quantum Computation of Electronic Transitions Using a Variational Quantum Eigensolver
Parrish, R. M., Hohenstein, E. G., McMahon, P. L., & Martínez, T. J. (2019) · Physical Review Letters · doi:10.1103/physrevlett.122.230401 · Cited by 282 · see citing works
Differentiable learning of quantum circuit Born machines
Liu, J.-G., & Wang, L. (2018) · Physical Review A · doi:10.1103/physreva.98.062324 · Cited by 279 · see citing works
High-order quantum algorithm for solving linear differential equations
Berry, D. W. (2014) · Journal of Physics A: Mathematical and Theoretical · doi:10.1088/1751-8113/47/10/105301 · Cited by 277 · see citing works
Prediction by linear regression on a quantum computer
Schuld, M., Sinayskiy, I., & Petruccione, F. (2016) · Physical Review A · doi:10.1103/physreva.94.022342 · Cited by 277 · see citing works
Opportunities and challenges for quantum-assisted machine learning in near-term quantum computers
Perdomo-Ortiz, A., Benedetti, M., Realpe-Gómez, J., & Biswas, R. (2018) · Quantum Science and Technology · doi:10.1088/2058-9565/aab859 · Cited by 274 · see citing works
Gard, B. T., Zhu, L., Barron, G. S., Mayhall, N. J., Economou, S. E., & Barnes, E. (2020) · npj Quantum Information · doi:10.1038/s41534-019-0240-1 · Cited by 266 · see citing works
Unsupervised Machine Learning on a Hybrid Quantum Computer
Otterbach, J. S., Manenti, R., Alidoust, N., Bestwick, A., Block, M., Bloom, B., Caldwell, S., Didier, N., Fried, E. S., Hong, S., et al. (2017) · arXiv · doi:10.48550/arxiv.1712.05771 · Cited by 263 · see citing works
Efficient and noise resilient measurements for quantum chemistry on near-term quantum computers
Huggins, W. J., McClean, J. R., Rubin, N. C., Jiang, Z., Wiebe, N., Whaley, K. B., & Babbush, R. (2021) · npj Quantum Information · doi:10.1038/s41534-020-00341-7 · Cited by 256 · see citing works
Low-cost error mitigation by symmetry verification
Bonet-Monroig, X., Sagastizabal, R., Singh, M., & O'Brien, T. E. (2018) · Physical Review A · doi:10.1103/physreva.98.062339 · Cited by 250 · see citing works
Quantum algorithms for topological and geometric analysis of data
Lloyd, S., Garnerone, S., & Zanardi, P. (2016) · Nature Communications · doi:10.1038/ncomms10138 · Cited by 241 · see citing works
Error-Mitigated Digital Quantum Simulation
McArdle, S., Yuan, X., & Benjamin, S. C. (2019) · Physical Review Letters · doi:10.1103/physrevlett.122.180501 · Cited by 238 · see citing works
Variational Quantum Simulation of General Processes
Endo, S., Sun, J., Li, Y., Benjamin, S. C., & Yuan, X. (2020) · Physical Review Letters · doi:10.1103/physrevlett.125.010501 · Cited by 237 · see citing works
Variational fast forwarding for quantum simulation beyond the coherence time
Cîrstoiu, C., Holmes, Z., Iosue, J., Cincio, L., Coles, P. J., & Sornborger, A. (2020) · npj Quantum Information · doi:10.1038/s41534-020-00302-0 · Cited by 232 · see citing works
Quantum Linear System Algorithm for Dense Matrices
Wossnig, L., Zhao, Z., & Prakash, A. (2018) · Physical Review Letters · doi:10.1103/physrevlett.120.050502 · Cited by 224 · see citing works
Stochastic gradient descent for hybrid quantum-classical optimization
Sweke, R., Wilde, F., Meyer, J., Schuld, M., Faehrmann, P. K., Meynard-Piganeau, B., & Eisert, J. (2020) · Quantum · doi:10.22331/q-2020-08-31-314 · Cited by 219 · see citing works
Berry, D. W., Childs, A. M., Ostrander, A., & Wang, G. (2017) · Communications in Mathematical Physics · doi:10.1007/s00220-017-3002-y · Cited by 218 · see citing works
Quantum chemistry as a benchmark for near-term quantum computers
McCaskey, A., Parks, Z. P., Jakowski, J., Moore, S., Morris, T., Humble, T. S., & Pooser, R. C. (2019) · npj Quantum Information · doi:10.1038/s41534-019-0209-0 · Cited by 216 · see citing works
Training of quantum circuits on a hybrid quantum computer
Zhu, D., Linke, N. M., Benedetti, M., Landsman, K. A., Nguyen, N. H., Alderete, C. H., Perdomo-Ortiz, A., Korda, N., Garfoot, A., Brecque, C., et al. (2019) · Science Advances · doi:10.1126/sciadv.aaw9918 · Cited by 215 · see citing works
Stochastic gradient descent for hybrid quantum-classical optimization
Sweke, R., Sweke, R., Meyer, J. J., Meyer, J. J., Faehrmann, P. K., Meynard-Piganeau, B., & Eisert, J. (2020) · Refubium (Universitätsbibliothek der Freien Universität Berlin) · doi:10.17169/refubium-28427 · Cited by 203 · see citing works
Quantum algorithms and the finite element method
Montanaro, A., & Pallister, S. (2016) · Physical Review A · doi:10.1103/physreva.93.032324 · Cited by 192 · see citing works
Quantum classifier with tailored quantum kernel
Blank, C., Park, D. K., Rhee, J. K., & Petruccione, F. (2020) · npj Quantum Information · doi:10.1038/s41534-020-0272-6 · Cited by 191 · see citing works
Romero, J., & Aspuru‐Guzik, A. (2021) · Advanced Quantum Technologies · doi:10.1002/qute.202000003 · Cited by 186 · see citing works
Quantum Algorithms for Systems of Linear Equations Inspired by Adiabatic Quantum Computing
Subaşı, Y., Somma, R. D., & Orsucci, D. (2019) · Physical Review Letters · doi:10.1103/physrevlett.122.060504 · Cited by 183 · see citing works
Yen, T.-C., Verteletskyi, V., & Izmaylov, A. F. (2020) · Journal of Chemical Theory and Computation · doi:10.1021/acs.jctc.0c00008 · Cited by 178 · see citing works
Finding flows of a Navier–Stokes fluid through quantum computing
Gaitan, F. (2020) · npj Quantum Information · doi:10.1038/s41534-020-00291-0 · Cited by 175 · see citing works
Bachmayr, M., Schneider, R., & Uschmajew, A. (2016) · Foundations of Computational Mathematics · doi:10.1007/s10208-016-9317-9 · Cited by 173 · see citing works
Quantum convolutional neural networks for high energy physics data analysis
Chen, S. Y.-C., Wei, T.-C., Zhang, C., Yu, H., & Yoo, S. (2022) · Physical Review Research · doi:10.1103/physrevresearch.4.013231 · Cited by 171 · see citing works
Variational algorithms for linear algebra
Xu, X., Sun, J., Endo, S., Li, Y., Benjamin, S. C., & Yuan, X. (2021) · 中国科学通报:英文版 · doi:10.1016/j.scib.2021.06.023 · Cited by 170 · see citing works
Differentiable quantum architecture search
Zhang, S., Hsieh, C., Zhang, S., & Yao, H. (2022) · Quantum Science and Technology · doi:10.1088/2058-9565/ac87cd · Cited by 170 · see citing works
Variational quantum eigensolver with fewer qubits
Liu, J.-G., Zhang, Y.-H., Wan, Y., & Wang, L. (2019) · Physical Review Research · doi:10.1103/physrevresearch.1.023025 · Cited by 166 · see citing works
Quantum computation and quantum information
Raychev, N., & Chuang, I. L. (2020) · doi:10.37686/qrl.v1i1.57 · Cited by 162 · see citing works
Quantum algorithm for simulating the wave equation
Costa, P. C. S., Jordan, S. P., & Ostrander, A. (2019) · Physical Review A · doi:10.1103/physreva.99.012323 · Cited by 159 · see citing works
Estimating the gradient and higher-order derivatives on quantum hardware
Mari, A., Bromley, T. R., & Killoran, N. (2021) · Physical Review A · doi:10.1103/physreva.103.012405 · Cited by 159 · see citing works
Yao.jl: Extensible, Efficient Framework for Quantum Algorithm Design
Luo, X.-Z., Liu, J.-G., Zhang, P., & Wang, L. (2020) · Quantum · doi:10.22331/q-2020-10-11-341 · Cited by 157 · see citing works
High-precision quantum algorithms for partial differential equations
Childs, A. M., Liu, J.-P., & Ostrander, A. (2021) · Quantum · doi:10.22331/q-2021-11-10-574 · Cited by 157 · see citing works
Quantum noise protects quantum classifiers against adversaries
Du, Y., Hsieh, M.-H., Liu, T., Tao, D., & Liu, N. (2021) · Physical Review Research · doi:10.1103/physrevresearch.3.023153 · Cited by 157 · see citing works
The Born supremacy: quantum advantage and training of an Ising Born machine
Coyle, B., Mills, D., Danos, V., & Kashefi, E. (2020) · npj Quantum Information · doi:10.1038/s41534-020-00288-9 · Cited by 155 · see citing works
Quantum gradient descent and Newton’s method for constrained polynomial optimization
Rebentrost, P., Schuld, M., Wossnig, L., Petruccione, F., & Lloyd, S. (2019) · New Journal of Physics · doi:10.1088/1367-2630/ab2a9e · Cited by 152 · see citing works
Quantum machine learning for quantum anomaly detection
Liu, N., & Rebentrost, P. (2018) · Physical Review A · doi:10.1103/physreva.97.042315 · Cited by 149 · see citing works
Gate-Efficient Simulation of Molecular Eigenstates on a Quantum Computer
Ganzhorn, M., Egger, D. J., Barkoutsos, P., Ollitrault, P. J., Salis, G., Moll, N., Roth, M., Fuhrer, A., Mueller, P., Woerner, S., et al. (2019) · Physical Review Applied · doi:10.1103/physrevapplied.11.044092 · Cited by 142 · see citing works
An Adaptive Optimizer for Measurement-Frugal Variational Algorithms
Kübler, J. M., Arrasmith, A., Cincio, L., & Coles, P. J. (2020) · Quantum · doi:10.22331/q-2020-05-11-263 · Cited by 141 · see citing works
Methodology for replacing indirect measurements with direct measurements
Mitarai, K., & Fujii, K. (2019) · Physical Review Research · doi:10.1103/physrevresearch.1.013006 · Cited by 139 · see citing works
Quantum Spectral Methods for Differential Equations
Childs, A. M., & Liu, J.-P. (2020) · Communications in Mathematical Physics · doi:10.1007/s00220-020-03699-z · Cited by 133 · see citing works
Simulating 2D Effects in Lattice Gauge Theories on a Quantum Computer
Paulson, D., Dellantonio, L., Haase, J. F., Celi, A., Kan, A., Jena, A., Kokail, C., van Bijnen, R., Jansen, K., Zoller, P., et al. (2021) · PRX Quantum · doi:10.1103/prxquantum.2.030334 · Cited by 131 · see citing works
Quantum gradient descent and Newton’s method for constrained polynomial optimization
Rebentrost, F. P., & Lloyd, S. (2019) · DSpace@MIT (Massachusetts Institute of Technology) · Cited by 130 · see citing works
Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables.
S., D., Abramowitz, M., & Stegun, I. A. (1966) · Mathematics of Computation · doi:10.2307/2004284 · Cited by 129 · see citing works
Machine Learning for Long-Distance Quantum Communication
Wallnöfer, J., Melnikov, A. A., Dür, W., & Briegel, H. J. (2020) · PRX Quantum · doi:10.1103/prxquantum.1.010301 · Cited by 121 · see citing works
Expressibility of the alternating layered ansatz for quantum computation
Nakaji, K., & Yamamoto, N. (2021) · Quantum · doi:10.22331/q-2021-04-19-434 · Cited by 119 · see citing works
Quantum Autoencoders to Denoise Quantum Data
Bondarenko, D., & Feldmann, P. (2020) · Physical Review Letters · doi:10.1103/physrevlett.124.130502 · Cited by 115 · see citing works
Experimental realization of quantum algorithm for solving linear systems of equations
Pan, J., Cao, Y., Yao, X., Li, Z., Ju, C., Chen, H., Peng, X., Kais, S., & Du, J. (2014) · Physical Review A · doi:10.1103/physreva.89.022313 · Cited by 110 · see citing works
A variational toolbox for quantum multi-parameter estimation
Meyer, J. J., Borregaard, J., & Eisert, J. (2021) · npj Quantum Information · doi:10.1038/s41534-021-00425-y · Cited by 109 · see citing works
Gate-Efficient Simulation of Molecular Eigenstates on a Quantum Computer
Ganzhorn, M., Egger, D. J., Tavernelli, I., Filipp, S., Barkoutsos, P. K., Ollitrault, P. J., Salis, G., Moll, N., Roth, M., Fuhrer, A., et al. (2019) · RWTH Publications (RWTH Aachen) · Cited by 109 · see citing works
Lin, L., & Tong, Y. (2020) · Quantum · doi:10.22331/q-2020-11-11-361 · Cited by 106 · see citing works
Variational-state quantum metrology
Koczor, B., Endo, S., Jones, T., Matsuzaki, Y., & Benjamin, S. C. (2020) · New Journal of Physics · doi:10.1088/1367-2630/ab965e · Cited by 101 · see citing works
Calculating energy derivatives for quantum chemistry on a quantum computer
O’Brien, T. E., Senjean, B., Sagastizabal, R., Bonet-Monroig, X., Dutkiewicz, A., Buda, F., DiCarlo, L., & Visscher, L. (2019) · npj Quantum Information · doi:10.1038/s41534-019-0213-4 · Cited by 100 · see citing works
Robust determination of molecular spectra on a quantum processorPreprint
Colless, J., Ramasesh, V., Dahlen, D., et al. (2017) · arXiv (Cornell University) · doi:10.48550/arxiv.1707.06408 · Cited by 95 · see citing works
Learning and inference on generative adversarial quantum circuits
Zeng, J., Wu, Y., Liu, J.-G., Wang, L., & Hu, J. (2019) · Physical Review A · doi:10.1103/physreva.99.052306 · Cited by 94 · see citing works
Elfving, V. E., Broer, B. W., Webber, M., Gavartin, J. L., Halls, M. D., Lorton, K. P., & Bochevarov, A. D. (2020) · arXiv (Cornell University) · doi:10.48550/arxiv.2009.12472 · Cited by 93 · see citing works
Self-citationA quantum algorithm to train neural networks using low-depth circuits
Verdon, G., Broughton, M., & Biamonte, J. (2017) · arXiv · doi:10.48550/arxiv.1712.05304 · Cited by 87 · see citing works
Quantum algorithm for solving linear differential equations: Theory and experiment
Xin, T., Wei, S., Cui, J., Xiao, J., Arrazola, Í., Lamata, L., Kong, X., Lu, D., Solano, E., & Long, G. (2020) · Physical Review A · doi:10.1103/physreva.101.032307 · Cited by 85 · see citing works
DiffEqFlux.jl - A Julia Library for Neural Differential EquationsPreprint
Rackauckas, C., Innes, M. J., Ma, Y., Bettencourt, J., White, L., & Dixit, V. (2019) · arXiv (Cornell University) · doi:10.48550/arxiv.1902.02376 · Cited by 84 · see citing works
Cost-Function-Dependent Barren Plateaus in Shallow Quantum Neural Networks.Preprint
Cerezo, M., Sone, A., Volkoff, T. J., Cincio, Ł., & Coles, P. J. (2020) · arXiv (Cornell University) · Cited by 83 · see citing works
Yalouz, S., Senjean, B., Günther, J., Buda, F., O’Brien, T. E., & Visscher, L. (2020) · Quantum Science and Technology · doi:10.1088/2058-9565/abd334 · Cited by 82 · see citing works
Lin, L., & Tong, Y. (2020) · eScholarship (California Digital Library) · Cited by 82 · see citing works
Adversarial quantum circuit learning for pure state approximation
Benedetti, M., Grant, E., Wossnig, L., & Simone Severini, B. (2019) · New Journal of Physics · doi:10.1088/1367-2630/ab14b5 · Cited by 80 · see citing works
Quantum vs. Classical Algorithms for Solving the Heat Equation
Linden, N., Montanaro, A., & Shao, C. (2022) · Communications in Mathematical Physics · doi:10.1007/s00220-022-04442-6 · Cited by 79 · see citing works
Metcalf, M., Bauman, N. P., Kowalski, K., & de Jong, W. A. (2020) · Journal of Chemical Theory and Computation · doi:10.1021/acs.jctc.0c00421 · Cited by 78 · see citing works
Theory of analytical energy derivatives for the variational quantum eigensolver
Mitarai, K., Nakagawa, Y. O., & Mizukami, W. (2020) · Physical Review Research · doi:10.1103/physrevresearch.2.013129 · Cited by 76 · see citing works
Scherer, A., Valiron, B., Mau, S.-C., Alexander, S., van den Berg, E., & Chapuran, T. E. (2017) · Quantum Information Processing · doi:10.1007/s11128-016-1495-5 · Cited by 73 · see citing works
Efficient Discrete Feature Encoding for Variational Quantum Classifier
Yano, H., Suzuki, Y., Itoh, K. M., Raymond, R., & Yamamoto, N. (2020) · IEEE International Conference on Quantum Computing and Engineering (QCE) · doi:10.1109/qce49297.2020.00012 · Cited by 73 · see citing works
MoG-VQE: Multiobjective genetic variational quantum eigensolverPreprint
Сергеевич, Ч. Д., Samarin, A., Игоревич, У. В., Iorsh, I. V., Оганов, А. Р., & Kyriienko, O. (2020) · arXiv (Cornell University) · doi:10.48550/arxiv.2007.04424 · Cited by 73 · see citing works
Self-citationInput Redundancy for Parameterized Quantum Circuits
Vidal, F. J. G., & Theis, D. O. (2020) · Frontiers in Physics · doi:10.3389/fphy.2020.00297 · Cited by 71 · see citing works
Advances in Quantum Deep Learning: An OverviewPreprint
Garg, S., & Ramakrishnan, G. (2020) · arXiv (Cornell University) · doi:10.48550/arxiv.2005.04316 · Cited by 70 · see citing works
García‐Ripoll, J. J. (2021) · Quantum · doi:10.22331/q-2021-04-15-431 · Cited by 69 · see citing works
A universal training algorithm for quantum deep learning
Verdon, G., Pye, J., & Broughton, M. (2018) · arXiv · doi:10.48550/arxiv.1806.09729 · Cited by 68 · see citing works
Adaptive pruning-based optimization of parameterized quantum circuits
Sim, S., Romero, J., Gonthier, J. F., & Kunitsa, A. A. (2021) · Quantum Science and Technology · doi:10.1088/2058-9565/abe107 · Cited by 66 · see citing works
A quantum algorithm to solve nonlinear differential equations
Leyton, S. K., & Osborne, T. J. (2008) · arXiv · doi:10.48550/arxiv.0812.4423 · Cited by 65 · see citing works
Quantum circuit design for solving linear systems of equations
Cao, Y., Daskin, A., Frankel, S., & Kais, S. (2012) · Molecular Physics · doi:10.1080/00268976.2012.668289 · Cited by 65 · see citing works
Near-term quantum algorithms for linear systems of equations
Huang, H.-Y., Bharti, K., & Rebentrost, P. (2019) · arXiv · doi:10.48550/arxiv.1909.07344 · Cited by 62 · see citing works
Analysis and synthesis of feature map for kernel-based quantum classifier
Suzuki, Y., Yano, H., Gao, Q., Uno, S., Tanaka, T., Akiyama, M., & Yamamoto, N. (2020) · Quantum Machine Intelligence · doi:10.1007/s42484-020-00020-y · Cited by 62 · see citing works
Quantum inverse iteration algorithm for programmable quantum simulators
Kyriienko, O. (2020) · npj Quantum Information · doi:10.1038/s41534-019-0239-7 · Cited by 62 · see citing works
Self-citationMeasurement-based adaptation protocol with quantum reinforcement learning
Albarrán-Arriagada, F., Retamal, J. C., Solano, E., & Lamata, L. (2018) · Physical Review A · doi:10.1103/physreva.98.042315 · Cited by 59 · see citing works
Computational Investigations of the Lithium Superoxide Dimer Rearrangement on Noisy Quantum Devices
Gao, Q., Nakamura, H., Gujarati, T. P., Jones, G. O., Rice, J. E., Wood, S., Pistoia, M., Garcı́a, J. M., & Yamamoto, N. (2021) · The Journal of Physical Chemistry A · doi:10.1021/acs.jpca.0c09530 · Cited by 59 · see citing works
Quantum machine learning and quantum biomimetics: A perspective
Lamata, L. (2020) · Machine Learning Science and Technology · doi:10.1088/2632-2153/ab9803 · Cited by 58 · see citing works
Numerical Solution of Ordinary Differential Equations: Is There Anything Left to Do?
Gear, C. W. (1981) · SIAM Review · doi:10.1137/1023002 · Cited by 53 · see citing works
Benchmarking Adaptive Variational Quantum Eigensolvers
Claudino, D., Wright, J., McCaskey, A. J., & Humble, T. S. (2020) · Frontiers in Chemistry · doi:10.3389/fchem.2020.606863 · Cited by 52 · see citing works
Kreula, J. M., Clark, S. R., & Jaksch, D. (2016) · Scientific Reports · doi:10.1038/srep32940 · Cited by 49 · see citing works
Koczor, B., & Benjamin, S. C. (2022) · Physical Review Research · doi:10.1103/physrevresearch.4.023017 · Cited by 48 · see citing works
Simulating quantum chemistry in the seniority-zero space on qubit-based quantum computers
Elfving, V. E., Millaruelo, M., Gámez, J. A., & Gogolin, C. (2021) · Physical Review A · doi:10.1103/physreva.103.032605 · Cited by 48 · see citing works
Self-citationAccounting for errors in quantum algorithms via individual error reduction
Otten, M., & Gray, S. K. (2019) · npj Quantum Information · doi:10.1038/s41534-019-0125-3 · Cited by 47 · see citing works
Enhancing the Quantum Linear Systems Algorithm Using Richardson Extrapolation
Vazquez, A. C., Hiptmair, R., & Woerner, S. (2022) · ACM Transactions on Quantum Computing · doi:10.1145/3490631 · Cited by 46 · see citing works
Hybrid classical-quantum linear solver using Noisy Intermediate-Scale Quantum machines
Chen, C.-C., Shiau, S.-Y., Wu, M.-F., & Wu, Y.-R. (2019) · Scientific Reports · doi:10.1038/s41598-019-52275-6 · Cited by 41 · see citing works
Differential equations: with applications and historical notes
Boyer, C. B. (1974) · Historia Mathematica · doi:10.1016/0315-0860(74)90191-8 · Cited by 40 · see citing works
On the natural gradient for variational quantum eigensolver
Yamamoto, N. (2019) · arXiv · doi:10.48550/arxiv.1909.05074 · Cited by 39 · see citing works
Hamiltonian operator approximation for energy measurement and ground state preparation
(21925472), T. B., & Kyriienko, O. (2025) · Figshare · Cited by 39 · see citing works
Self-citationToward Trainability of Quantum Neural Networks
Zhang, K., Hsieh, M.-H., Liu, L., & Tao, D. (2020) · arXiv · doi:10.48550/arxiv.2011.06258 · Cited by 36 · see citing works
Bauman, N. P., Chládek, J., Veis, L., Pittner, J., & Kowalski, K. (2021) · Quantum Science and Technology · doi:10.1088/2058-9565/abf602 · Cited by 36 · see citing works
Quantum natural gradient generalised to non-unitary circuitsPreprint
Koczor, B., & Benjamin, S. C. (2019) · arXiv (Cornell University) · Cited by 35 · see citing works
Setting Up Experimental Bell Tests with Reinforcement Learning
Melnikov, A. A., Sekatski, P., & Sangouard, N. (2020) · Physical Review Letters · doi:10.1103/physrevlett.125.160401 · Cited by 35 · see citing works
Du, Y., Huang, T., You, S., Hsieh, M.-H., & Tao, D. (2020) · arXiv (Cornell University) · Cited by 35 · see citing works
Robust Quantum Metrology With Explicit Symmetric States
Ouyang, Y., Shettell, N., & Markham, D. (2021) · IEEE Transactions on Information Theory · doi:10.1109/tit.2021.3132634 · Cited by 34 · see citing works
Quantum approximate optimization for hard problems in linear algebra
Borle, A., Elfving, V. E., & Lomonaco, S. J. (2021) · SciPost Physics Core · doi:10.21468/scipostphyscore.4.4.031 · Cited by 32 · see citing works
Self-citationQuantum inverse iteration algorithm for programmable quantum simulators
Kyriienko, O. (2025) · Figshare · Cited by 27 · see citing works
Self-citationA diagrammatic approach to variational quantum ansatz construction
Herasymenko, Y., & O’Brien, T. E. (2021) · Quantum · doi:10.22331/q-2021-12-02-596 · Cited by 22 · see citing works
Olivares-Sánchez, J., Casanova, J., Solano, E., & Lamata, L. (2020) · Quantum Reports · doi:10.3390/quantum2020019 · Cited by 19 · see citing works
Parrish, R. M., Hohenstein, E. G., McMahon, P. L., & Martı́nez, T. J. (2019) · arXiv (Cornell University) · doi:10.48550/arxiv.1906.08728 · Cited by 18 · see citing works
Hohenstein, E. G. (2020) · OSTI OAI (U.S. Department of Energy Office of Scientific and Technical Information) · Cited by 18 · see citing works
Impact of Barren Plateaus on the Hessian and Higher Order DerivativesPreprint
Cerezo, M., & Coles, P. J. (2020) · arXiv (Cornell University) · Cited by 15 · see citing works
Universal Approximation Property of Quantum Feature MapPreprint
Goto, T., Tran, Q. H., & Nakajima, K. (2020) · arXiv (Cornell University) · Cited by 11 · see citing works
Variational Fast Forwarding for Quantum Simulation Beyond the Coherence TimePreprint
Cîrstoiu, C., Holmes, Z., Iosue, J. T., Cincio, Ł., Coles, P. J., & Sornborger, A. T. (2019) · arXiv (Cornell University) · doi:10.48550/arxiv.1910.04292 · Cited by 7 · see citing works
Elfving, V. E., Gámez, J. A., & Gogolin, C. (2020) · arXiv (Cornell University) · Cited by 6 · see citing works
Self-citationA quantum Poisson solver implementable on NISQ devicesPreprint
Wang, S., Wang, Z., Li, W., Fan, L., Cui, G., Wei, Z., & Gu, Y. (2020) · arXiv (Cornell University) · Cited by 5 · see citing works
Quantum-Assisted Clustering Algorithms for NISQ-Era DevicesPreprint
Mendelson, S. S., Strand, R. W., Oldaker, G. B., & Farinholt, J. (2019) · arXiv (Cornell University) · doi:10.48550/arxiv.1904.08992 · Cited by 4 · see citing works
Advanced quantum supremacy using a hybrid algorithm for linear systems of equationsPreprint
Perelshtein, M. R., Pakhomchik, A. I., Melnikov, A. A., Novikov, A., Glatz, A., Paraoanu, G. S., Vinokur, V. M., & Lesovik, G. B. (2020) · arXiv (Cornell University) · Cited by 4 · see citing works
Optimal quantum eigenstate filtering with application to solving quantum linear systemsPreprint
Lin, L., & Tong, Y. (2019) · arXiv (Cornell University) · Cited by 3 · see citing works
Ремез, Е. Я., & Гаврилюк, В. Т. (1960) · Ukrainian Mathematical Journal · doi:10.1007/bf02526408 · Cited by 1 · see citing works
Flagged first, then by citations
Research works printed but not linked: 1
- D. P. Kingma, 2015, Proceedings of the 3rd International Conference on Learning Representations (ICLR)
Cited by
Sorted by citations
Variational quantum algorithms
Cerezo, M., Arrasmith, A., Babbush, R., Benjamin, S. C., Endo, S., Fujii, K., McClean, J. R., Mitarai, K., Yuan, X., Cincio, L., et al. (2021) · Nature Reviews Physics · doi:10.1038/s42254-021-00348-9 · Cited by 3,385 · see citing works
Higher order derivatives of quantum neural networks with barren plateaus
Cerezo, M., & Coles, P. J. (2021) · Quantum Science and Technology · doi:10.1088/2058-9565/abf51a · Cited by 118 · see citing works
- Authors
- Kyriienko, O., Paine, A. E., & Elfving, V. E.
- Affiliations
- University of Exeter (GB)
- Qu & Co. (Netherlands) (NL)
- Venue
- Physical Review A
- Publisher
- American Physical Society (APS)
- Published
- 2021-05-17
- Volume
- 103
- Issue
- 5
- ISSN
- 0556-2791 (ISSN-L)
- 2469-9926
- 2469-9934
- OpenAlex
- W3108818881
- Semantic Scholar
- ae03babddded3cd7360cc658359e98055bff3540
- Cited by
- 185
- References
- 188
- Citations by year
- 2026: 28 · 2025: 45 · 2024: 44 · 2023: 32 · 2022: 20 · 2021: 16
- FWCI
- 9.86
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Physical Review A (publishedVersion)
- arXiv (Cornell University) (publishedVersion)
- Figshare (submittedVersion)
- Open Research Exeter (University of Exeter) (submittedVersion)
- arXiv (Cornell University)
- Topics
- Physical Sciences › Computer Science › Artificial Intelligence › Quantum Computing Algorithms and Architecture
- Physical Sciences › Mathematics › Numerical Analysis › Numerical methods for differential equations
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum many-body systems
- Keywords
- nonlinear differential equations, quantum feature maps, automatic differentiation, hybrid quantum-classical algorithms, spectral methods, Navier-Stokes equations, convergent-divergent nozzle, fluid flow, boundary conditions
About these checks
Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
Claims read by deepseek-v4.1-flash under definition version 3 (extract-v3) on 2026-10-10.
Classified by jev-1.13-20260917 (gold-guideline-v0.2) on 2026-10-10.
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