The power of quantum neural networks
Open accessAbstract
It is unknown whether near-term quantum computers are advantageous for machine learning tasks. In this work we address this question by trying to understand how powerful and trainable quantum machine learning models are in relation to popular classical neural networks. We propose the effective dimension-a measure that captures these qualities-and prove that it can be used to assess any statistical model's ability to generalize on new data. Crucially, the effective dimension is a data-dependent measure that depends on the Fisher information, which allows us to gauge the ability of a model to train. We demonstrate numerically that a class of quantum neural networks is able to achieve a considerably better effective dimension than comparable feedforward networks and train faster, suggesting an advantage for quantum machine learning, which we verify on real quantum hardware.
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TL;DR
The paper uses information geometry and the effective dimension to argue that well-designed quantum neural networks can achieve higher capacity and faster training than comparable classical feedforward networks. It links the Fisher information spectrum to barren plateaus and verifies a training advantage on the ibmq montreal 27-qubit device.
Key findings
- The quantum neural network consistently achieves the highest effective dimension over the finite-data ranges considered, followed by the easy quantum model and then the classical feedforward network; with \(s_{\text{in}}=4\), \(s_{\text{out}}=2\), and \(d=40\), the quantum model’s Fisher information spectrum is more uniform and lacks the classical model’s few very large eigenvalues.
- In training on the first two classes of the Iris dataset with \(d=8\), 100 iterations, ADAM with initial learning rate \(0.1\), and 100 trials, the quantum neural network reaches the lowest average training loss: \(23.14\%\), versus \(43.05\%\) for the easy quantum model and \(37.90\%\) for the classical network; average Fisher-Rao norms are \(117.84\), \(104.89\), and \(46.45\), respectively.
- The Fisher information spectrum connects to barren plateaus: the easy, classically simulable feature map becomes more “barren plateau-like” as qubit number increases, while the harder higher-order feature map shows resilience, with eigenvalues not concentrating near zero as system size grows.
- On real hardware, the quantum neural network is trained on the ibmq montreal 27-qubit device using 4 qubits with linear connectivity; training stabilizes after roughly 33 iterations, and the paper reports performance even better than simulated results.
Methods
- The paper defines neural networks as statistical models, uses the Fisher information matrix and effective dimension as capacity measures, proves a novel generalisation bound based on effective dimension (Theorem 3.2), and extends it to models without full-rank Fisher information via discretisation.
- It compares a quantum neural network using a depth-2 higher-order feature map and parameterised RY/CNOT variational form against classical feedforward networks and an “easy” quantum model with classically simulable angle encoding, matching models by number of trainable parameters \(d\), input size \(s_{\text{in}}\), and output size \(s_{\text{out}}\), with \(d \le 100\), \(s_{\text{in}} \in \{4,6,8,10\}\), and \(s_{\text{out}}=2\).
- Numerical experiments sample 100 parameter sets to estimate Fisher information spectra, train on the first two Iris classes with \(d=8\), 100 iterations, ADAM, learning rate \(0.1\), and 100 trials, and run one hardware training on ibmq montreal with 4 qubits and linear entanglement.
Limitations
- Stated: the hardware experiment is run only once due to limited hardware availability, and the authors note that analysis of hardware noise and spread over differently sampled initial parameters would make the results more robust.
- Stated: future work is needed on noise-induced barren plateaus, generalisation on multiple datasets, and larger models; the hard feature map’s classical hardness is conjectured rather than proven.
- Evident: comparisons are limited to specific feedforward topologies, a small Iris subset, and \(d \le 100\); effective-dimension estimates rely on Monte Carlo sampling and the paper notes that higher dimensions likely require more samples.
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- Findingcitation§ 1 Introduction · p. 2
Quantum neural networks with an easier data encoding strategy have an increased likelihood of encountering a barren plateau.
“a quantum neural network with an easier data encoding strategy, increases the likelihood of encountering a barren plateau”
Quote in the paperSubstantial claim - Findingown data§ 3.3 Generalisation error bounds · p. 6
The effective dimension for a model trained on confusion sets with increasing label corruption accurately captures generalisation behaviour.
“We find that the effective dimension for a model trained on confusion sets with increasing label corruption, accurately captures generalisation behaviour.”
Quote in the paperSubstantial claim - Findingreasoning§ Abstract · p. 1
Quantum neural networks are able to achieve a significantly better effective dimension than comparable classical neural networks.
“We show that quantum neural networks are able to achieve a significantly better effective dimension than comparable classical neural networks.”
Quote in the paperSubstantial claim - Findingreasoning§ 1 Introduction · p. 2
Quantum neural networks with a harder data encoding strategy show resilience to the barren plateau phenomenon.
“whilst a harder data encoding strategy shows resilience to the phenomenon.”
- Also stated in: § Abstract · p. 1 · plain
“Importantly, certain quantum neural networks can show resilience to this phenomenon and train faster than classical models due to their favourable optimisation landscapes, captured by a more evenly spread Fisher information spectrum.”
Quote in the paperSubstantial claim - Also stated in: § Abstract · p. 1 · plain
- Findingown data§ 4.1 The Fisher information spectrum · p. 8
The concentration of the classical Fisher information spectrum around zero is observed across all classical network configurations considered.
“This behaviour is observed across all classical network configurations that we consider.”
Quote in the paperSubstantial claim
- Findingown data§ 1 Introduction · p. 2
Well-designed quantum neural networks achieve faster training ability than comparable classical feedforward neural networks.
“We find that well-designed quantum neural networks are able to achieve a higher capacity and faster training ability than comparable classical feedforward neural networks.”
Quote in the paperSubstantial claim - Findingown data§ 2 Quantum neural networks · p. 3
The feature map adds substantial power to a model.
“which we find adds substantial power to a model (as seen in Section 4.2)”
Quote in the paperSubstantial claim - Findingreasoning§ B.5 Removing the rank constraint via discretisation · p. 18
For a statistical model satisfying (4), its discretised version, and a loss function that is α-Hölder continuous, there exists a dimensional constant c_d such that for γ ∈ (0,1] and all n, a generalisation bound holds (as given in Theorem B.5).
“Theorem B.5 (Generalisation bound for effective dimension without rank constraint) . Let Θ = [ -1 , 1] d and consider a statistical model M Θ := { p ( · , · ; θ ) : θ ∈ Θ } satisfying (4) . For κ ∈ N , let M ( κ ) Θ := { p ( κ ) ( · , · ; θ ) : θ ∈ Θ } be the discretised form as described above. Let d ( κ ) γ,n denote the effective dimension of M ( κ ) Θ as defined in (2) . Furthermore, let L : P(”
Quote in the paperSubstantial claim - Findingreasoning§ B.5 Removing the rank constraint via discretisation · p. 18
Under the assumption of Theorem B.5, there exists a dimensional constant c_d < ∞ such that for γ ∈ (0,1] and all n, the number of boxes of side length ε required to cover the parameter set Θ satisfies a bound (as given in Lemma B.6).
“Lemma B.6. Let Θ = [ -1 , 1] d , and let N ( κ ) ( ε ) denote the number of boxes of side length ε required to cover the parameter set Θ , the length being measured with respect to the metric ˆ F ( κ ) ij ( θ ) . Under the assumption of Theorem B.5, there exists a dimensional constant c d < ∞ such that for γ ∈ (0 , 1] and for all n ∈ N , we have”
Quote in the paperSubstantial claim - Findingown data§ C.2 The Fisher information spectra for varying model size · p. 19
The quantum neural network maintains a more uniform spectrum over increasing s_in and d.
“The quantum neural network, however, maintains a more uniform spectrum over increasing s in and d , showing promise in avoiding unfavourable qualities, such as barren plateaus.”
Quote in the paperSubstantial claim - Findingnone given§ B.5 Removing the rank constraint via discretisation · p. 17
With the discretised model definition, the Fisher information matrix F(κ)(θ) is constant inside each simplex Θl.
“Note that, with this definition, the Fisher information matrix of the discretised model F ( κ ) ( θ ) is constant inside each simplex Θ ℓ .”
Quote in the paperSubstantial claim - Findingown data§ 4.2 Capacity analysis · p. 9
The average Fisher-Rao norm over 100 trials is roughly 250% higher in the quantum neural network than in the classical neural network after training on a simple dataset for a fixed number of iterations.
“The average Fisher-Rao norm over 100 trials is roughly 250% higher in the quantum neural network than in the classical neural network, after training the models on a simple dataset for a fixed number of iterations (see Appendix C.3 for details).”
Quote in the paperSubstantial claim - Findingown data§ 4.2 Capacity analysis · p. 9
The classical model never achieves an effective dimension greater than or equal to the quantum models for the range of finite data considered.
“The classical model never achieves an effective dimension greater or equal to the quantum models for the range of finite data considered in this study.”
Quote in the paperSubstantial claim - Findingown data§ C.1 Sensitivity analysis for the effective dimension · p. 19
For networks with less trainable parameters, d, the results stabilise with as little as 40 data and parameter samples.
“For networks with less trainable parameters, d , the results stabilise with as little as 40 data and parameter samples.”
Quote in the paperNot a substantial claim - Findingreasoning§ 4.2 Capacity analysis · p. 9
The quantum neural network consistently achieves the highest effective dimension over all ranges of finite data considered.
“The quantum neural network consistently achieves the highest effective dimension over all ranges of finite data we consider.”
- Also stated in: § 4.2 Capacity analysis · p. 9 · plain
“Notably, the quantum neural network achieves the highest effective dimension over a wide range of data availability, followed by the easy quantum model.”
Quote in the paperSubstantial claim - Also stated in: § 4.2 Capacity analysis · p. 9 · plain
- Findingown data§ C.4 Training the quantum neural network on real hardware · p. 21
The real hardware shows remarkable performance relative to all other models.
“The results are contained in Figure 3b and the real hardware shows remarkable performance relative to all other models.”
Quote in the paperNot a substantial claim - Findingown data§ 4.3 Trainability · p. 10
The easy quantum model's Fisher information spectrum becomes more 'barren plateau-like', with eigenvalues becoming smaller as the number of qubits increases.
“This is not the case in the easy quantum model. The Fisher information spectrum becomes more 'barren plateau-like', with the eigenvalues becoming smaller as the number of qubits increase.”
Quote in the paperSubstantial claim - Findingown data§ C.2 The Fisher information spectra for varying model size · p. 19
In all scenarios, the classical model has a majority of its eigenvalues near or equal to zero, with a few very large eigenvalues.
“In all scenarios, the classical model has a majority of its eigenvalues near or equal to zero, with a few very large eigenvalues.”
Quote in the paperSubstantial claim - Findingreasoning§ B.5 Removing the rank constraint via discretisation · p. 17
By construction, the discretised model p(κ)(·,·;θ) is still M1-Lipschitz continuous.
“We note that, by construction, θ ↦→ p ( κ ) ( · , · ; θ ) is still M 1 -Lipschitz continuous.”
Quote in the paperSubstantial claim - Interpretationreasoning§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 7
A model suffering from a barren plateau will have a Fisher information spectrum with an increasing concentration of eigenvalues approaching zero as the number of qubits in the model increases.
“We can conclude that a model suffering from a barren plateau will have a Fisher information spectrum with an increasing concentration of eigenvalues approaching zero as the number of qubits in the model increase.”
Quote in the paperSubstantial claim - Premisecitation§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 6
The Fisher information spectrum for fully connected feedforward neural networks reveals that the parameter space is flat in most dimensions and strongly distorted in a few others.
“The Fisher information spectrum for fully connected feedforward neural networks reveals that the parameter space is flat in most dimensions, and strongly distorted in a few others [34].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [34] Bishop, C. Exact calculation of the Hessian matrix for the multilayer perceptron. Neural Comput. 4, 494–501 (1992). source
Not checked in the free run.
- Interpretationreasoning§ Abstract · p. 1
The faster training of quantum neural networks is due to their favourable optimisation landscapes, captured by a more evenly spread Fisher information spectrum.
“train faster than classical models due to their favourable optimisation landscapes, captured by a more evenly spread Fisher information spectrum.”
Quote in the paperSubstantial claim - Premisecitation§ 3.3 Generalisation error bounds · p. 6
Non-linear feedforward neural networks have particularly degenerate Fisher information matrices.
“Non-linear feedforward neural networks, which we consider in this study, have particularly degenerate Fisher information matrices [34].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [34] Bishop, C. Exact calculation of the Hessian matrix for the multilayer perceptron. Neural Comput. 4, 494–501 (1992). source
Not checked in the free run.
- Premisecitation§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 6
In the quantum realm, the negative effect of barren plateaus on training quantum neural networks has been linked to the Hessian matrix.
“In the quantum realm, the negative effect of barren plateaus on training quantum neural networks has been linked to the Hessian matrix [32].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [32] Skolik, A., McClean, J. R., Mohseni, M., van der Smagt, P. & Leib, M. Layerwise learning for quantum neural networks. Quant. Mach. Intell. 3, 5 (2021). source
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- Premisecitation§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 7
The barren plateau result tells us that Var θ [ ∂ ∂θ j R n ( θ )] ≤ ω S for models in a barren plateau.
“The barren plateau result also tells us that Var θ [ ∂ ∂θ j R n ( θ )] ≤ ω S for models in a barren plateau.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [23] Rissanen, J. J. Fisher information and stochastic complexity. IEEE Trans. Inf. Theory 42, 40–47 (1996). source
Not checked in the free run.
- Interpretationreasoning§ Abstract · p. 1
The effective dimension is a robust, bounded capacity measure useful for analysing the power of statistical models.
“The effective dimension, which depends on the Fisher information, is used to prove a novel generalisation bound and establish a robust measure of expressibility.”
- Also stated in: § 1 Introduction · p. 2 · plain
“We argue that the effective dimension is a robust capacity measure through proof of a novel generalisation bound with supporting numerical analyses”
- Also stated in: § 3.2 The effective dimension · p. 5 · plain
“the effective dimension can be interpreted as a bounded capacity measure that serves as a useful tool to analyse the power of statistical models.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The statistical model satisfies the regularity assumption (4).
- Also stated in: § 1 Introduction · p. 2 · plain
- Premisecitation§ 1 Introduction · p. 1
Generalisation bounds based on the VC dimension, and other measures alike, are typically vacuous because modern deep neural networks are heavily overparameterised.
“Since modern deep neural networks are heavily overparameterised, generalisation bounds based on the VC dimension, and other measures alike, are typically vacuous [17,18].”
Quote in the paperSubstantial claim0 of 2 sources checked- cites [17] Neyshabur, B., Bhojanapalli, S., McAllester, D. & Srebro, N. Exploring generalization in deep learning. In Advances in Neural Information Processing Systems 30, 5947–5956 (NIPS, 2017).
Not checked in the free run.
- cites [18] Arora, S., Ge, R., Neyshabur, B. & Zhang, Y. Stronger generalization bounds for deep nets via a compression approach. In Proc. 35th International Conference on Machine Learning Vol. 80, 254–263 (PMLR, 2018); http://proceedings.mlr.press/v80/arora18b.html
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- Interpretationreasoning§ 3.3 Generalisation error bounds · p. 5
For statistical models satisfying the regularity assumption, full-rank Fisher information matrix, and bounded gradient of log Fisher, and for Hölder continuous loss, there exists a constant such that the generalisation error is bounded by a term involving the effective dimension.
“Theorem 3.2 (Generalisation bound for the effective dimension) . Let Θ = [ -1 , 1] d and consider a statistical model M Θ := { p ( · , · ; θ ) : θ ∈ Θ } satisfying (4) such that the normalised Fisher information matrix ˆ F ( θ ) has full rank for all θ ∈ Θ , and ‖∇ θ log ˆ F ( θ ) ‖ ≤ Λ for some Λ ≥ 0 and all θ ∈ Θ .”
Quote in the paperSubstantial claim- The authors state this as an assumption: The statistical model satisfies the regularity assumption (4).
- Premisecitation§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 6
The entries of the Hessian vanish exponentially with the size of the system in models that are in a barren plateau.
“It was found that the entries of the Hessian vanish exponentially with the size of the system in models that are in a barren plateau.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [32] Skolik, A., McClean, J. R., Mohseni, M., van der Smagt, P. & Leib, M. Layerwise learning for quantum neural networks. Quant. Mach. Intell. 3, 5 (2021). source
Not checked in the free run.
- Premisecitation§ 1 Introduction · p. 1
A systematic study of the trade-offs between quantum and classical models has yet to be conducted.
“Whilst there has been much development in the growing field of quantum machine learning, a systematic study of the trade-offs between quantum and classical models has yet to be conducted [12].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [12] Aaronson, S. Read the fine print. Nat. Phys. 11, 291–293 (2015). source
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- Interpretationnone given§ 4 Numerical experiments and results · p. 7
Minimising the empirical risk with a log-likelihood loss function coincides with minimising the relative entropy between the distribution induced by applying the neural network to the observed input distribution and the observed output distribution.
“Minimising the empirical risk with a log-likelihood loss function coincides with the task of minimising the relative entropy D ( ·‖· ) between the distribution induced by applying the neural network to the observed input distribution r and the observed output distribution q .”
Quote in the paperNot a substantial claim - Interpretationreasoning§ 3.3 Generalisation error bounds · p. 6
The generalisation bound can be modified to hold for a statistical model without a full rank Fisher information matrix.
“The generalisation bound in (5) can be modified to hold for a statistical model without a full rank Fisher information matrix.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The statistical model satisfies the regularity assumption (4).
- Premisecitation§ 3.3 Generalisation error bounds · p. 6
The continuity assumptions of Theorem 3.2 are satisfied for a large class of classical and quantum statistical models, as well as many popular loss functions.
“The continuity assumptions of Theorem 3.2 are satisfied for a large class of classical and quantum statistical models [49, 50], as well as many popular loss functions.”
Quote in the paperSubstantial claim0 of 2 sources checked- cites [49] Marrero, C. O., Kieferová, M. & Wiebe, N. Entanglement induced barren plateaus. Preprint at https://arxiv.org/abs/2010.15968 (2020).
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- cites [50] Havlíček, V. et al. Supervised learning with quantum-enhanced feature spaces. Nature 567, 209–212 (2019). source
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- Premisecitation§ 1 Introduction · p. 1
Using the VC dimension to bound generalisation error requires several unrealistic assumptions, including that the model has access to infinite data.
“Further, using the VC dimension to bound generalisation error requires several unrealistic assumptions, including that the model has access to infinite data [15,16].”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [15] Sontag, E. D Neural Networks and Machine Learning 69–95 (Springer, 1998).
Not checked in the free run.
- cites [16] Vapnik, V., Levin, E. & Cun, Y. L. Measuring the VC-dimension of a learning machine. Neural Comput. 6, 851–876 (1994). source
Not checked in the free run.
- Premisecitation§ 3.3 Generalisation error bounds · p. 6
The full rank assumption on the Fisher information matrix often does not hold in classical models.
“The full rank assumption on the Fisher information matrix, however, often does not hold in classical models.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [34] Bishop, C. Exact calculation of the Hessian matrix for the multilayer perceptron. Neural Comput. 4, 494–501 (1992). source
Not checked in the free run.
- Premisecitation§ 1 Introduction · p. 2
For certain loss functions, the Fisher information matrix coincides with the Hessian of the loss function.
“For certain loss functions, the Fisher information matrix coincides with the Hessian of the loss function [33].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [33] Huembeli, P. & Dauphin, A. Characterizing the loss landscape of variational quantum circuits. Quant. Sci. Technol. 6, 025011 (2021). source
Not checked in the free run.
- Interpretationreasoning§ B.4 A geometric depiction of the effective dimension · p. 16
The effective dimension defined in (2) does not necessarily increase monotonically with the number of data, n.
“The effective dimension defined in (2) does not necessarily increase monotonically with the number of data, n .”
- Also stated in: § B.4 A geometric depiction of the effective dimension · p. 17 · plain
“Thus, the effective dimension does not necessarily increase monotonically with the number of data used.”
Quote in the paperNot a substantial claim - Also stated in: § B.4 A geometric depiction of the effective dimension · p. 17 · plain
- Premisecitation§ 5 Conclusion · p. 10
Classical neural networks are known to produce highly degenerate Fisher information matrices, which can significantly slow down training.
“Moreover, classical neural networks are known to produce highly degenerate Fisher information matrices, which can significantly slow down training.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [34] Bishop, C. Exact calculation of the Hessian matrix for the multilayer perceptron. Neural Comput. 4, 494–501 (1992). source
Not checked in the free run.
- Interpretationreasoning§ 4.2 Capacity analysis · p. 9
The quantum neural network's effective dimension converges faster than the classical and easy quantum models due to its more evenly spread Fisher information spectrum.
“It also converges much faster due to its more evenly spread Fisher information spectrum.”
Quote in the paperSubstantial claim - Interpretationreasoning§ 4.3 Trainability · p. 10
The feature map can influence the likelihood of experiencing a barren plateau.
“This highlights the importance of the feature map which can influence the likelihood of experiencing a barren plateau.”
- Also stated in: § 5 Conclusion · p. 10 · plain
“Changing the feature map, influences the Fisher spectrum and hence, alters the likelihood of encountering a barren plateau.”
Quote in the paperSubstantial claim - Also stated in: § 5 Conclusion · p. 10 · plain
- Interpretationown data§ 4.3 Trainability · p. 10
The higher order feature map used in the quantum neural network seems to structurally change the optimisation landscape and remove the flatness usually associated with barren plateaus or suboptimal optimisation conditions.
“The higher order feature map used in the quantum neural network seems to structurally change the optimisation landscape and remove the flatness, usually associated with barren plateaus or suboptimal optimisation conditions.”
Quote in the paperSubstantial claim - Interpretationreasoning§ B.5 Removing the rank constraint via discretisation · p. 19
Lemma B.2 remains valid for the discretised setting and under the assumption of Theorem B.5.
“We start be noting that Lemma B.2 remains valid for the discretised setting and under the assumption of Theorem B.5, 27 i.e.,”
Quote in the paperSubstantial claim - Interpretationown data§ C.2 The Fisher information spectra for varying model size · p. 19
The quantum neural network's more uniform spectrum shows promise in avoiding unfavourable qualities, such as barren plateaus.
“The quantum neural network, however, maintains a more uniform spectrum over increasing s in and d , showing promise in avoiding unfavourable qualities, such as barren plateaus.”
Quote in the paperSubstantial claim
- May combine two claims. 27
- Classified as probably not a substantial claim. 18
May combine two claims.
Findingown data§ 4.1 The Fisher information spectrum · p. 8The classical model's Fisher information spectrum is concentrated around zero, with the majority of eigenvalues negligible at order 10^-14 and a few very large eigenvalues.
“The classical model's Fisher information spectrum is concentrated around zero, where the majority of eigenvalues are negligible 17 , however, there are a few very large eigenvalues.”
- Also stated in: § 4.1 The Fisher information spectrum · p. 8 · plain
“Specifically, of the order 10 -14 , i.e., close to machine precision and thus, indistinguishable from zero.”
Quote in the paperSubstantial claim- Also stated in: § 4.1 The Fisher information spectrum · p. 8 · plain
May combine two claims.
Findingown data§ 4.2 Capacity analysis · p. 9On average, the classical model trains to a lower loss than the easy quantum model, but with significantly larger spread.
“Whilst on average, the classical model trains to a lower loss than the easy quantum model, the spread is significantly larger.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 4.2 Capacity analysis · p. 9The quantum neural network's training advantage persists on real quantum hardware, and its performance is even better than simulated results.
“We further verify the performance of the quantum neural network on real quantum hardware and train the model using the ibmq montreal 27-qubit device, where the training advantage persists.”
- Also stated in: § 4.2 Capacity analysis · p. 9 · plain
“We plot the hardware results till they stabilise, at roughly 33 training iterations and find the performance to be even better than the simulated results.”
Quote in the paperSubstantial claim- Also stated in: § 4.2 Capacity analysis · p. 9 · plain
May combine two claims.
Findingown data§ 4.3 Trainability · p. 10The quantum neural network trains to a lower loss, faster than the other two models over an average of 100 trials.
“Using a cross-entropy loss function, optimised with ADAM for a fixed number of training iterations = 100 and an initial learning rate = 0 . 1, the quantum neural network trains to a lower loss, faster than the other two models over an average of 100 trials.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown data§ C.1 Sensitivity analysis for the effective dimension · p. 19When higher dimensions are considered, the standard deviation around the results increases, but 100 data and parameter samples are still reasonable given that we consider a maximum of d = 100.
“When higher dimensions are considered, the standard deviation around the results increases, but 100 data and parameter samples are still reasonable given that we consider a maximum of d = 100.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 4.2 Capacity analysis · p. 9The quantum neural network maintains the lowest loss value on average across all three models, with the lowest spread over all training iterations.
“The quantum neural network maintains the lowest loss value on average across all three models, with the lowest spread over all training iterations.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ C.4 Training the quantum neural network on real hardware · p. 21The hardware training stops after roughly 33 training steps.
“This occurs after roughly 33 training steps.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingreasoning§ 4.2 Capacity analysis · p. 9The quantum neural network has a non-degenerate Fisher information matrix and its effective dimension converges to the maximum effective dimension d.
“The quantum neural network, on the other hand, has a non-degenerate Fisher information matrix and the effective dimension converges to the maximum effective dimension, d .”
Quote in the paperSubstantial claimMay combine two claims.
Findingown data§ C.2 The Fisher information spectra for varying model size · p. 19The easy quantum model has a somewhat uniform spectrum for a smaller input size, but this deteriorates as the input size (also equal to the number of qubits in this particular model) increases.
“The easy quantum model has a somewhat uniform spectrum for a smaller input size, but this deteriorates as the input size (also equal to the number of qubits in this particular model) increases.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown data§ C.3 Training the models using a simulator · p. 20The quantum neural network notably has the highest Fisher-Rao norm and lowest training loss on average.
“The quantum neural network notably has the highest Fisher-Rao norm and lowest training loss on average.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown data§ 4.1 The Fisher information spectrum · p. 8The easy quantum model has most of its eigenvalues close to zero, with some large eigenvalues whose magnitudes are not as extreme as the classical model.
“The easy quantum model also has most of its eigenvalues close to zero, and whilst there are some large eigenvalues, their magnitudes are not as extreme as the classical model.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown data§ 4.1 The Fisher information spectrum · p. 8The quantum neural network has a more uniform Fisher information spectrum, with no outlying values, and this distribution remains more or less constant as the number of qubits increases.
“The quantum neural network, on the other hand, has a different Fisher information spectrum. The distribution of eigenvalues is more uniform, with no outlying values and remains more or less constant as the number of qubits increase (see Appendix C.2).”
- Also stated in: § 4.1 The Fisher information spectrum · p. 8 · plain
“The distribution of eigenvalues is the most uniform in the quantum neural network, whereas the other models contain mostly small eigenvalues and larger condition numbers.”
Quote in the paperSubstantial claim- Also stated in: § 4.1 The Fisher information spectrum · p. 8 · plain
May combine two claims.
Findingown data§ B.3 Effective dimension converges to maximal rank of Fisher information matrix · p. 16The effective dimension correctly increases as the data becomes 'more random' and is thus able to accurately capture a model's generalisation behaviour.
“The effective dimension correctly increases as the data becomes 'more random' and is thus, able to accurately capture a model's generalisation behaviour.”
Quote in the paperSubstantial claimClassified as probably not a substantial claim.
Interpretationnone given§ 3.2 The effective dimension · p. 4The number of data observations determines a natural scale or resolution used to observe model space.
“The number of data observations determines a natural scale or resolution used to observe model space.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Interpretationreasoning§ 3.2 The effective dimension · p. 4The effective dimension's dependence on data availability helps understand how data availability influences the accurate capture of model complexity.
“This is beneficial for practical reasons where data is often limited, and can help in understanding how data availability influences the accurate capture of model complexity.”
Quote in the paperNot a substantial claimMay combine two claims.
Premisecitation§ 3.1 The Fisher information · p. 4The Fisher-Rao norm acts as an umbrella for several other existing norm-based measures and has demonstrated desirable properties both theoretically and empirically.
“Notably, the Fisher-Rao norm acts as an umbrella for several other existing norm-based measures [45-47] and has demonstrated desirable properties both theoretically, and empirically.”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [45] Neyshabur, B., Salakhutdinov, R. R. & Srebro, N. Path-SGD: path-normalized optimization in deep neural networks. In Advances in Neural Information Processing Systems 28, 2422–2430 (NIPS, 2015).
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- cites [46] Neyshabur, B., Tomioka, R. & Srebro, N. Norm-based capacity control in neural networks. In Proc. Machine Learning Research Vol. 40, 1376–1401 (PMLR, 2015); http://proceedings.mlr.press/v40/Neyshabur15.html
Not checked in the free run.
- cites [47] Bartlett, P. L., Foster, D. J. & Telgarsky, M. J. Spectrally-normalized margin bounds for neural networks. In Advances in Neural Information Processing Systems 30, 6240–6249 (NIPS, 2017); http://papers.nips.cc/paper/7204-spectrally-normalized
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May combine two claims.
Interpretationreasoning§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 6The loss landscape becomes increasingly flat as the size of the model increases, making optimisation more difficult.
“This implies that the loss landscape becomes increasingly flat as the size of the model increases, making optimisation more difficult.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premisecitation§ 4.1 The Fisher information spectrum · p. 8The Fisher information matrix of non-linear classical neural networks is known to be highly degenerate, with a few large eigenvalues.
“This is consistent with results from literature, where the Fisher information matrix of non-linear classical neural networks is known to be highly degenerate, with a few large eigenvalues [34].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [34] Bishop, C. Exact calculation of the Hessian matrix for the multilayer perceptron. Neural Comput. 4, 494–501 (1992). source
Not checked in the free run.
Classified as probably not a substantial claim.
Premisecitation§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 7From [23], we are in a barren plateau if, for parameters uniformly sampled from Θ, each element of the gradient of the loss function with respect to θ vanishes exponentially in the number of qubits S.
“From [23], we know that we are in a barren plateau if, for parameters θ uniformly sampled from Θ, each element of the gradient of the loss function with respect to θ vanishes exponentially in the number of qubits, S .”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [23] Rissanen, J. J. Fisher information and stochastic complexity. IEEE Trans. Inf. Theory 42, 40–47 (1996). source
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing).
Premisecitation§ 3.1 The Fisher information · p. 4The Fisher-Rao norm is a robust norm-based capacity measure.
“In [44], the authors leverage geometric invariances associated with the Fisher information, to produce the Fisher-Rao norm-a robust norm-based capacity measure”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [44] Liang, T., Poggio, T., Rakhlin, A. & Stokes, J. Fisher–Rao metric, geometry, and complexity of neural networks. In Proc. Machine Learning Research Vol. 89, 888–896 (PMLR, 2019); http://proceedings.mlr.press/v89/liang19a.html
Not checked in the free run.
May combine two claims.
Interpretationreasoning§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 7A model with a Fisher information spectrum that is not concentrated around zero, or whose eigenvalues do not vanish as the number of qubits grows, is unlikely to experience a barren plateau.
“Conversely, a model with a Fisher information spectrum that is not concentrated around zero is unlikely to experience a barren plateau.”
- Also stated in: § 5 Conclusion · p. 10 · hedged
“A model with eigenvalues of the Fisher information matrix that do not vanish as the number of qubits grow, is unlikely to suffer from a barren plateau.”
Quote in the paperSubstantial claim- Also stated in: § 5 Conclusion · p. 10 · hedged
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Premisecitation§ 1 Introduction · p. 2The Fisher information describes the geometry of a model's parameter space and is essential in both statistics and machine learning.
“a quantity that describes the geometry of a model's parameter space and is essential in both statistics and machine learning [20-22].”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [20] Du, Y., Hsieh, M.-H., Liu, T. & Tao, D. Expressive power of parametrized quantum circuits. Phys. Rev. Res. 2, 033125 (2020). source
Not checked in the free run.
- cites [21] Huang, H.-Y. et al. Power of data in quantum machine learning. Nat. Commun. 12, 2631 (2021). source
Not checked in the free run.
- cites [22] Berezniuk, O., Figalli, A., Ghigliazza, R. & Musaelian, K. A scale-dependent notion of effective dimension. Preprint at https://arxiv.org/abs/2001.10872 (2020).
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Premisecitation§ 1 Introduction · p. 2Often, quantum neural networks suffer from a barren plateau phenomenon, wherein the loss landscape is perilously flat, and consequently, parameter optimisation is extremely difficult.
“Often, quantum neural networks suffer from a barren plateau phenomenon, wherein the loss landscape is perilously flat, and consequently, parameter optimisation is extremely difficult [23].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [23] Rissanen, J. J. Fisher information and stochastic complexity. IEEE Trans. Inf. Theory 42, 40–47 (1996). source
Not checked in the free run.
Probably not a substantial claim: may not pass S3 (load-bearing).
Interpretationnone given§ 3.3 Generalisation error bounds · p. 6The effective dimension does not necessarily increase monotonically with n.
“it is worthwhile to note that the effective dimension does not necessarily increase monotonically with n”
Quote in the paperNot a substantial claimMay combine two claims.
Premisecitation§ 3.4 The Fisher spectrum and the barren plateau phenomenon · p. 6These types of spectra slow down a model's training and may render optimisation suboptimal.
“These types of spectra are known to slow down a model's training and may render optimisation suboptimal [31].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [31] Volkoff, T. & Coles, P. J. Large gradients via correlation in random parameterized quantum circuits. Quant. Sci. Technol. 6, 025008 (2021). source
Not checked in the free run.
Classified as probably not a substantial claim.
Premisecitation§ 1 Introduction · p. 2The effective dimension depends on the Fisher information.
“measures such as the effective dimension have been motivated from an information-theoretic standpoint and depend on the Fisher information”
Quote in the paperSubstantial claim0 of 3 sources checked- cites [20] Du, Y., Hsieh, M.-H., Liu, T. & Tao, D. Expressive power of parametrized quantum circuits. Phys. Rev. Res. 2, 033125 (2020). source
Not checked in the free run.
- cites [21] Huang, H.-Y. et al. Power of data in quantum machine learning. Nat. Commun. 12, 2631 (2021). source
Not checked in the free run.
- cites [22] Berezniuk, O., Figalli, A., Ghigliazza, R. & Musaelian, K. A scale-dependent notion of effective dimension. Preprint at https://arxiv.org/abs/2001.10872 (2020).
Not checked in the free run.
May combine two claims.
Interpretationown data§ 5 Conclusion · p. 11Overall, quantum neural networks can possess a desirable Fisher information spectrum that enables them to train faster and express more functions than comparable classical and quantum models.
“Overall, we have shown that quantum neural networks can possess a desirable Fisher information spectrum that enables them to train faster and express more functions than comparable classical and quantum models-a promising reveal for quantum machine learning, which we hope leads to further studies on the power of quantum models.”
Quote in the paperSubstantial claimMay combine two claims.
Interpretationreasoning§ 4.2 Capacity analysis · p. 9The effective dimension converges slowest for classical models, followed by the easy quantum model, because classical models contain highly degenerate Fisher information matrices.
“Since the classical models contain highly degenerate Fisher information matrices, the effective dimension converges the slowest, followed by the easy quantum model.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductown data§ 4.1 The Fisher information spectrum · p. 8A sensitivity analysis verifies that 100 parameter samples are reasonable for the models considered.
“A sensitivity analysis is included in Appendix C.1 to verify that 100 parameter samples are reasonable for the models we consider.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductnone given§ B.4 A geometric depiction of the effective dimension · p. 16In all experiments conducted in this study, the effective dimension is examined over a wide range of n to ensure it is sufficient in accurately estimating the size of a model.
“In all experiments conducted in this study, we examine the effective dimension over a wide range of n , to ensure it is sufficient in accurately estimating the size of a model.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Interpretationnone given§ 4.2 Capacity analysis · p. 9In the limit n→∞, all models converge to an effective dimension equal to the maximum rank of the Fisher information matrix.
“In the limit n →∞ , all models will converge to an effective dimension equal to the maximum rank of the Fisher information matrix.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premisecitation§ 4.3 Trainability · p. 10The observed classical Fisher information spectrum is known to have undesirable optimisation properties where outlying eigenvalues slow down training and loss convergence.
“Classically, the observed Fisher information spectrum is known to have undesirable optimisation properties where the outlying eigenvalues slow down training and loss convergence [31].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [31] Volkoff, T. & Coles, P. J. Large gradients via correlation in random parameterized quantum circuits. Quant. Sci. Technol. 6, 025008 (2021). source
Not checked in the free run.
May combine two claims.
Interpretationreasoning§ C.1 Sensitivity analysis for the effective dimension · p. 19The capacity results will be sensitive to the number of data samples used in estimating the Fisher information matrix for a given θ, and to the number of θ samples then used to calculate the effective dimension.
“The capacity results will, thus, be sensitive to the number of data samples used in estimating the Fisher information matrix for a given θ , and to the number of θ samples then used to calculate the effective dimension.”
Quote in the paperNot a substantial claimMay combine two claims.
Interpretationreasoning§ 5 Conclusion · p. 10The quantum neural network with a hard feature map is an example of a model showing resilience to barren plateaus with good trainability, supported by results from real quantum hardware.
“The quantum neural network with a hard feature map is an example of such a model showing resilience to this phenomenon with good trainability, supported by results from real quantum hardware.”
Quote in the paperSubstantial claim- Rests on an assumption: The feature map used in the quantum neural network is hard to simulate classically.
May combine two claims.
Interpretationown data§ 5 Conclusion · p. 10A particular quantum neural network offers advantages from both a capacity and trainability perspective, captured by a high effective dimension and a non-degenerate Fisher information matrix.
“A particular quantum neural network offers advantages from both a capacity and trainability perspective. These advantages are captured by a high effective dimension and a non-degenerate Fisher information matrix.”
Quote in the paperSubstantial claim- Rests on an assumption: The feature map used in the quantum neural network is hard to simulate classically.
May combine two claims.
Interpretationown data§ 4.3 Trainability · p. 10The quantum neural network shows resilience against barren plateaus because its Fisher information eigenvalue distribution remains more or less constant and many eigenvalues are not near zero as system size increases.
“Upon examining the quantum neural network over an increasing system size (see Appendix C.2), the eigenvalue distribution of the Fisher information matrix remains more or less constant, and a large amount of the eigenvalues are not near zero, thus, the model shows resilience against barren plateaus.”
Quote in the paperSubstantial claimMay combine two claims.
Interpretationown data§ 5 Conclusion · p. 10The effective dimension is a robust capacity measure for quantum and classical models, justified through proof of a novel generalisation bound.
“In this study, the effective dimension is presented as a robust capacity measure for quantum and classical models, which we justify through proof of a novel generalisation bound.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing). May combine two claims.
Study design and conductreasoning§ C.4 Training the quantum neural network on real hardware · p. 21Due to limited hardware availability, this experiment is only run once and an analysis of the hardware noise and the spread of the training loss for differently sampled initial parameters would make these results more robust.
“Due to limited hardware availability, this experiment is only run once and an analysis of the hardware noise and the spread of the training loss for differently sampled initial parameters would make these results more robust.”
Quote in the paperNot a substantial claimMay combine two claims.
Interpretationreasoning§ B.5 Removing the rank constraint via discretisation · p. 19If the model M Θ satisfies an additional regularity assumption ‖∇θ F(θ)‖ ≤ Λ for some Λ ≥ 0 and all θ ∈ Θ, then choosing the discretisation parameter κ ≫ Λ ensures that M Θ ≈ M (κ) Θ and F(θ) ≈ F (κ)(θ); furthermore, √n ≫ κ is required to ensure that the balls used to cover each simplex of the triangulation are smaller than the size of each simplex.
“Remark B.7 (How to choose the discretisation parameter κ ) . In this remark we discuss conditions such that the generalisation bound of Theorem B.5 for the discretised model M ( k ) Θ is a good approximation to a generalisation bound of the original model M Θ . Assume that the model M Θ satisfies an additional regularity assumption of the form ‖∇ θ ˆ F ( θ ) ‖ ≤ Λ for some Λ ≥ 0 and for all θ ∈ Θ,”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S4 (based).
Premisenone given§ B.5 Removing the rank constraint via discretisation · p. 17The bound ||∇θ log F|| ≤ Λ forces the Fisher information matrix to have constant rank.
“Indeed, this is a rather strong bound as it forces ˆ F to have constant rank, so it is desirable to find a variant of Lemmas B.1 and B.2 that do not require such an assumption.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationreasoning§ 5 Conclusion · p. 10Replacing the quantum neural network's feature map with one that is easily simulable impairs these advantages.
“The feature map in the quantum neural network is conjectured to be hard to simulate classically, and replacing it with one that is easily simulable, impairs these advantages.”
Quote in the paperNot a substantial claim- Rests on an assumption: The feature map used in the quantum neural network is hard to simulate classically.
Probably not a substantial claim: may not pass S3 (load-bearing).
Interpretationreasoning§ C.1 Sensitivity analysis for the effective dimension · p. 19For higher d, it is likely that more samples will be needed.
“For higher d , it is likely that more samples will be needed.”
Quote in the paperNot a substantial claim
The authors state this as an assumption.
The statistical model satisfies the regularity assumption (4).
“We assume the following regularity assumption on the model M Θ := { p ( · , · ; θ ) : θ ∈ Θ } :”
The paper relies on this without support.
The feature map used in the quantum neural network is hard to simulate classically.
“The feature map in the quantum neural network is conjectured to be hard to simulate classically”
“The quantum neural network's encoding scheme is conjectured to be difficult.”
The paper relies on this without support.
The capacity of quantum neural networks is not well explored, and no such Fisher information analysis has been done for them.
“In stark contrast to classical models, understanding the capacity of quantum neural networks is not well explored.”
“For quantum neural networks, no such analysis has been done.”
The authors state this as an assumption.
The loss function in Theorem 3.2 is bounded.
“the assumption that the loss function in Theorem 3.2 has to be bounded.”
The paper relies on this without support.
The relative entropy is α-Hölder continuous in its first argument for α∈(0,1) and log-Lipschitz continuous in its first argument.
“We further note that the relative entropy is α -H¨ older continuous in the first argument for α ∈ (0 , 1). In fact, the relative entropy is even log-Lipschitz continuous in the first argument”
The paper relies on this without support.
In practical applications, the Fisher matrix is evaluated at finitely many points.
“Our approach to this general problem is based on the idea that, in practical applications, the Fisher matrix is evaluated at finitely many points, so it makes sense to approximate a statistical model with a discretised one where the corresponding Fisher information matrix is piecewise constant.”
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?
QNNs exploit quantum superposition and entanglement to process information in ways classical networks cannot, potentially accelerating training times and improving performance on complex data sets.
“Quantum neural networks (QNNs), for instance, exploit quantum superposition and entanglement to process information in ways that classical networks cannot, potentially accelerating training times and improving performance on complex data sets [18].”
From Quantum-Trained Convolutional Neural Network for Deepfake Audio Detection (2025) · cites this paper as [18]
The Introduction (p. 1) says QNNs use superposition and entanglement and describes potential training speed-ups; the Trainability section (p. 10) reports faster training than the classical models tested. But the Introduction says whether QNNs are more powerful than classical networks remains open. The paper does not establish that classical networks cannot process information in those ways or that QNNs improve performance on complex datasets. (LLM, conf=0.87)
Experimental — accuracy not yet measuredVariational approaches have made strides in evaluating or compressing quantum system evolutions.
“there have been a number of strides in evaluating or compressing these evolutions using variational approaches [90, 91].”
From Variational quantum algorithms (2021) · cites this paper as [90]
Section 2 (pp. 2–3) describes variational quantum neural networks and the evolution of an encoded state through a variational circuit. It does not report strides in evaluating or compressing quantum-system evolutions; searches for evolution evaluation and compression found no passage addressing that claim. (LLM, conf=0.75)
Experimental — accuracy not yet measuredVariational methods can be applied incrementally by stepping the electronic wavefunction forward with time-dependent variational principles and sampling forces to move nuclei classically, resulting in Born-Oppenheimer type molecular dynamics.
“Variational methods can be applied incrementally in these cases, by stepping the electronic wavefunction forward with time-dependent variational principles [90, 91] and sampling the forces [260] to move the nuclei classically, resulting in a Born-Oppenheimer type molecular dynamics.”
From Variational quantum algorithms (2021) · cites this paper as [90]
Split into 2 atoms — 0 confirmed, 0 partially supported, 0 disputed, 0 misattributed, 2 unverifiable. Expand the claim to see per-atom verdicts.
Experimental — accuracy not yet measuredQuantum neural networks can be more expressive-even exponentially for specific architectures-than classical counterparts.
“For a given number of neurons, quantum neural networks can be more expressiveeven exponentially, for specific network architectures -than their classical counterpart.[225][226][227]”
From Quantum Computing for Molecular Biology** (2023) · cites this paper as [227]
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.
Conflicting specifications of the easy quantum model's feature map
MinorSection 2 specifies RY-gate angle encoding for the easy quantum model, whereas Appendix A specifies an unrepeated layer of Hadamard and RZ gates. These are different gate sequences for the same feature map.
“We use a straightforward angle encoding scheme, where data points are encoded via RY-gates on each qubit without entangling them, with rotations equal to feature values normalised to [ -1 , 1].”
“The classically simulable feature map employed in the easy quantum model, is simply the first sets of Hadamard and RZgates, as done in Figure 4 and is not repeated.”
Specified RZZ-gate indices extend beyond the circuit's qubits
MinorThe feature map has S qubits, but the stated ranges permit j = S and any i ≥ 1, placing a gate on qubit i + S, beyond qubit S. This conflicts with the description of gates between pairs of the circuit's qubits.
“Then, RZZ-gates are implemented on qubits i, i + j for i ∈ [1 , . . . , S -1] and j ∈ [ i +1 , . . . , S ]”
“Figure 4 contains a circuit representation of the feature map developed in [39] and used in this study in the quantum neural network model. First, the feature map applies Hadamard gates on each of the S := s in qubits”
Cites
The Nature of Statistical Learning Theory
Vapnik, V. (2000) · Statistics for Engineering and Information Science · doi:10.1007/978-1-4757-3264-1 · Cited by 46,387 · see citing works
Elements of Information Theory
Cover, T. M., & Thomas, J. A. (2005) · doi:10.1002/047174882x · Cited by 13,791 · see citing works
Scikit-learn: Machine Learning in Python
(2011) · Journal of Machine Learning Research · doi:10.5555/1953048.2078195 · Cited by 8,539 · see citing works
Natural Gradient Works Efficiently in Learning
Амари, Ш.-И. (1998) · Neural Computation · doi:10.1162/089976698300017746 · Cited by 2,745 · 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
On the Uniform Convergence of Relative Frequencies of Events to Their Probabilities
Vapnik, V. N., & Chervonenkis, A. Y. (1971) · Theory of Probability & Its Applications · doi:10.1137/1116025 · Cited by 2,448 · see citing works
Advances in Neural Information Processing Systems 27 (NIPS 2014)
Zhong, M., Goddard, N., & Sutton, C. A. (2014) · 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
Neural Networks: Tricks of the Trade: Second Edition
(2012) · Lecture Notes in Computer Science · doi:10.1007/978-3-642-35289-8 · Cited by 2,116 · 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
Qiskit: An Open-source Framework for Quantum Computing
Aleksandrowicz, G., Alexander, T., Barkoutsos, P. K., Bello, L., Ben-Haim, Y., Bucher, D., Cabrera-Hernández, F. J., Carballo-Franquis, J., Chen, A., Chen, C.-F., et al. (2019) · Zenodo (CERN European Organization for Nuclear Research) · doi:10.5281/zenodo.2562110 · Cited by 1,454 · see citing works
Self-citationLeCun, Y., Bottou, L., Orr, G., & Müller, K. (2012) · Lecture notes in computer science · doi:10.1007/978-3-642-35289-8_3 · Cited by 1,268 · 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
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
Sim, S., Johnson, P. D., & Aspuru‐Guzik, A. (2019) · Advanced Quantum Technologies · doi:10.1002/qute.201900070 · Cited by 972 · see citing works
Power of data in quantum machine learning
Huang, H.-Y., Broughton, M., Mohseni, M., Babbush, R., Boixo, S., Neven, H., & McClean, J. R. (2021) · Nature Communications · doi:10.1038/s41467-021-22539-9 · Cited by 896 · see citing works
Fisher information and stochastic complexity
Rissanen, J. J. (1996) · IEEE Transactions on Information Theory · doi:10.1109/18.481776 · Cited by 814 · see citing works
Noise-induced barren plateaus in variational quantum algorithms
Wang, S., Fontana, E., Cerezo, M., Sharma, K., Sone, A., Cincio, L., & Coles, P. J. (2021) · Nature Communications · doi:10.1038/s41467-021-27045-6 · Cited by 773 · 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
Supervised Learning with Quantum Computers
Schuld, M., & Petruccione, F. (2018) · Quantum Science and Technology · doi:10.1007/978-3-319-96424-9 · Cited by 730 · see citing works
The quest for a Quantum Neural Network
Schuld, M., Sinayskiy, I., & Petruccione, F. (2014) · Quantum Information Processing · doi:10.1007/s11128-014-0809-8 · Cited by 671 · see citing works
Science from Fisher Information
Frieden, B. R. (2004) · Cambridge University Press eBooks · doi:10.1017/cbo9780511616907 · Cited by 586 · see citing works
Connecting Ansatz Expressibility to Gradient Magnitudes and Barren Plateaus
Holmes, Z., Sharma, K., Cerezo, M., & Coles, P. J. (2022) · PRX Quantum · doi:10.1103/prxquantum.3.010313 · Cited by 570 · see citing works
Aaronson, S. (2015) · Nature Physics · doi:10.1038/nphys3272 · Cited by 567 · see citing works
Quantum autoencoders for efficient compression of quantum data
Romero, J., Olson, J. P., & Aspuru-Guzik, A. (2017) · Quantum Science and Technology · doi:10.1088/2058-9565/aa8072 · Cited by 559 · see citing works
Quantum machine learning: a classical perspective
Ciliberto, C., Herbster, M., Ialongo, A. D., Pontil, M., Rocchetto, A., Severini, S., & Wossnig, L. (2018) · Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences · doi:10.1098/rspa.2017.0551 · Cited by 518 · 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
Self-citationContinuous-variable quantum neural networks
Killoran, N., Bromley, T. R., Arrazola, J. M., Schuld, M., Quesada, N., & Lloyd, S. (2019) · Physical Review Research · doi:10.1103/physrevresearch.1.033063 · Cited by 418 · see citing works
Measuring the VC-Dimension of a Learning Machine
Vapnik, V., Levin, E., & Cun, Y. L. (1994) · Neural Computation · doi:10.1162/neco.1994.6.5.851 · Cited by 388 · see citing works
Stronger generalization bounds for deep nets via a compression approachPreprint
Arora, S., Ge, R., Neyshabur, B., & Zhang, Y. (2018) · arXiv (Cornell University) · doi:10.48550/arxiv.1802.05296 · Cited by 359 · 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
Expressive power of parametrized quantum circuits
Du, Y., Hsieh, M.-H., Liu, T., & Tao, D. (2020) · Physical Review Research · doi:10.1103/physrevresearch.2.033125 · Cited by 318 · see citing works
Finite-Dimensional Vector Spaces
Halmos, P. R. (1974) · Undergraduate texts in mathematics · doi:10.1007/978-1-4612-6387-6 · Cited by 287 · see citing works
Soundness and completeness of quantum root-mean-square errors
Ozawa, M. (2018) · npj Quantum Information · doi:10.1038/s41534-018-0113-z · Cited by 266 · see citing works
Dziugaite, G. K., & Roy, D. M. (2017) · arXiv (Cornell University) · doi:10.48550/arxiv.1703.11008 · 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
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 embeddings for machine learning
Lloyd, S., Schuld, M., Ijaz, A., Izaac, J., & Killoran, N. (2020) · arXiv · doi:10.48550/arxiv.2001.03622 · Cited by 198 · see citing works
Exact Calculation of the Hessian Matrix for the Multilayer Perceptron
Bishop, C. (1992) · Neural Computation · doi:10.1162/neco.1992.4.4.494 · Cited by 146 · see citing works
Large gradients via correlation in random parameterized quantum circuits
Volkoff, T., & Coles, P. J. (2021) · Quantum Science and Technology · doi:10.1088/2058-9565/abd891 · Cited by 143 · see citing works
Learning to learn with quantum neural networks via classical neural networksPreprint
Verdon, G., Broughton, M., McClean, J. R., Sung, K. J., Babbush, R., Zhang, J., Neven, H., & Mohseni, M. (2019) · arXiv (Cornell University) · doi:10.48550/arxiv.1907.05415 · Cited by 134 · 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
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
The capacity of feedforward neural networks
Baldi, P., & Vershynin, R. (2019) · Neural Networks · doi:10.1016/j.neunet.2019.04.009 · Cited by 79 · see citing works
Characterizing the loss landscape of variational quantum circuits
Huembeli, P., & Dauphin, A. (2021) · Quantum Science and Technology · doi:10.1088/2058-9565/abdbc9 · Cited by 71 · see citing works
Introduction: Four Periods in the Research of the Learning Problem
Vapnik, V. N. (2000) · Springer eBooks · doi:10.1007/978-1-4757-3264-1_1 · Cited by 60 · see citing works
The Capacity of Quantum Neural Networks
Wright, L. G., & McMahon, P. L. (2020) · Conference on Lasers and Electro-Optics · doi:10.1364/cleo_at.2020.jm4g.5 · Cited by 35 · see citing works
Approximate Fisher Information Matrix to Characterize the Training of Deep Neural Networks
Liao, Z., Drummond, T. W., Reid, I. D., et al. (2018) · IEEE Transactions on Pattern Analysis and Machine Intelligence · doi:10.1109/tpami.2018.2876413 · Cited by 26 · see citing works
A scale-dependent notion of effective dimensionPreprint
Berezniuk, O., Figalli, A., Ghigliazza, R. M., et al. (2020) · arXiv (Cornell University) · doi:10.48550/arxiv.2001.10872 · Cited by 7 · see citing works
Self-citationInformation-Theoretic Local Minima Characterization and RegularizationPreprint
Jia, Z., & Su, H. (2019) · arXiv (Cornell University) · doi:10.48550/arxiv.1911.08192 · Cited by 4 · see citing works
amyami187/effective_dimension: First release of the effective dimension code
Abbas, A. (2021) · Zenodo (CERN European Organization for Nuclear Research) · doi:10.5281/zenodo.4732830 · Cited by 1 · see citing works
Self-citationamyami187/effective_dimension:
Abbas, A. (2021) · Zenodo (CERN European Organization for Nuclear Research) · doi:10.5281/zenodo.4732829 · Cited by 1 · see citing works
Self-citation
Flagged first, then by citations
Research works printed but not linked: 13
- Goodfellow, I., Bengio, Y. & Courville, A. Deep Learning (MIT Press, 2016); http://www.deeplearningbook.org
- Farhi, E. & Neven, H. Classification with quantum neural networks on near term processors. Quant. Rev. Lett. 1, 2 (2020).
- Sontag, E. D Neural Networks and Machine Learning 69–95 (Springer, 1998).
- Neyshabur, B., Bhojanapalli, S., McAllester, D. & Srebro, N. Exploring generalization in deep learning. In Advances in Neural Information Processing Systems 30, 5947–5956 (NIPS, 2017).
- Kunstner, F., Hennig, P. & Balles, L. Limitations of the empirical Fisher approximation for natural gradient descent. In Advances in Neural Information Processing Systems 32 4156–4167 (NIPS, 2019); http://papers.nips.cc/paper/limitations-of-fisher-approximation
- Karakida, R., Akaho, S. & Amari, S.-I. Universal statistics of Fisher information in deep neural networks: mean field approach. In Proc. Machine Learning Research Vol. 89, 1032–1041 (PMLR, 2019); http://proceedings.mlr.press/v89/karakida19a.html
- Liang, T., Poggio, T., Rakhlin, A. & Stokes, J. Fisher–Rao metric, geometry, and complexity of neural networks. In Proc. Machine Learning Research Vol. 89, 888–896 (PMLR, 2019); http://proceedings.mlr.press/v89/liang19a.html
- Neyshabur, B., Salakhutdinov, R. R. & Srebro, N. Path-SGD: path-normalized optimization in deep neural networks. In Advances in Neural Information Processing Systems 28, 2422–2430 (NIPS, 2015).
- Neyshabur, B., Tomioka, R. & Srebro, N. Norm-based capacity control in neural networks. In Proc. Machine Learning Research Vol. 40, 1376–1401 (PMLR, 2015); http://proceedings.mlr.press/v40/Neyshabur15.html
- Bartlett, P. L., Foster, D. J. & Telgarsky, M. J. Spectrally-normalized margin bounds for neural networks. In Advances in Neural Information Processing Systems 30, 6240–6249 (NIPS, 2017); http://papers.nips.cc/paper/7204-spectrally-normalized
- Rissanen, J. J. Fisher information and stochastic complexity. IEEE Trans. Inf. Theory 42, 40–47 (1996). · DOI · Paper page
- Marrero, C. O., Kieferová, M. & Wiebe, N. Entanglement induced barren plateaus. Preprint at https://arxiv.org/abs/2010.15968 (2020). · arXiv
- Virmaux, A. & Scaman, K. Lipschitz regularity of deep neural networks: analysis and efficient estimation. In Advances in Neural Information Processing Systems 31, 3835–3844 (NIPS, 2018); http://papers.nips.cc/paper/lipschitz-regularity-of-deep-neural-networks
Cited by
Sorted by citations
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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
“For instance, it has been shown that quantum neural networks can achieve a significantly better effective dimension than comparable classical neural networks [258].”
BackgroundNoisy intermediate-scale quantum algorithms
Bharti, K., Cervera-Lierta, A., Kyaw, T. H., Haug, T., Alperin-Lea, S., Anand, A., Degroote, M., Heimonen, H., Kottmann, J. S., Menke, T., et al. (2022) · Reviews of Modern Physics · doi:10.1103/revmodphys.94.015004 · Cited by 1,726 · see citing works
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Tilly, J., Chen, H., Cao, S., Picozzi, D., Setia, K., Li, Y., Grant, E., Wossnig, L., Rungger, I., Booth, G. H., et al. (2022) · Physics Reports · doi:10.1016/j.physrep.2022.08.003 · Cited by 1,031 · see citing works
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Quantum Computing for Molecular Biology**
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Ranga, D., Rana, A., Prajapat, S., Kumar, P., Kumar, K., & Vasilakos, A. V. (2024) · Mathematics · doi:10.3390/math12213318 · Cited by 101 · see citing works
Chow, J. C. L. (2024) · Medical Sciences · doi:10.3390/medsci12040067 · Cited by 101 · see citing works
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Pal, S., Bhattacharya, M., Lee, S.-S., & Chakraborty, C. (2024) · Molecular Biotechnology · doi:10.1007/s12033-023-00765-4 · Cited by 84 · see citing works
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Rozenman, G. G., Kundu, N. K., Liu, R., Zhang, L., Maslennikov, A., Reches, Y., & Youm, H. Y. (2023) · IET Quantum Communication · doi:10.1049/qtc2.12069 · Cited by 84 · see citing works
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Self-citationHybrid quantum-classical-quantum convolutional neural networks
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Quantum Machine Learning for Finance ICCAD Special Session Paper
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Tüysüz, C., Rieger, C., Novotny, K., Demirköz, B. M., Dobos, D., Potamianos, K. J., Vallecorsa, S., Vlimant, J.-R., & Forster, R. (2021) · Quantum Machine Intelligence · doi:10.1007/s42484-021-00055-9 · Cited by 56 · see citing works
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Dritsas, E., & Τρίγκα, Μ. (2025) · Machine Learning and Knowledge Extraction · doi:10.3390/make7010013 · Cited by 62 · see citing works
Analytic Theory for the Dynamics of Wide Quantum Neural Networks
Liu, J., Najafi, K., Sharma, K., Tacchino, F., Jiang, L., & Mezzacapo, A. (2023) · Physical Review Letters · doi:10.1103/physrevlett.130.150601 · Cited by 53 · see citing works
Oncological Applications of Quantum Machine Learning
Rahimi, M., & Asadi, F. (2023) · Technology in Cancer Research & Treatment · doi:10.1177/15330338231215214 · Cited by 56 · see citing works
Quantum-Classical Hybrid Machine Learning for Image Classification (ICCAD Special Session Paper)
Alam, M., Kundu, S., Topaloglu, R. O., & Ghosh, S. (2021) · International Conference on Computer Aided Design · doi:10.1109/iccad51958.2021.9643516 · Cited by 57 · see citing works
Quantum Neural Network Classifiers: A Tutorial
Li, W., Lu, Z., & Deng, D.-L. (2022) · SciPost Physics Lecture Notes · doi:10.21468/scipostphyslectnotes.61 · Cited by 52 · see citing works
Quantum kernel methods for solving regression problems and differential equations
Paine, A. E., Elfving, V. E., & Kyriienko, O. (2023) · Physical Review A · doi:10.1103/physreva.107.032428 · Cited by 52 · see citing works
Quantum Machine Learning for Next-G Wireless Communications: Fundamentals and the Path Ahead
Narottama, B., Mohamed, Z., & Aı̈ssa, S. (2023) · IEEE Open Journal of the Communications Society · doi:10.1109/ojcoms.2023.3309268 · Cited by 52 · see citing works
Graph neural network initialisation of quantum approximate optimisation
Jain, N., Coyle, B., Kashefi, E., & Kumar, N. (2022) · Quantum · doi:10.22331/q-2022-11-17-861 · Cited by 50 · see citing works
Quantum phase detection generalization from marginal quantum neural network models
Monaco, S., Kiss, O., Mandarino, A., Vallecorsa, S., & Grossi, M. (2023) · Physical review. B./Physical review. B · doi:10.1103/physrevb.107.l081105 · Cited by 46 · see citing works
Deep quantum neural networks on a superconducting processor
Pan, X., Lu, Z., Wang, W., Hua, Z., Xu, Y., Li, W., Cai, W., Li, X., Wang, H., Song, Y., et al. (2023) · Nature Communications · doi:10.1038/s41467-023-39785-8 · Cited by 49 · see citing works
Practical advantage of quantum machine learning in ghost imaging
Xiao, T., Zhai, X., Wu, X., Jianping Fan, B., & Zeng, G. (2023) · Communications Physics · doi:10.1038/s42005-023-01290-1 · Cited by 47 · see citing works
Variational Inference with a Quantum Computer
Benedetti, M., Coyle, B., Fiorentini, M., Lubasch, M., & Rosenkranz, M. (2021) · Physical Review Applied · doi:10.1103/physrevapplied.16.044057 · Cited by 49 · see citing works
The Dilemma of Quantum Neural Networks
Yang, Q., Wang, X., Du, Y., Wu, X., & Tao, D. (2022) · IEEE Transactions on Neural Networks and Learning Systems · doi:10.1109/tnnls.2022.3208313 · Cited by 49 · see citing works
EQNAS: Evolutionary Quantum Neural Architecture Search for Image Classification
Li, Y., Liu, R., Hao, X., Shang, R., Zhao, P., & Jiao, L. (2023) · Neural Networks · doi:10.1016/j.neunet.2023.09.040 · Cited by 45 · see citing works
Dynamical simulation via quantum machine learning with provable generalization
Gibbs, J., Holmes, Z., Caro, M. C., Ezzell, N., Huang, H.-Y., Cincio, Ł., Sornborger, A. T., & Coles, P. J. (2024) · Physical Review Research · doi:10.1103/physrevresearch.6.013241 · Cited by 48 · see citing works
Federated quantum long short-term memory (FedQLSTM)
Chehimi, M. M., Chen, S. Y.-C., Saad, W., & Yoo, S. (2024) · Quantum Machine Intelligence · doi:10.1007/s42484-024-00174-z · Cited by 45 · see citing works
Benchmarking Simulated and Physical Quantum Processing Units Using Quantum and Hybrid Algorithms
Kordzanganeh, M., Buchberger, M., Kyriacou, B., Povolotskii, M., Fischer, W., Kurkin, A., Somogyi, W., Sagingalieva, A., Pflitsch, M., & Melnikov, A. A. (2023) · Advanced Quantum Technologies · doi:10.1002/qute.202300043 · Cited by 43 · see citing works
Federated Quantum Machine Learning with Differential Privacy
Rofougaran, R., Yoo, S., Tseng, H.-H., & Chen, S. Y.-C. (2024) · IEEE International Conference on Acoustics Speech and Signal Processing · doi:10.1109/icassp48485.2024.10447155 · Cited by 45 · see citing works
- Authors
- Abbas, A., Sutter, D., Zoufal, C., Lucchi, A., Figalli, A., & Woerner, S.
- Affiliations
- IBM Research - Zurich (CH)
- ETH Zurich (CH)
- Corresponding author
- Woerner, Stefan
- Venue
- Nature Computational Science
- Published
- 2021-06-24
- Volume
- 1
- Issue
- 6
- Pages
- 403-409
- ISSN
- 2662-8457 (ISSN-L)
- OpenAlex
- W3097610849
- Cited by
- 1,082
- References
- 39
- Citations by year
- 2026: 266 · 2025: 266 · 2024: 216 · 2023: 178 · 2022: 87 · 2021: 69
- FWCI
- 48.59
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Licence
- Locations
- Nature Computational Science (publishedVersion)
- PubMed (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- arXiv (Cornell University)
- Funders
- International Business Machines Corporation
- Topics
- Physical Sciences › Computer Science › Artificial Intelligence › Quantum Computing Algorithms and Architecture
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum many-body systems
- Physical Sciences › Computer Science › Artificial Intelligence › Quantum Information and Cryptography
- Keywords
- quantum neural networks, quantum machine learning, effective dimension, Fisher information, generalization, model capacity, training speed, quantum advantage, feedforward neural networks, quantum computing hardware
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 2026-10-07.
Classified by jev-1.13-20260917 (gold-guideline-v0.2) on 2026-10-07.
Statistics and arithmetic are recomputed, not judged.
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