REVIEW 2 major objections 2 minor 74 references
Under certainty the whole distribution grid forms one stable local energy market; under severe congestion every prosumer is better off alone.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · grok-4.5
2026-07-15 14:45 UTC pith:ECAVESQ3
load-bearing objection We do not have the energy-market manuscript: the full text supplied is a different paper (ML-SDRG for quantum spin chains), so the two limiting theorems and the partitioning algorithm cannot be checked. the 2 major comments →
Uncertainty and Autarky: Cooperative Game Theory for Stable Local Energy Market Partitioning
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In a cooperative-game model of distribution grids with coalitional externalities and grid constraints, the optimal stable partition is the grand coalition when prosumption is deterministic, and is pure individual self-consumption when congestion is high; for stochastic prosumption and moderate congestion an algorithm evaluates the optimal stable partition between those extremes.
What carries the argument
The optimal stable partitioning problem: a cooperative game over grid partitions whose value function encodes uncertain prosumption, network constraints, and externalities between coalitions, solved for partitions that are stable for strategic prosumers while balancing operator objectives.
Load-bearing premise
That the paper’s chosen notion of coalitional stability and the way grid physics and uncertainty enter each coalition’s value really match how prosumers decide to join or leave a market.
What would settle it
On a feeder with near-deterministic measured load and generation and mild congestion, show that the grand coalition is unstable under the paper’s value function, or that real prosumers systematically refuse the all-in market while accepting smaller coalitions—directly contradicting the deterministic limiting claim.
If this is right
- Grid operators can treat congestion severity as a structural switch: mild congestion favors one integrated local market; severe congestion favors autarky.
- Prosumption uncertainty alone can block the grand coalition even when lines are not heavily loaded.
- Market-design and tariff rules must be checked for stability under externalities between multiple simultaneous local markets on the same feeder.
- The algorithm gives a concrete way to recompute partitions as forecasts of load, generation, and congestion change.
Where Pith is reading between the lines
- The two limiting regimes suggest a congestion-and-uncertainty driven transition in market structure that operators could monitor with a small set of network metrics.
- The same stability-plus-partition template may transfer to other shared-network resource markets (heat, water, EV charging) where coalitions create externalities on a physical graph.
- If the value function is misspecified, the algorithm still runs but can recommend partitions that real prosumers would leave—so field trials that observe exit behavior are the natural next test.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. From the abstract, the manuscript claims a cooperative-game framework for partitioning a distribution grid into local energy markets (LEMs) under uncertain prosumption, grid constraints, and coalitional externalities. It formulates an “optimal stable partitioning” problem balancing the grid operator against strategic prosumers, asserts that under deterministic load/generation the grand coalition is the optimal stable partition, that under high congestion individual autarky is optimal, and that for stochastic prosumption with moderate congestion an algorithm evaluates the optimal stable partition, with numerical validation on benchmark and real grids. The supplied full-text body, however, is an unrelated manuscript on machine-learning the strong-disorder renormalization group for disordered quantum spin chains (arXiv:2603.05164), so none of the energy-market theorems, value function, stability concept, algorithm, or experiments can be inspected.
Significance. If the abstract claims hold under a well-specified core/stability notion and a faithful network-physics value function, the work would clarify how uncertainty and congestion shape LEM scale and composition and would give operators a concrete partitioning tool. That significance cannot be assessed from the materials provided: the limiting theorems, the algorithm, and the numerical evidence are not present in the full text that was supplied.
major comments (2)
- Manuscript mismatch: the title, abstract, and arXiv id (2603.05169, eess.SY) describe cooperative-game LEM partitioning, but the full-text body is the ML-SDRG quantum-spin-chain paper (arXiv:2603.05164, cond-mat.dis-nn). No definition of the characteristic function, stability concept (core, nucleolus, etc.), uncertainty model, optimal-stable-partitioning program, algorithm, or grid experiments for the energy-market claims appears in the supplied text. The two limiting statements and the algorithm claim are therefore unverifiable.
- Because the correct body is absent, the load-bearing modeling choice identified in the abstract—the value function that encodes grid constraints and coalitional externalities, and the stability notion used for “optimal stable partition”—cannot be checked for internal consistency or operational fidelity. Without that, neither the deterministic grand-coalition result nor the high-congestion autarky result can be audited.
minor comments (2)
- Abstract alone does not name the cooperative-game solution concept or the prosumption uncertainty model (scenario set vs. distribution family); those should be stated explicitly once the correct manuscript is supplied.
- Abstract uses “largest market coalition” and “individual self-consumption” without defining the partition lattice or the congestion metric that separates the “high” vs. “moderate” regimes; precise definitions will be needed for reproducibility.
Circularity Check
No circularity can be established: the supplied full-text block is a different manuscript (ML-SDRG quantum spins) and supplies no equations or proofs for the energy-market claims.
full rationale
The abstract of 2603.05169 asserts two limiting theorems (grand coalition optimal under deterministic prosumption; autarky optimal under high congestion) plus an algorithm for the stochastic moderate-congestion regime. The CACHEABLE full-text block, however, is the unrelated arXiv:2603.05164 manuscript on graph-neural-network approximation of strong-disorder RG for long-range spin chains; it contains none of the cooperative-game value functions, stability notions, grid-constraint encodings, or partition algorithms required to audit those claims. Consequently no load-bearing step of the energy-market derivation can be quoted or reduced to its own inputs. On the abstract alone the structure is the ordinary non-circular pattern of proving extremes and supplying a computational method for the intermediate case; residual modeling risk (choice of core concept or uncertainty representation) is a correctness issue, not circularity. Score is therefore 0 with empty steps.
Axiom & Free-Parameter Ledger
free parameters (2)
- Congestion level thresholds separating 'high' vs 'moderate' regimes
- Uncertainty model for prosumption (distribution family / scenario set)
axioms (3)
- domain assumption Prosumers form coalitions according to a cooperative-game stability concept that remains meaningful under coalitional externalities induced by shared grid constraints.
- domain assumption Grid constraints and network physics can be encoded into coalition values so that the optimal stable partition balances operator and prosumer interests.
- ad hoc to paper Deterministic and high-congestion extremes are analytically tractable and yield grand-coalition and autarky optima respectively.
invented entities (1)
-
Optimal stable partitioning problem (operator–prosumer balanced objective over stable partitions)
no independent evidence
read the original abstract
Local energy markets empower prosumers in distribution grids to form coalitions for collective self-consumption. An open question is to analyze the scale and composition of local energy market coalitions formed by strategic prosumers in distribution grids. This analysis must account for grid constraints, stochasticity of load and generation, as well as the interaction between possibly multiple local energy markets in the distribution grid. In this work, we present a cooperative game theoretic framework to study distribution grid partitioning into local energy markets under uncertain prosumption, grid constraints, and coalitional externalities. We formulate the optimal stable partitioning problem to balance the interests of the grid operator with that of strategic prosumers. Under deterministic load and generation, we show that the largest market coalition is the optimal stable partition. Under high levels of grid congestion, we show that individual self-consumption corresponds to the optimal stable partition. For the general case of stochastic prosumption and moderate grid congestion levels, we provide an algorithm to evaluate the optimal stable partition. We validate our algorithm and theory using numerical experiments on benchmark and real world distribution grids. Our results help in understanding the impact of prosumption uncertainty and grid constraints on coalition formation.
Reference graph
Works this paper leans on
-
[1]
P. W. Anderson, Absence of diffusion in certain random lattices, Phys. Rev.109, 1492 (1958)
1958
-
[2]
H. v. L¨ ohneysen, Disorder, electron-electron interactions and the metal-insulator transition in heavily doped Si:P, Adv. in Solid State Phys.40, 143 (2000)
2000
-
[3]
Kettemann, Towards a Comprehensive Theory of Metal-Insulator Transitions in Doped Semiconductors, Special Issue in memory of K
S. Kettemann, Towards a Comprehensive Theory of Metal-Insulator Transitions in Doped Semiconductors, Special Issue in memory of K. B. Efetov, Annals of Physics 456, 169306 (2023)
2023
-
[4]
S. Kettemann, Competition between Kondo Effect and RKKY Coupling, Lecture Notes of the Autumn School on Correlated Electrons 2024, Correlations and Phase Transitions, Band/Volume 14 edited by Eva Pavarini and Erik Koch,Verlag des Forschungszentrums J¨ ulich (2024)
2024
-
[5]
Salvino, S
D. Salvino, S. Rogge, B. Tigner, D. Osheroff, Low Temperature ac Dielectric Response of Glasses to High dc Electric Fields, Phys. Rev. Lett.73, 286 (1994)
1994
-
[6]
C. C. Yu and A. J. Leggett, Low temperature properties of amorphous materials: Through a glass darkly, Commun. Condens. Mat. Phys.14, 231 (1988)
1988
-
[7]
Graß and M
T. Graß and M. Lewenstein, Trapped-ion quantum simulation of tunable-range Heisenberg chains, EPJ Quantum Tech- nology 1:8 (2014)
2014
-
[8]
Signoles, T
A. Signoles, T. Franz, R. F. Alves, M. G¨ arttner, S. Whitlock, G. Z¨ urn, and M. Weidem¨ uller, Glassy dynamics in a disordered Heisenberg quantum spin system, Phys. Rev.X 11, 011011 (2021)
2021
-
[9]
Browaeys and T
A. Browaeys and T. Lahaye, Many-body physics with individually controlled Rydberg atoms, Nature Physics16, 132 (2020)
2020
-
[10]
Islam, C
R. Islam, C. Senko, W. C. Campbell, S. Korenblit, J. Smith, A. Lee, E. E. Edwards, C.-C. J. Wang, J. K. Freericks, and C. Monroe, Emergence and Frustration of Magnetic Order with Variable-Range Interactions in a Trapped Ion Quantum Simulator, Science340, 583 (2013)
2013
-
[11]
Richerme, Z.-X
P. Richerme, Z.-X. Gong, A. Lee, C. Senko, J. Smith, M. Foss- Feig, S. Michalakis, A. V. Gorshkov, and C. Monroe, Non-local propagation of correlations in quantum systems with long-range interactions, Nature (London) 511, 198 (2014)
2014
-
[12]
B. L. Dwyer, L. V. H. Rodgers, E. K. Urbach, D. Bluvstein, S. Sangtawesin, H. Zhou, Y. Nassab, M. Fitzpatrick, Z. Yuan, K. De Greve, E. L. Peterson, H. Knowles, T. Sumarac, J.-P. Chou, A. Gali, V.V. Dobrovitski, M. D. Lukin and N. P. de Leon, Probing spin dynamics on diamond surfaces using a single quantum sensor, PRX Quantum3, 040328 (2022)
2022
-
[13]
E. J. Davis, B. Ye, F. Machado, S. A. Meynell, W. Wu, T. Mittiga, W. Schenken, M. Joos, B. Kobrin, Y. Lyu, Z. Wang, D. Bluvstein, S. Choi, C. Zu, A. C. Bleszynski Jayich, N. Y. Yao, Probing many-body dynamics in a two dimensional dipolar spin ensemble, Nature Physics, 19, 836–844 (2023)
2023
-
[14]
Altman et al., Quantum simulators: Architectures and opportunities, PRX Quantum 2, 017003 (2021)
E. Altman et al., Quantum simulators: Architectures and opportunities, PRX Quantum 2, 017003 (2021)
2021
-
[15]
A. Lunkin et al., Evidence for a two-dimensional quantum glass state at high temperatures, https://arxiv.org/abs/2601.01309v1 (2026)
Pith/arXiv arXiv 2026
-
[16]
R. N. Bhatt and P. A. Lee, A scaling method for low temperature behavior of random antiferromagnetic systems, Journal of Applied Physics52, 1703-1707 (1981)
1981
-
[17]
R. N. Bhatt and P. A. Lee, Scaling studies of highly disordered spin-1/2 antiferromagnetic systems, Phys. Rev. Lett.48, 344(1982)
1982
-
[18]
D. S. Fisher, Random antiferromagnetic quantum spin chains, Phys. Rev. B50, 3799 (1994)
1994
-
[19]
D. S. Fisher, Critical behavior of random transverse-field Ising spin chains , Phys. Rev. B51, 6411 (1995)
1995
-
[20]
Igloi and C
F. Igloi and C. Monthus, Strong disorder RG approach of random systems, Phys. Rep.412, 277 (2005)
2005
-
[21]
Igl´ oi and C
F. Igl´ oi and C. Monthus, Strong disorder RG approach - a short review of recent developments, Eur. Phys. J.B 91, 290 (2018)
2018
-
[22]
Vosk and E
R. Vosk and E. Altman, Many-Body Localization in One Dimension as a Dynamical Renormalization Group Fixed Point, Phys. Rev. Lett.110, 067204 (2013)
2013
-
[23]
Igloi, Z
F. Igloi, Z. Szatm´ ari, and Y-C. Lin, Entanglement entropy dynamics of disordered quantum spin chains, Phys. Rev. B 85, 094417 (2012)
2012
-
[24]
Moure, S
N. Moure, S. Haas, S. Kettemann, Many Body Localization Transition in Random Quantum Spin Chains with Long Range Interactions, Europhys. Lett.111, 27003 (2015)
2015
-
[25]
Moure, Hyun-Yong Lee, S
N. Moure, Hyun-Yong Lee, S. Haas, R. N. Bhatt, S. Kettemann, Disordered Quantum SCs with Long-Range Antiferro- magnetic Interactions, Phys. Rev.B 97, 014206 (2018)
2018
-
[26]
Mohdeb, J
Y. Mohdeb, J. Vahedi, N. Moure, A. Roshani, H.Y. Lee, R. Bhatt, S. Haas, S. Kettemann, Entanglement Properties of Disordered Quantum SCs with Long-Range Antiferromagnetic Interactions, Phys. Rev.B 102, 214201 (2020)
2020
-
[27]
S. Kettemann, Strong Disorder Renormalization Group Method for Bond Disordered Antiferromagnetic Quantum Spin Chains with Long Range Interactions: Ground State Properties, accepted for publication in Phys. Rev. B (2025), https://doi.org/10.1103/b6wg-bt9k
-
[28]
Juh´ asz, I
R. Juh´ asz, I. A. Kov´ acs, F. Igl´ oi, Random transverse-field Ising chain with long-range interactions, Europhys. Lett.,107, 47008 (2014)
2014
-
[29]
I. A. Kov´ acs, R. Juh´ asz, F. Igl´ oi, Long-range random transverse-field Ising model in three dimensions, Phys. Rev. B93, 184203 (2016)
2016
-
[30]
Pekker, G
D. Pekker, G. Refael, E. Altman, E. Demler, and V. Oganesyan, Hilbert-glass transition: New universality of temperature- tuned many-body dynamical quantum criticality, Phys. Rev. X 4, 011052 (2014). 12
2014
-
[31]
Huang and J
Y. Huang and J. E. Moore, Excited-state entanglement and thermal mutual information in random spin chains, Phys. Rev. B 90, 220202 (2014)
2014
-
[32]
A. S. Aramthottil, P. Sierant, M. Lewenstein, and J. Zakrzewski, Phenomenology of many-body localization in bond- disordered spin chains, Phys. Rev. Lett. 133, 196302 (2024)
2024
-
[33]
Mohdeb, J
Y. Mohdeb, J. Vahedi, S. Kettemann, Excited-Eigenstate Properties of XX Spin Chains with Random Long-Range Inter- actions, Phys. Rev. BB 106, 104201 (2022)
2022
-
[34]
S. Kettemann, Finite Temperature Properties of Antiferromagnetic Quantum Spin Chains with Random Long Range Couplings, submitted for publication in Phys. Rev. B (2025), https://arxiv.org/abs/2509.17828
Pith/arXiv arXiv 2025
-
[35]
Mohdeb, J
Y. Mohdeb, J. Vahedi, S. Haas, R. N. Bhatt, S. Kettemann, Global Quench Dynamics and the Growth of Entanglement Entropy in Disordered Spin Chains with Tunable Range Interactions, Phys. Rev. B 108, L140203 (2023)
2023
-
[37]
Mehta, M
P. Mehta, M. Bukov, C.-H. Wang, A. G.R. Day, C. Richardson, C. K. Fisher, D. J. Schwab, Physics Reports810. 1–124 (2019)
2019
-
[38]
Carleo, I
G. Carleo, I. Cirac, K. Cranmer, L. Daudet, M. Schuld, N. Tishby, L. Vogt-Maranto, L. Zdeborov´ a, Rev. Mod. Phys.91, 045002 (2019)
2019
-
[39]
Carleo and M
G. Carleo and M. Troyer, Solving the Quantum Many-Body Problem with Artificial Neural Networks, Science 355, 602 (2017)
2017
-
[40]
D.-L. Deng, X. Li and S. Das Sarma, Quantum Entanglement in Neural Network States, Phys. Rev. X 7, 021021 (2017)
2017
-
[41]
Nomura,Helping restricted Boltzmann machines with quantum-state representation by restoring symmetry, J
Y. Nomura,Helping restricted Boltzmann machines with quantum-state representation by restoring symmetry, J. Phys.: Condens. Matter 33 (2020)
2020
-
[42]
K. Choo, G. Carleo, N. Regnault, T. Neupert,Symmetries and Many-Body Excitations with Neural-Network Quantum States, Phys. Rev. Lett. 121, 167204 (2018)
2018
-
[43]
R. Rende, L. L. Viteritti, F. Becca, et al., Foundation neural-networks quantum states as a unified Ansatz for multiple hamiltonians. Nat Commun 16, 7213 (2025). https://doi.org/10.1038/s41467-025-62098-x
-
[44]
Luciano Loris Viteritti, Riccardo Rende, Giacomo Bracci Testasecca, Jacopo Niedda, Roderich Moessner, Giuseppe Carleo, Antonello Scardicchio, Quantum Spin Glass in the Two-Dimensional Disordered Heisenberg Model via Foundation Neural- Network Quantum States, https://arxiv.org/abs/2507.05073 (2025)
arXiv 2025
-
[45]
K. Choo, T. Neupert, G. Carleo,Two-dimensional frustrated J1-J2 model studied with neural network quantum states, Phys. Rev. B 100, 125124 (2019)
2019
-
[46]
Roca-Jerat, M
S. Roca-Jerat, M. Gallego, F. Luis, J. Carrete, D. Zueco,Transformer wave function for quantum long-range models, Phys. Rev. B 110, 205147 (2024)
2024
-
[47]
Sharir, Y
O. Sharir, Y. Levine, N. Wies, G. Carleo, A. Shashua,Deep autoregressive models for the efficient variational simulation of many-body quantum systems, Phys. Rev. Lett. 124, 020503 (2019)
2019
-
[48]
Lange, A
H. Lange, A. Van de Walle, A. Abedinnia and A. Bohrdt, From architectures to applications: a review of neural quantum states, Quantum Sci. Technol.9, 040501 (2024)
2024
-
[49]
A. Sheshmani, Y.-Z. You, B. Buyukates, A. Ziashahabi, S. Avestimehr,Renormalization Group flow, Optimal Transport and Diffusion-based Generative Model, https://arxiv.org/abs/2402.17090 (2024)
Pith/arXiv arXiv 2024
-
[50]
P. Mehta and D. J. Schwab, An exact mapping between the variational renormalization group and deep learning, arXiv:1410.3831. (2014)
Pith/arXiv arXiv 2014
-
[51]
C. Fan, M. Shen, Z. Nussinov, et al.,Searching for spin glass ground states through deep reinforcement learning, Nat. Commun.14, 725 (2023)
2023
-
[52]
W. Hou and Y.-Z. You, Machine Learning Renormalization Group for Statistical Physics, arXiv:2306.11054 (2023)
Pith/arXiv arXiv 2023
-
[53]
X.-Z. Luo, D. Luo and R. G. Melko, Operator Learning Renormalization Group, arXiv:2403.03199 (2024)
Pith/arXiv arXiv 2024
-
[54]
Di Sante, M
D. Di Sante, M. Medvid´ ovi´ c, A. Toschi, G. Sangiovanni, C. Franchini, A. M. Sengupta and A. J. Millis, Deep Learning the Functional Renormalization Group, Physical Review Letters 129, 136402 (2022)
2022
-
[55]
T. Marchand, M. Ozawa, G. Biroli and S. Mallat, Wavelet Conditional Renormalization Group, arXiv:2207.04941 (2022)
Pith/arXiv arXiv 2022
-
[56]
Y. Zhao, M. M. Fogler and Y.-Z. You, Application of deep neural networks for computing the renormalization group flow of the two-dimensionalϕ 4 field theory, arXiv:2510.06508 (2024)
Pith/arXiv arXiv 2024
-
[57]
P. M. Lenggenhager, D. E. G¨ okmen, Z. Ringel, S. D. Huber and M. Koch-Janusz, Optimal Renormalization Group Transformation from Information Theory, Physical Review X 10, 011037 (2020)
2020
-
[58]
D. E. G¨ okmen, Z. Ringel, S. D. Huber and M. Koch-Janusz, Statistical physics through the lens of real-space mutual information, Physical Review Letters 127, 240603 (2021)
2021
-
[59]
D. E. G¨ okmen, S. Biswas, S. D. Huber, Z. Ringel, F. Flicker and M. Koch-Janusz, Compression theory for inhomogeneous systems, Nature Communications 15, 10123 (2024)
2024
-
[60]
Erdmenger, K
J. Erdmenger, K. T. Grosvenor and R. Jefferson, Towards quantifying information flows: relative entropy in deep neural networks and the renormalization group, SciPost Physics 12, 041 (2022)
2022
-
[61]
T Ohtsuki, T Ohtsuki, Deep learning the quantum phase transitions in random two-dimensional electron systems, Journal of the Physical Society of Japan 85 (12), 123706 (2016)
2016
-
[62]
C. Beetar, J. Murugan and D. Rosa, Neural Networks as Universal Probes of Many-Body Localization in Quantum Graphs, arXiv:2108.05737 (2021)
Pith/arXiv arXiv 2021
-
[63]
Chen, Many-body mobility edges in one and two dimensions revealed by convolutional neural networks, Physical Review B 109, 075124 (2024)
A. Chen, Many-body mobility edges in one and two dimensions revealed by convolutional neural networks, Physical Review B 109, 075124 (2024)
2024
-
[64]
A. Saleh, Predicting the von Neumann Entanglement Entropy Using a Graph Neural Network, arXiv:2503.23635 (2025). 13
Pith/arXiv arXiv 2025
-
[65]
Huang et al., Direct entanglement detection of quantum systems using machine learning, npj Quantum Information 11, 29 (2025)
J. Huang et al., Direct entanglement detection of quantum systems using machine learning, npj Quantum Information 11, 29 (2025)
2025
-
[66]
Passetti, A
G. Passetti, A. Mollabashi, M. Haque, F. Marquardt and N. Mohseni, Deep learning of many-body observables and quantum information scrambling, Quantum 8, 1417 (2024)
2024
-
[67]
P. Schmidt, F. Marquardt and N. Mohseni, Transfer learning in predicting quantum many-body dynamics: from physical observables to entanglement entropy, Quantum Science and Technology, doi:10.1088/2058-9565/adbd6d (2024)
-
[68]
E. A. Meirom, H. Maron, S. Mannor and G. Chechik, Optimizing Tensor Network Contraction Using Reinforcement Learning, Proceedings of the 39th International Conference on Machine Learning, PMLR 162, 15278–15312 (2022)
2022
-
[69]
Refael and J
G. Refael and J. E. Moore, Entanglement Entropy of Random Quantum Critical Points in One Dimension, Phys. Rev. Lett.93, 260602 (2004)
2004
-
[70]
J. A. Hoyos, A. P. Vieira, N. Laflorencie, and E. Miranda, Correlation amplitude and entanglement entropy in random spin chains, Phys. Rev.B 76, 174425 (2007)
2007
-
[71]
Calabrese and J
P. Calabrese and J. Cardy, Entanglement entropy and quantum field theory, J. Stat. Mech.: Theory Exp. P06002 (2004)
2004
-
[72]
T. Hikihara et al., Tensor-network strong-disorder renormalization groups for random quantum spin systems in two di- mensions, arXiv:2006.12857 (2020)
Pith/arXiv arXiv 2006
-
[73]
K. Seki, T. Hikihara and K. Okunishi, Entanglement-based tensor-network strong-disorder renormalization group, arXiv:2107.01555 (2021)
Pith/arXiv arXiv 2021
-
[74]
Hikihara, H
T. Hikihara, H. Ueda, K. Okunishi, K. Harada and T. Nishino, Automatic structural optimization of tree tensor networks, Physical Review Research 5, 013031 (2023)
2023
-
[75]
Ozawa and Y
T. Ozawa and Y. Kitano, Renormalization-group-inspired neural networks for computing topological invariants, Physical Review B 105, 205139 (2022)
2022
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.