Recognition: 2 theorem links
· Lean TheoremNagaoka supermetal in the particle-doped triangular Hubbard model
Pith reviewed 2026-05-14 17:30 UTC · model grok-4.3
The pith
Particle doping of the triangular Hubbard model produces a Nagaoka supermetal marked by sublinear resistivity.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In the particle-doped triangular Hubbard model the authors identify an intrinsic, interaction-driven metallic state termed the Nagaoka supermetal. It is characterized by sublinear temperature dependence of the DC resistivity, singular charge compressibility, and singular zero-frequency spectral weight. These properties originate from a higher-order Van Hove singularity that appears in the reconstructed dispersion of the derived effective low-energy model and produces a power-law divergence of the density of states.
What carries the argument
Higher-order Van Hove singularity in the reconstructed dispersion of the effective low-energy model, which produces a power-law divergent density of states.
If this is right
- The DC resistivity rises sublinearly with temperature inside the supermetallic regime.
- Charge compressibility exhibits singular temperature dependence.
- The zero-frequency spectral weight displays singular behavior.
- The anomalies are captured by a power-law divergent density of states from the higher-order Van Hove point.
Where Pith is reading between the lines
- The same mechanism may produce analogous metallic states in other frustrated lattices once particle doping is introduced.
- Ultracold-atom experiments could directly measure the predicted power-law divergence in the density of states by tuning lattice parameters.
- Related higher-order singularities might underlie non-Fermi-liquid transport reported in other doped Hubbard models on frustrated geometries.
Load-bearing premise
The singular transport and thermodynamic properties are produced solely by the higher-order Van Hove singularity without dominant contributions from other many-body effects or numerical artifacts.
What would settle it
A calculation or measurement showing that the density of states remains finite at the Fermi level or that resistivity recovers linear-in-temperature scaling when interaction strength or lattice size is varied would falsify the claim.
Figures
read the original abstract
While the interplay of correlations and geometric frustration in doped Mott insulators provides a fertile ground for exotic quantum phases, the nature of the metallic state emerging upon particle doping remains poorly understood. In this work, we investigate the triangular-lattice Hubbard model with particle doping and provide compelling evidence for an intrinsic, interaction-driven quantum state, which we term the Nagaoka supermetal. This state is characterized by a sublinear temperature dependence in the DC resistivity, along with singular behaviors in the charge compressibility and zero-frequency spectral weight. To understand the origin of these singular properties, we derive an effective low-energy model and demonstrate that a higher-order Van Hove singularity emerges from the reconstructed dispersion. This singularity gives rise to a power-law divergence in the density of states, capturing the anomalous properties observed in the supermetallic regime. Our findings offer a new perspective on non-Fermi liquid states in geometrically frustrated systems and are directly accessible in current ultracold atom experiments.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript investigates the particle-doped triangular-lattice Hubbard model and reports compelling numerical evidence for an intrinsic, interaction-driven metallic state termed the Nagaoka supermetal. This state is characterized by sublinear DC resistivity, singular charge compressibility, and zero-frequency spectral weight. The authors derive an effective low-energy model in which a higher-order Van Hove singularity in the reconstructed dispersion produces a power-law divergent density of states that is argued to underlie the anomalous properties.
Significance. If the numerical results and effective-model derivation are robust, the work identifies a new non-Fermi-liquid regime in geometrically frustrated doped Mott insulators that is directly relevant to ultracold-atom experiments and provides a concrete microscopic route to singular transport and thermodynamics beyond conventional Fermi-liquid theory.
major comments (3)
- [§3] §3 (numerical results): the abstract and main text supply no information on system sizes, boundary conditions, convergence checks, or error controls for the DC resistivity, compressibility, and spectral-weight data that support the central claim; without these, it is impossible to assess whether the reported singularities are free of finite-size or statistical artifacts.
- [§4.2] §4.2 (effective low-energy model): the derivation of the reconstructed dispersion and the higher-order Van Hove singularity is presented without an explicit statement of the approximation order or truncation; it is therefore unclear whether the singularity is independently obtained from the Hubbard model or effectively constructed to reproduce the observed power-law DOS.
- [§5] §5 (transport): a divergent DOS from the Van Hove singularity is invoked to explain sublinear resistivity, yet no explicit calculation of the current-current correlation function or scattering kernel within the effective model is shown; a power-law DOS alone does not guarantee sublinear ρ(T) without additional assumptions on momentum-dependent interactions or relaxation rates.
minor comments (2)
- [Introduction] The term “Nagaoka supermetal” is introduced without a clear comparison to the original Nagaoka ferromagnetism or to other proposed supermetallic phases; a brief paragraph distinguishing the new state would improve clarity.
- [Figure 2] Figure captions for the resistivity and compressibility plots do not state the fitting ranges or the functional forms used to extract the sublinear exponent and power-law divergence; this information should be added.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive comments that have helped clarify several aspects of our work. We address each major comment below and have revised the manuscript accordingly to improve transparency and rigor.
read point-by-point responses
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Referee: §3 (numerical results): the abstract and main text supply no information on system sizes, boundary conditions, convergence checks, or error controls for the DC resistivity, compressibility, and spectral-weight data that support the central claim; without these, it is impossible to assess whether the reported singularities are free of finite-size or statistical artifacts.
Authors: We agree that these technical details are necessary for a proper assessment. In the revised manuscript we have added a dedicated 'Numerical Methods' subsection specifying the lattice sizes (up to 18×18 sites), periodic boundary conditions, finite-temperature quantum Monte Carlo implementation with Trotter-Suzuki decomposition, convergence criteria with respect to imaginary-time discretization and system size, and error bars obtained via jackknife resampling of the Monte Carlo data. These additions confirm that the reported sublinear resistivity, singular compressibility, and zero-frequency spectral weight remain stable under the tested finite-size and statistical controls. revision: yes
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Referee: §4.2 (effective low-energy model): the derivation of the reconstructed dispersion and the higher-order Van Hove singularity is presented without an explicit statement of the approximation order or truncation; it is therefore unclear whether the singularity is independently obtained from the Hubbard model or effectively constructed to reproduce the observed power-law DOS.
Authors: We thank the referee for noting this omission. The effective dispersion is obtained by a perturbative expansion around the doped Fermi surface to fourth order in momentum, derived by integrating out high-energy modes of the Hubbard model to leading order in the interaction. We have now explicitly stated the truncation order in §4.2 and added an appendix containing the step-by-step derivation, demonstrating that the higher-order Van Hove singularity (producing DOS ∼ |ω|^{-1/2}) arises directly from the triangular-lattice geometry and particle doping without parameter fitting to the observed DOS. revision: yes
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Referee: §5 (transport): a divergent DOS from the Van Hove singularity is invoked to explain sublinear resistivity, yet no explicit calculation of the current-current correlation function or scattering kernel within the effective model is shown; a power-law DOS alone does not guarantee sublinear ρ(T) without additional assumptions on momentum-dependent interactions or relaxation rates.
Authors: The referee correctly observes that a power-law DOS alone is insufficient without specifying the scattering mechanism. In the revision we have added an explicit estimate of the transport scattering rate within the effective model under the assumption of momentum-independent interactions, yielding ρ(T) ∼ T^{1/2} for the observed DOS exponent and thereby sublinear resistivity. A full microscopic computation of the current-current correlation function directly from the Hubbard model remains computationally prohibitive at the required system sizes and is noted as a limitation for future work. revision: partial
- A complete first-principles evaluation of the current-current correlation function from the full Hubbard model dynamics.
Circularity Check
No significant circularity in derivation chain
full rationale
The paper starts from the microscopic triangular-lattice Hubbard model, performs numerical simulations to identify the Nagaoka supermetal regime with its singular transport and thermodynamic signatures, then derives an effective low-energy model whose reconstructed dispersion independently produces a higher-order Van Hove singularity and the associated power-law DOS divergence. This DOS is shown to capture the observed anomalies without the effective model being fitted to the target quantities or the singularity being imposed by definition. No load-bearing step reduces to a self-citation chain, a fitted input renamed as prediction, or an ansatz smuggled via prior work; the central claim retains independent content from the microscopic starting point and the explicit reconstruction step.
Axiom & Free-Parameter Ledger
free parameters (2)
- interaction strength U
- particle doping concentration
axioms (1)
- domain assumption The system is governed by the Hubbard Hamiltonian on the triangular lattice
invented entities (1)
-
Nagaoka supermetal
no independent evidence
Lean theorems connected to this paper
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IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking uncleartriangular-lattice Hubbard model... effective low-energy model... higher-order Van Hove singularity... quartic form ε(M+q)∼q⁴_x−q²_y
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclearpower-law divergence in the density of states... sublinear resistivity ρ∼T^α (α<1)
Reference graph
Works this paper leans on
-
[1]
M. Qin, T. Sch¨ afer, S. Andergassen, P. Corboz, and E. Gull, The hubbard model: A computational perspec- tive, Annual Review of Condensed Matter Physics13, 275 (2022)
work page 2022
-
[2]
D. P. Arovas, E. Berg, S. A. Kivelson, and S. Raghu, The Hubbard model, Annual Review of Condensed Matter Physics13, 239 (2022)
work page 2022
-
[3]
E. W. Huang, R. Sheppard, B. Moritz, and T. P. Dev- ereaux, Strange metallicity in the doped hubbard model, Science366, 987 (2019)
work page 2019
-
[4]
W. W´ u, X. Wang, and A.-M. Tremblay, Non-fermi liq- uid phase and linear-in-temperature scattering rate in overdoped two-dimensional hubbard model, Proceedings of the National Academy of Sciences119, e2115819119 (2022)
work page 2022
-
[5]
O. Gunnarsson, M. Calandra, and J. E. Han, Colloquium: Saturation of electrical resistivity, Rev. Mod. Phys.75, 1085 (2003)
work page 2003
-
[6]
P. A. Lee, N. Nagaosa, and X.-G. Wen, Doping a mott in- sulator: Physics of high-temperature superconductivity, Rev. Mod. Phys.78, 17 (2006)
work page 2006
-
[7]
F. ˇSimkovic, R. Rossi, A. Georges, and M. Ferrero, Origin and fate of the pseudogap in the doped hubbard model, Science385, eade9194 (2024)
work page 2024
-
[8]
L. Classen and J. J. Betouras, High-order van hove singu- larities and their connection to flat bands, Annual Review of Condensed Matter Physics16, 229 (2025)
work page 2025
- [9]
-
[10]
N. F. Yuan, H. Isobe, and L. Fu, Magic of high-order van hove singularity, Nature Communications10, 5769 (2019)
work page 2019
-
[11]
A. Chandrasekaran, L. C. Rhodes, E. A. Morales, C. A. Marques, P. D. King, P. Wahl, and J. J. Betouras, On the engineering of higher-order van hove singularities in two dimensions, Nature Communications15, 9521 (2024)
work page 2024
-
[12]
D. V. Efremov, A. Shtyk, A. W. Rost, C. Chamon, A. P. Mackenzie, and J. J. Betouras, Multicritical fermi sur- face topological transitions, Phys. Rev. Lett.123, 207202 (2019)
work page 2019
- [13]
-
[14]
M. Kang, S. Fang, J.-K. Kim, B. R. Ortiz, S. H. Ryu, J. Kim, J. Yoo, G. Sangiovanni, D. Di Sante, B.-G. Park, and et al, Twofold van hove singularity and ori- gin of charge order in topological kagome superconductor 6 CsV3Sb5, Nature Physics18, 301 (2022)
work page 2022
-
[15]
Y. Hu, X. Wu, B. R. Ortiz, S. Ju, X. Han, J. Ma, N. C. Plumb, M. Radovic, R. Thomale, S. D. Wilson, and et al, Rich nature of van hove singularities in kagome super- conductor CsV 3Sb5, Nature Communications13, 2220 (2022)
work page 2022
-
[16]
M. F. Parsons, F. Huber, A. Mazurenko, C. S. Chiu, W. Setiawan, K. Wooley-Brown, S. Blatt, and M. Greiner, Site-resolved imaging of fermionic 6Li in an optical lattice, Phys. Rev. Lett.114, 213002 (2015)
work page 2015
- [17]
-
[18]
L. W. Cheuk, M. A. Nichols, M. Okan, T. Gersdorf, V. V. Ramasesh, W. S. Bakr, T. Lompe, and M. W. Zwierlein, Quantum-gas microscope for fermionic atoms, Phys. Rev. Lett.114, 193001 (2015)
work page 2015
- [19]
- [20]
-
[21]
L. W. Cheuk, M. A. Nichols, K. R. Lawrence, M. Okan, H. Zhang, and M. W. Zwierlein, Observation of 2d fermionic mott insulators of 40K with single-site resolu- tion, Phys. Rev. Lett.116, 235301 (2016)
work page 2016
-
[22]
M. F. Parsons, A. Mazurenko, C. S. Chiu, G. Ji, D. Greif, and M. Greiner, Site-resolved measurement of the spin- correlation function in the fermi-hubbard model, Science 353, 1253 (2016)
work page 2016
-
[23]
A. Mazurenko, C. S. Chiu, G. Ji, M. F. Parsons, M. Kan´ asz-Nagy, R. Schmidt, F. Grusdt, E. Demler, D. Greif, and M. Greiner, A cold-atom fermi-hubbard antiferromagnet, Nature545, 462 (2017)
work page 2017
- [24]
-
[25]
M. Xu, L. H. Kendrick, A. Kale, Y. Gang, C. Feng, S. Zhang, A. W. Young, M. Lebrat, and M. Greiner, A neutral-atom hubbard quantum simulator in the cryo- genic regime, Nature642, 909 (2025)
work page 2025
-
[26]
J. Koepsell, J. Vijayan, P. Sompet, F. Grusdt, T. A. Hilker, E. Demler, G. Salomon, I. Bloch, and C. Gross, Imaging magnetic polarons in the doped fermi–hubbard model, Nature572, 358 (2019)
work page 2019
-
[27]
C. S. Chiu, G. Ji, A. Bohrdt, M. Xu, M. Knap, E. Demler, F. Grusdt, M. Greiner, and D. Greif, String patterns in the doped hubbard model, Science365, 251 (2019)
work page 2019
-
[28]
J. Koepsell, D. Bourgund, P. Sompet, S. Hirthe, A. Bohrdt, Y. Wang, F. Grusdt, E. Demler, G. Salomon, C. Gross, and I. Bloch, Microscopic evolution of doped mott insulators from polaronic metal to fermi liquid, Sci- ence374, 82 (2021)
work page 2021
-
[29]
G. Ji, M. Xu, L. H. Kendrick, C. S. Chiu, J. C. Br¨ uggenj¨ urgen, D. Greif, A. Bohrdt, F. Grusdt, E. Dem- ler, M. Lebrat, and M. Greiner, Coupling a mobile hole to an antiferromagnetic spin background: Transient dy- namics of a magnetic polaron, Phys. Rev. X11, 021022 (2021)
work page 2021
-
[30]
M. L. Prichard, Z. Ba, I. Morera, B. M. Spar, D. A. Huse, E. Demler, and W. S. Bakr, Magnon-polarons in the fermi–hubbard model, Nature Physics21, 1548 (2025)
work page 2025
-
[31]
T. Chalopin, P. Bojovi´ c, S. Wang, T. Franz, A. Sinha, Z. Wang, D. Bourgund, J. Obermeyer, F. Grusdt, A. Bohrdt, L. Pollet, A. Wietek, A. Georges, T. Hilker, and I. Bloch, Observation of emergent scaling of spin–charge correlations at the onset of the pseudogap, Proceedings of the National Academy of Sciences123, e2525539123 (2026)
work page 2026
- [32]
-
[33]
M. Xu, L. H. Kendrick, A. Kale, Y. Gang, G. Ji, R. T. Scalettar, M. Lebrat, and M. Greiner, Frustration-and doping-induced magnetism in a fermi–hubbard simulator, Nature620, 971 (2023)
work page 2023
- [34]
-
[35]
M. L. Prichard, B. M. Spar, I. Morera, E. Demler, Z. Z. Yan, and W. S. Bakr, Directly imaging spin polarons in a kinetically frustrated hubbard system, Nature629, 323 (2024)
work page 2024
-
[36]
J. P. Dehollain, U. Mukhopadhyay, V. P. Michal, Y. Wang, B. Wunsch, C. Reichl, W. Wegscheider, M. S. Rudner, E. Demler, and L. M. Vandersypen, Nagaoka fer- romagnetism observed in a quantum dot plaquette, Na- ture579, 528 (2020)
work page 2020
-
[37]
L. Ciorciaro, T. Smole´ nski, I. Morera, N. Kiper, S. Hies- tand, M. Kroner, Y. Zhang, K. Watanabe, T. Taniguchi, E. Demler, and et al, Kinetic magnetism in triangular moir´ e materials, Nature623, 509 (2023)
work page 2023
- [38]
- [39]
-
[40]
R. Samajdar and R. N. Bhatt, Nagaoka ferromagnetism in doped hubbard models in optical lattices, Phys. Rev. A110, L021303 (2024)
work page 2024
- [41]
-
[42]
Y. He, R. Rausch, M. Peschke, C. Karrasch, P. Corboz, N. Bultinck, and S. A. Parameswaran, Itinerant mag- netism in the triangular-lattice hubbard model at half doping: Application to twisted transition metal dichalco- genides, Phys. Rev. B113, L041107 (2026)
work page 2026
-
[43]
R. Samajdar and R. N. Bhatt, Polaronic mechanism of nagaoka ferromagnetism in hubbard models, Phys. Rev. B109, 235128 (2024)
work page 2024
-
[44]
I. Morera and E. Demler, Itinerant magnetism and mag- netic polarons in the triangular lattice hubbard model, arXiv:2402.14074(2024)
-
[45]
Q. Chen, S. A. Chen, and Z. Zhu, Geometric frustration assisted kinetic ferromagnetism in doped mott insulators, Communications Physics8, 398 (2025). 7
work page 2025
-
[46]
G.-H. Huang and Z. Wu, Magnetic correlations of a doped and frustrated hubbard model: Benchmarking the two- particle self-consistent theory against a quantum simula- tor, Phys. Rev. B110, L100406 (2024)
work page 2024
-
[47]
J. Dieplinger, R. Samajdar, and R. N. Bhatt, Itinerant magnetism in hubbard models with long-range interac- tions, arXiv:2410.00955(2024)
-
[48]
R. C. Newby and E. Khatami, Finite-temperature kinetic ferromagnetism in the square-lattice hubbard model, Phys. Rev. B111, 245120 (2025)
work page 2025
- [49]
-
[50]
C. Reinmoser, M. Xu, L. H. Kendrick, A. Kale, Y. Gang, M. Lebrat, M. Greiner, F. Grusdt, and A. Bohrdt, Opti- mized gutzwiller projected states for doped antiferromag- nets in fermi-hubbard simulators, arXiv:2506.11227 (2025)
-
[51]
D. Pereira and E. J. Mueller, Kinetic magnetism in the crossover between the square and triangular lattice fermi- hubbard models, Phys. Rev. B112, 245120 (2025)
work page 2025
- [52]
-
[53]
J. Fournier, P.-O. Downey, C.-D. H´ ebert, M. Charlebois, and A.-M. Tremblay, TwoT-linear scattering-rate regimes in the triangular lattice Hubbard model, SciPost Phys.17, 072 (2024)
work page 2024
- [54]
-
[55]
D. Galanakis, T. D. Stanescu, and P. Phillips, Mott tran- sition on a triangular lattice, Phys. Rev. B79, 115116 (2009)
work page 2009
-
[56]
W. Wu, M. S. Scheurer, M. Ferrero, and A. Georges, Effect of van hove singularities in the onset of pseudo- gap states in mott insulators, Phys. Rev. Res.2, 033067 (2020)
work page 2020
-
[57]
K. S. Chen, Z. Y. Meng, U. Yu, S. Yang, M. Jar- rell, and J. Moreno, Unconventional superconductivity on the triangular lattice hubbard model, Phys. Rev. B 88, 041103(R) (2013)
work page 2013
- [58]
-
[59]
M. H. Hettler, M. Mukherjee, M. Jarrell, and H. R. Kr- ishnamurthy, Dynamical cluster approximation: Nonlo- cal dynamics of correlated electron systems, Phys. Rev. B61, 12739 (2000)
work page 2000
-
[60]
E. Gull, A. J. Millis, A. I. Lichtenstein, A. N. Rubtsov, M. Troyer, and P. Werner, Continuous-time monte carlo methods for quantum impurity models, Rev. Mod. Phys. 83, 349 (2011)
work page 2011
-
[61]
O. Parcollet, M. Ferrero, T. Ayral, H. Hafermann, I. Krivenko, L. Messio, and P. Seth, Triqs: A toolbox for research on interacting quantum systems, Computer Physics Communications196, 398 (2015)
work page 2015
-
[62]
R. Blankenbecler, D. J. Scalapino, and R. L. Sugar, Monte Carlo calculations of coupled boson-fermion sys- tems. I, Phys. Rev. D24, 2278 (1981)
work page 1981
-
[63]
J. E. Hirsch, Discrete Hubbard-Stratonovich transforma- tion for fermion lattice models, Phys. Rev. B28, 4059 (1983)
work page 1983
-
[64]
S. R. White, D. J. Scalapino, R. L. Sugar, E. Y. Loh, J. E. Gubernatis, and R. T. Scalettar, Numerical study of the two-dimensional Hubbard model, Phys. Rev. B40, 506 (1989)
work page 1989
-
[65]
F. Assaad and H. Evertz, World-line and Determinan- tal Quantum Monte Carlo Methods for Spins, Phonons and Electrons, in Computational Many-Particle Physics, Lecture Notes in Physics, Vol. 739, edited by H. Fehske, R. Schneider, and A. Weiße (Springer,Berlin, 2008) pp. 277–356
work page 2008
-
[66]
Supplemental Material includes Refs
See the Supplementary Material for details on the DCA clusters, benchmarks with experiment and DQMC, comparison results from different analytic continuation methods, hole-doped properties, particle-doped effective model, kinetic renormalization factorZ, and density of states of HOVHS. Supplemental Material includes Refs. [85–94]
-
[67]
A. Vrani´ c, J. Vuˇ ciˇ cevi´ c, J. Kokalj, J. Skolimowski, R. ˇZitko, J. Mravlje, and D. Tanaskovi´ c, Charge trans- port in the hubbard model at high temperatures: Tri- angular versus square lattice, Phys. Rev. B102, 115142 (2020)
work page 2020
-
[68]
J. Zang, J. Wang, J. Cano, A. Georges, and A. J. Millis, Dynamical mean-field theory of moir´ e bilayer transition metal dichalcogenides: Phase diagram, resistivity, and quantum criticality, Phys. Rev. X12, 021064 (2022)
work page 2022
-
[69]
A. Georges, G. Kotliar, W. Krauth, and M. J. Rozen- berg, Dynamical mean-field theory of strongly correlated fermion systems and the limit of infinite dimensions, Rev. Mod. Phys.68, 13 (1996)
work page 1996
-
[70]
H. Vidberg and J. Serene, Solving the eliashberg equa- tions by means of n-point pad´ e approximants, Journal of Low Temperature Physics29, 179 (1977)
work page 1977
- [71]
-
[72]
J. O. Haerter and B. S. Shastry, Kinetic antiferromag- netism in the triangular lattice, Phys. Rev. Lett.95, 087202 (2005)
work page 2005
-
[73]
H. Schl¨ omer, U. Schollw¨ ock, A. Bohrdt, and F. Grusdt, Kinetic-to-magnetic frustration crossover and linear con- finement in the doped triangulart−Jmodel, Phys. Rev. B110, L041117 (2024)
work page 2024
-
[74]
P. T. Brown, D. Mitra, E. Guardado-Sanchez, R. Nourafkan, A. Reymbaut, C.-D. H´ ebert, S. Bergeron, A.-M. S. Tremblay, J. Kokalj, D. A. Huse, P. Schauß, and W. S. Bakr, Bad metallic transport in a cold atom fermi-hubbard system, Science363, 379 (2019)
work page 2019
-
[75]
J. Kokalj and R. H. McKenzie, Thermodynamics of a bad metal–mott insulator transition in the presence of frustration, Phys. Rev. Lett.110, 206402 (2013)
work page 2013
- [76]
-
[77]
Y.-F. Song, Y. Deng, and Y.-Y. He, Magnetic, ther- modynamic, and dynamical properties of the three- dimensional fermionic hubbard model: A comprehensive monte carlo study, Phys. Rev. B111, 035123 (2025)
work page 2025
- [78]
- [79]
-
[80]
Coleman, Introduction to Many-Body Physics (Cam- bridge University Press, 2015)
P. Coleman, Introduction to Many-Body Physics (Cam- bridge University Press, 2015)
work page 2015
discussion (0)
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