pith. sign in

arxiv: 2511.22927 · v3 · submitted 2025-11-28 · ❄️ cond-mat.str-el · cond-mat.mtrl-sci· physics.comp-ph

Two-Electron Correlations in the Metallic Electron Gas

Pith reviewed 2026-05-17 04:51 UTC · model grok-4.3

classification ❄️ cond-mat.str-el cond-mat.mtrl-sciphysics.comp-ph
keywords uniform electron gasfour-point vertex functionLandau parametersKukkonen-Overhauser interactionthermal resistivityvariational diagrammatic Monte Carlotwo-electron scatteringmetallic transport
0
0 comments X p. Extension

The pith

A minimal s-wave correction to the Kukkonen-Overhauser interaction captures two-electron scattering and matches thermal resistivity data in simple metals.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper computes the four-point vertex function for the three-dimensional uniform electron gas to high precision using variational diagrammatic Monte Carlo. From these results the authors extract Landau parameters showing a density-driven crossover from underscreening to overscreening and determine the full two-electron scattering amplitude on the Fermi surface. Residual analysis demonstrates that only a minimal s-wave correction in the antiparallel-spin channel is required beyond the charge-channel Kukkonen-Overhauser interaction, which defines the sKO+ ansatz. When this ansatz is used to calculate the electron-electron contribution to thermal resistivity, the values agree quantitatively with experiments on aluminum, sodium, potassium, and rubidium.

Core claim

High-precision variational diagrammatic Monte Carlo calculations of the four-point vertex function in the uniform electron gas reveal Landau parameters that cross over from underscreening to overscreening with changing density. The complete two-electron scattering amplitude on the Fermi surface is obtained with controlled accuracy. A residual analysis against the charge-channel Kukkonen-Overhauser interaction shows that only a minimal s-wave correction in the antiparallel-spin channel is needed, defining the sKO+ ansatz that combines the local-density approximation to the Kukkonen-Overhauser interaction with this short-range term. This ansatz then yields quantitative agreement with measured

What carries the argument

The sKO+ ansatz: the Kukkonen-Overhauser interaction within the local-density approximation supplemented by a minimal short-range s-wave correction in the antiparallel-spin channel, which acts as a transferable effective interaction for transport calculations.

If this is right

  • The electron-electron contribution to thermal resistivity can be computed for simple metals with quantitative accuracy using this effective interaction.
  • First-principles transport calculations in metals can incorporate electron correlations via this transferable ansatz without requiring a full treatment of the vertex function.
  • The approach bridges results from the idealized uniform gas directly to measured transport properties in real materials.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The dominance of a single short-range correction suggests that local correlations are the primary missing ingredient beyond standard interaction models.
  • The same ansatz could be tested on related transport coefficients such as electrical resistivity or on the specific heat to check consistency across observables.
  • Extensions to two-dimensional electron gases or to metals with stronger band-structure effects would reveal the boundaries of transferability from the uniform-gas limit.

Load-bearing premise

The minimal s-wave correction extracted from the uniform electron gas remains accurate and sufficient when applied to real metals that include lattice and band-structure effects.

What would settle it

A clear mismatch between the thermal resistivity predicted by the sKO+ ansatz and new experimental measurements on a simple metal such as cesium, or a lattice-model calculation showing that substantially larger corrections are required once periodicity is included.

Figures

Figures reproduced from arXiv: 2511.22927 by Bao-Zong Wang, Kun Chen, Pengcheng Hou, Youjin Deng, Zhiyi Li.

Figure 1
Figure 1. Figure 1: FIG. 1. The electron-electron contribution to the thermal [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Numerical results of the symmetric (left panel) and [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Angle-resolved Landau quasiparticle interaction for [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. The dimensionless two-electron scattering amplitude [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
read the original abstract

We present high-precision \emph{ab initio} calculations of the four-point vertex function for the three-dimensional uniform electron gas using variational diagrammatic Monte Carlo. From these results, we extract Landau parameters that reveal a density-driven crossover from underscreening to overscreening, and obtain the full two-electron scattering amplitude on the Fermi surface with controlled accuracy. A residual analysis of the scattering amplitude against the charge-channel Kukkonen--Overhauser (KO$^+$) interaction shows that only a minimal s-wave correction in the antiparallel-spin channel is needed, defining the sKO$^+$ ansatz: KO$^+$ within the local-density approximation plus this short-range correction. Using both our direct VDMC amplitudes and the sKO$^+$ ansatz, we compute the electron-electron contribution to the thermal resistivity, obtaining quantitative agreement with experiments on simple metals (Al, Na, K, Rb). sKO$^+$ thus provides a transferable effective interaction for first-principles transport calculations in metals.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript presents high-precision variational diagrammatic Monte Carlo calculations of the four-point vertex function in the three-dimensional uniform electron gas. It extracts Landau parameters indicating a density-driven crossover from underscreening to overscreening and determines the two-electron scattering amplitude on the Fermi surface. A residual analysis against the charge-channel Kukkonen-Overhauser interaction identifies a minimal s-wave correction in the antiparallel channel, leading to the sKO+ ansatz. This ansatz is applied to compute the electron-electron contribution to thermal resistivity in simple metals, yielding quantitative agreement with experimental data for Al, Na, K, and Rb.

Significance. Should the transferability of the sKO+ ansatz be confirmed, this work would offer a valuable effective interaction for ab initio calculations of transport properties in metals, allowing quantitative predictions of electron-electron scattering effects without full many-body simulations for each material. The controlled accuracy of the VDMC vertex calculations is a notable technical strength.

major comments (2)
  1. [transport calculations] In the transport calculations section, the quantitative agreement with experiment is presented without accompanying error bars, convergence tests, or a detailed description of the fitting procedure for the s-wave correction amplitude from the VDMC data. This information is necessary to evaluate the robustness of the central claim.
  2. [application to real metals] In the section on application to real metals, the sKO+ ansatz is derived entirely from uniform electron gas calculations and applied to real metals; no direct assessment or bound is given on how lattice potentials and band structure might modify the short-range antiparallel s-wave correction, which underpins the transferability assertion.
minor comments (2)
  1. Some figures could benefit from additional labels or legends for clarity in comparing VDMC and sKO+ results.
  2. [Introduction] The definition of the sKO+ ansatz could be introduced with more explicit reference to the equations defining the correction term.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive comments. We address each major point below and have revised the manuscript accordingly to strengthen the presentation of the transport results and to clarify the assumptions underlying the transferability of the sKO+ ansatz.

read point-by-point responses
  1. Referee: In the transport calculations section, the quantitative agreement with experiment is presented without accompanying error bars, convergence tests, or a detailed description of the fitting procedure for the s-wave correction amplitude from the VDMC data. This information is necessary to evaluate the robustness of the central claim.

    Authors: We agree that the robustness of the quantitative agreement would be better established with these details. In the revised manuscript we have added statistical error bars to the thermal resistivity curves, obtained from the Monte Carlo sampling variance in the VDMC vertex calculations. We have included a new subsection on numerical convergence, showing results for increasing diagrammatic order (up to order 6) and for different numbers of Monte Carlo samples. We have also expanded the description of the fitting procedure: the s-wave correction amplitude in the antiparallel channel is obtained by a least-squares minimization of the residual between the full VDMC scattering amplitude and the KO+ interaction on the Fermi surface, with the optimal value and its uncertainty now reported explicitly. These additions appear in the updated transport calculations section. revision: yes

  2. Referee: In the section on application to real metals, the sKO+ ansatz is derived entirely from uniform electron gas calculations and applied to real metals; no direct assessment or bound is given on how lattice potentials and band structure might modify the short-range antiparallel s-wave correction, which underpins the transferability assertion.

    Authors: We acknowledge that a direct, quantitative bound on lattice-induced modifications to the short-range correction would require extending the VDMC calculations beyond the uniform electron gas. Such an extension lies outside the scope of the present work. In the revised manuscript we have added a dedicated paragraph in the application section that discusses the expected size of these effects for simple metals. We note that the nearly spherical Fermi surfaces and weak pseudopotentials in Al, Na, K, and Rb make the uniform-gas approximation particularly appropriate, and we cite earlier comparisons of electron-gas and band-structure results for related quantities to provide qualitative bounds. We also emphasize that the quantitative match to experiment for these four metals offers indirect support for the ansatz, while explicitly stating the assumption of limited lattice modification as a limitation of the current study. revision: partial

Circularity Check

0 steps flagged

No significant circularity in the derivation chain

full rationale

The paper computes the four-point vertex and scattering amplitudes via VDMC for the uniform electron gas, identifies a minimal s-wave correction via residual analysis against KO+, defines the sKO+ ansatz from that analysis, and applies the ansatz (with LDA) to compute thermal resistivity for real metals, reporting quantitative agreement with independent experimental data on Al, Na, K, and Rb. The final comparison is to external benchmarks outside the fitted UEG amplitudes; no equation or result reduces to its inputs by construction, and the transferability step is an assumption rather than a definitional loop. The derivation remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 1 invented entities

The central claim rests on the assumption that the uniform electron gas captures the dominant electron-electron scattering physics relevant to transport in real simple metals, plus the empirical determination of one short-range correction parameter.

free parameters (1)
  • minimal s-wave correction amplitude
    Short-range correction in the antiparallel-spin channel obtained from residual analysis of the VDMC scattering amplitude against the KO+ interaction.
axioms (1)
  • domain assumption The uniform electron gas model is sufficiently representative of metallic electron behavior for quantitative transport predictions.
    Invoked when mapping computed resistivities onto experimental data for Al, Na, K, and Rb.
invented entities (1)
  • sKO+ ansatz no independent evidence
    purpose: Transferable effective two-electron interaction for first-principles transport calculations
    Defined as the charge-channel KO+ interaction within the local-density approximation plus the fitted short-range s-wave correction.

pith-pipeline@v0.9.0 · 5483 in / 1457 out tokens · 33188 ms · 2026-05-17T04:51:26.086183+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

  • IndisputableMonolith/Cost/FunctionalEquation.lean washburn_uniqueness_aczel unclear
    ?
    unclear

    Relation between the paper passage and the cited Recognition theorem.

    We present high-precision ab initio calculations of the four-point vertex function for the three-dimensional uniform electron gas using variational diagrammatic Monte Carlo... propose a charge-based Kukkonen–Overhauser effective interaction within the local-density approximation, supplemented by a small s-wave correction (sKO+)

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Forward citations

Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. First-Principles Effective Mass in the Three-Dimensional Uniform Electron Gas

    cond-mat.str-el 2026-05 unverdicted novelty 6.0

    The effective mass ratio m*/m in the 3D uniform electron gas stays close to 1 with only shallow non-monotonic density dependence up to r_s=6.

  2. Quantum effects in plasmas

    physics.plasm-ph 2026-04 unverdicted novelty 2.0

    Quantum effects govern behavior in warm dense matter and inertial fusion plasmas and are best modeled by combining quantum methods through downfolding from first-principles simulations.

Reference graph

Works this paper leans on

86 extracted references · 86 canonical work pages · cited by 2 Pith papers · 1 internal anchor

  1. [1]

    Alexandradinata, N

    A. Alexandradinata, N. P. Armitage, A. Baydin, W. Bi, Y. Cao, H. J. Changlani, E. Chertkov, E. H. da Silva Neto, L. Delacretaz, I. E. Baggari, G. M. Fer- guson, W. J. Gannon, S. A. A. Ghorashi, B. H. Goodge, O. Goulko, G. Grissonnanche, A. Hallas, I. M. Hayes, Y. He, E. W. Huang, A. Kogar, D. Kumah, J. Y. Lee, A. Legros, F. Mahmood, Y. Maximenko, N. Pella...

  2. [2]

    Dagotto, Correlated electrons in high-temperature su- perconductors, Rev

    E. Dagotto, Correlated electrons in high-temperature su- perconductors, Rev. Mod. Phys. 66, 763 (1994)

  3. [3]

    R. L. Greene, P. R. Mandal, N. R. Poniatowski, and T. Sarkar, The strange metal state of the electron-doped cuprates, Annual Review of Condensed Matter Physics 11, 213 (2020)

  4. [4]

    M. Z. Hasan and C. L. Kane, Colloquium: Topological insulators, Rev. Mod. Phys. 82, 3045 (2010)

  5. [5]

    Loos and P

    P.-F. Loos and P. M. W. Gill, The uniform electron gas, WIREs Computational Molecular Science 6, 410 (2016)

  6. [7]

    A. A. Abrikosov, L. P. Gorkov, and I. E. Dzyaloshin- ski, Methods of quantum field theory in statistical physics (Courier Corporation, 2012)

  7. [8]

    J. W. Negele, Quantum many-particle systems (CRC Press, 2018)

  8. [9]

    Bardeen, L

    J. Bardeen, L. N. Cooper, and J. R. Schrieffer, Theory of superconductivity, Phys. Rev. 108, 1175 (1957)

  9. [10]

    G. A. Brooker and J. Sykes, Transport properties of a fermi liquid, Phys. Rev. Lett. 21, 279 (1968)

  10. [11]

    Galler, P

    A. Galler, P. Thunstr¨ om, P. Gunacker, J. M. Tomczak, and K. Held, Ab initio dynamical vertex approximation, Phys. Rev. B 95, 115107 (2017)

  11. [12]

    Kaufmann, C

    J. Kaufmann, C. Eckhardt, M. Pickem, M. Kitatani, A. Kauch, and K. Held, Self-consistent ladder dynamical vertex approximation, Phys. Rev. B 103, 035120 (2021)

  12. [13]

    Cunningham, Many-body vertex effects: Time- dependent interaction kernel with correlated multiexci- tons in the bethe-salpeter equation, Phys

    B. Cunningham, Many-body vertex effects: Time- dependent interaction kernel with correlated multiexci- tons in the bethe-salpeter equation, Phys. Rev. B 112, 115153 (2025)

  13. [14]

    J. Zang, M. Medvidovi´ c, D. Kiese, D. Di Sante, A. M. Sengupta, and A. J. Millis, Machine learning-based com- pression of quantum many body physics: Pca and au- toencoder representation of the vertex function, Machine Learning: Science and Technology 5, 045076 (2024)

  14. [15]

    T. P. Devereaux, M. Claassen, X.-X. Huang, M. Zaletel, 6 J. E. Moore, D. Morr, F. Mahmood, P. Abbamonte, and Z.-X. Shen, Angle-resolved pair photoemission theory for correlated electrons, Phys. Rev. B 108, 165134 (2023)

  15. [16]

    Su and C

    Y. Su and C. Zhang, Coincidence angle-resolved pho- toemission spectroscopy: Proposal for detection of two- particle correlations, Phys. Rev. B 101, 205110 (2020)

  16. [17]

    Fresch, F

    E. Fresch, F. V. Camargo, Q. Shen, C. C. Bellora, T. Pullerits, G. S. Engel, G. Cerullo, and E. Collini, Two-dimensional electronic spectroscopy, Nature Re- views Methods Primers 3, 84 (2023)

  17. [18]

    K. S. Dy and C. J. Pethick, Transport coefficients of a normal fermi liquid: Application to liquid he 3, Phys. Rev. 185, 373 (1969)

  18. [19]

    A. H. MacDonald and D. J. W. Geldart, Electron- electron scattering and the thermal resistivity of sim- ple metals, Journal of Physics F: Metal Physics 10, 677 (1980)

  19. [20]

    C. A. Kukkonen and A. W. Overhauser, Electron- electron interaction in simple metals, Phys. Rev. B 20, 550 (1979)

  20. [21]

    J. G. Cook, M. P. V. d. Meer, and M. J. Laubitz, Ther- mal and electrical conductivities of sodium from 40 to 360 k, Canadian Journal of Physics 50, 1386 (1972), https://doi.org/10.1139/p72-190

  21. [22]

    M. J. Laubitz and J. G. Cook, High-temperature thermal resistivity of the polyvalent metals al and pb, Phys. Rev. B 7, 2867 (1973)

  22. [23]

    J. G. Cook, Electron–electron scattering in potas- sium, Canadian Journal of Physics 57, 1216 (1979), https://doi.org/10.1139/p79-170

  23. [24]

    Uher, Thermal conductivity of metals, in Ther- mal Conductivity: Theory, Properties, and Applications , edited by T

    C. Uher, Thermal conductivity of metals, in Ther- mal Conductivity: Theory, Properties, and Applications , edited by T. M. Tritt (Springer US, Boston, MA, 2004) pp. 21–91

  24. [25]

    B. Levy, M. Sinvani, and A. J. Greenfield, Sample depen- dence of the electron-electron contribution to the electri- cal resistivity of sodium and potassium, Phys. Rev. Lett. 43, 1822 (1979)

  25. [26]

    van Kempen, J

    H. van Kempen, J. H. J. M. Ribot, and P. Wyder, The electrical resistivity of potassium at low temperatures, Journal of Physics F: Metal Physics 11, 597 (1981)

  26. [27]

    N. R. Shaffer and C. E. Starrett, Model of electron trans- port in dense plasmas spanning temperature regimes, Phys. Rev. E 101, 053204 (2020)

  27. [28]

    Lindhard, On the properties of a gas of charged par- ticles, Kgl

    J. Lindhard, On the properties of a gas of charged par- ticles, Kgl. Danske Videnskab. Selskab Mat.-Fys. Medd. 28 (1954)

  28. [29]

    C. A. Kukkonen and J. W. Wilkins, Electron-electron scattering in simple metals, Phys. Rev. B 19, 6075 (1979)

  29. [30]

    Chen and K

    K. Chen and K. Haule, A combined variational and dia- grammatic quantum monte carlo approach to the many- electron problem, Nature communications 10, 1 (2019)

  30. [31]

    Haule and K

    K. Haule and K. Chen, Single-particle excitations in the uniform electron gas by diagrammatic monte carlo, Sci- entific reports 12, 2294 (2022)

  31. [32]

    N. V. Prokof’ev and B. V. Svistunov, Polaron problem by diagrammatic quantum monte carlo, Phys. Rev. Lett. 81, 2514 (1998)

  32. [33]

    Prokof’ev and B

    N. Prokof’ev and B. Svistunov, Fermi-polaron problem: Diagrammatic monte carlo method for divergent sign- alternating series, Phys. Rev. B 77, 020408(R) (2008)

  33. [34]

    Kozik, M

    E. Kozik, M. Ferrero, and A. Georges, Nonexistence of the luttinger-ward functional and misleading convergence of skeleton diagrammatic series for hubbard-like models, Phys. Rev. Lett. 114, 156402 (2015)

  34. [35]

    Rossi, Determinant diagrammatic monte carlo algo- rithm in the thermodynamic limit, Phys

    R. Rossi, Determinant diagrammatic monte carlo algo- rithm in the thermodynamic limit, Phys. Rev. Lett. 119, 045701 (2017)

  35. [36]

    Prokof’ev and B

    N. Prokof’ev and B. Svistunov, Bold diagrammatic monte carlo technique: When the sign problem is wel- come, Phys. Rev. Lett. 99, 250201 (2007)

  36. [37]

    Rossi, T

    R. Rossi, T. Ohgoe, K. Van Houcke, and F. Werner, Re- summation of diagrammatic series with zero convergence radius for strongly correlated fermions, Phys. Rev. Lett. 121, 130405 (2018)

  37. [38]

    Van Houcke, F

    K. Van Houcke, F. Werner, E. Kozik, N. V. Prokof’ev, B. V. Svistunov, M. Ku, A. Sommer, L. Cheuk, A. Schi- rotzek, and M. Zwierlein, Feynman diagrams versus fermi-gas feynman emulator, Nature Physics 8, 366 (2012)

  38. [39]

    Brolli, C

    S. Brolli, C. Barbieri, and E. Vigezzi, Diagrammatic monte carlo for finite systems at zero temperature, Phys. Rev. Lett. 134, 182502 (2025)

  39. [40]

    Wang and K

    Y. Wang and K. Haule, Variational diagrammatic monte carlo built on dynamical mean-field theory, Phys. Rev. Lett. 135, 176501 (2025)

  40. [42]

    Z. Li, P. Hou, Y. Deng, and K. Chen, Matsubara- frequency-resolved spin exchange-correlation kernel for the three-dimensional uniform electron gas, Phys. Rev. B 111, 155132 (2025)

  41. [43]

    Hou, B.-Z

    P.-C. Hou, B.-Z. Wang, K. Haule, Y. Deng, and K. Chen, Exchange-correlation effect in the charge response of a warm dense electron gas, Phys. Rev. B 106, L081126 (2022)

  42. [44]

    Chen, Partial renormalization of quasiparticle inter- actions (2024), arXiv:2404.15844 [cond-mat.str-el]

    K. Chen, Partial renormalization of quasiparticle inter- actions (2024), arXiv:2404.15844 [cond-mat.str-el]

  43. [45]

    Takada, Quasiparticle properties of the electron gas at metallic densities in the effective-potential expansion method, Phys

    Y. Takada, Quasiparticle properties of the electron gas at metallic densities in the effective-potential expansion method, Phys. Rev. B 43, 5979 (1991)

  44. [46]

    Matsuda, K

    K. Matsuda, K. Tamura, and M. Inui, Instability of the electron gas in an expanding metal, Phys. Rev. Lett. 98, 096401 (2007)

  45. [47]

    Takayanagi and E

    K. Takayanagi and E. Lipparini, Ghost plasmon and neg- ative dielectric function, Phys. Rev. B 56, 4872 (1997)

  46. [48]

    J. P. Perdew and Y. Wang, Accurate and simple ana- lytic representation of the electron-gas correlation energy, Phys. Rev. B 45, 13244 (1992)

  47. [49]

    Silin, Theory of a degenerate electron liquid, Sov

    V. Silin, Theory of a degenerate electron liquid, Sov. Phys. JETP-USSR 6, 387 (1958)

  48. [50]

    Silin, On the theory of the anomalous skin effect in metals, Soviet Physics JETP 6, 33 (1958)

    V. Silin, On the theory of the anomalous skin effect in metals, Soviet Physics JETP 6, 33 (1958)

  49. [51]

    Pseudo-Quantum Criticality in Electron Liquids Exhibited in Expanded Alkali Metals

    H. Maebashi and Y. Takada, Pseudo-quantum criticality in electron liquids exhibited in expanded alkali metals (2007), arXiv:0706.4001 [cond-mat.other]

  50. [52]

    IV in the supplemental material with our numerical results of the density response function and the ion-ion interaction

    A further discussion of this crossover phenomenon will be discussed in Sec. IV in the supplemental material with our numerical results of the density response function and the ion-ion interaction

  51. [53]

    Takada, Low-energy peak in the one-particle spectral function of the electron gas at metallic densities, Phys

    Y. Takada, Low-energy peak in the one-particle spectral function of the electron gas at metallic densities, Phys. Rev. B 110, 085132 (2024)

  52. [54]

    Holzmann, B

    M. Holzmann, B. Bernu, V. Olevano, R. M. Martin, and D. M. Ceperley, Renormalization factor and effective 7 mass of the two-dimensional electron gas, Phys. Rev. B 79, 041308 (2009)

  53. [55]

    X. Cai, T. Wang, N. V. Prokof’ev, B. V. Svistunov, and K. Chen, Superconductivity in the uniform electron gas: Irrelevance of the kohn-luttinger mechanism, Phys. Rev. B 106, L220502 (2022)

  54. [56]

    Hammer and R

    H.-W. Hammer and R. Furnstahl, Effective field theory for dilute fermi systems, Nuclear Physics A 678, 277 (2000)

  55. [57]

    Wellenhofer, C

    C. Wellenhofer, C. Drischler, and A. Schwenk, Dilute fermi gas at fourth order in effective field theory, Physics Letters B 802, 135247 (2020)

  56. [58]

    H. H. Jensen, H. Smith, and J. W. Wilkins, Upper and lower bounds on transport coefficients arising from a lin- earized boltzmann equation, Phys. Rev. 185, 323 (1969)

  57. [59]

    Kittel and P

    C. Kittel and P. McEuen, Introduction to solid state physics (John Wiley & Sons, 2018)

  58. [60]

    SVI in the supplemental material

    See Sec. SVI in the supplemental material

  59. [61]

    Koskelo, L

    J. Koskelo, L. Reining, and M. Gatti, Short-range exci- tonic phenomena in low-density metals, Phys. Rev. Lett. 134, 046402 (2025). Supplemental Material SI. V ARIA TIONAL DIAGRAMMA TIC MONTE CARLO METHOD AND CONVER GENCE ANAL YSIS In this section, we provide the theoretical foundation and technical details of the Variational Diagrammatic Monte Carlo (VDM...

  60. [62]

    (S19) This effective interaction also share the same structure of the charge -based Kukkonen-Overhauser interaction derived from the linear response theory [13]. SIV. CROSSOVER OF THE COULOMB SCREENING EFFECT In this section, we provide further details on the density-driv en crossover of the Coulomb screening effect discussed in the main text. To visualize ...

  61. [63]

    S4 constitut es the basis of the sKO + ansatz employed in the main text

    This derived correction term δR with its relevant parameters shown in the inset of Fig. S4 constitut es the basis of the sKO + ansatz employed in the main text. (0,0) (0,1) (1,1) (0,2) (1,2) (2,2) (l, k) −0.3 −0.2 −0.1 0.0 0.1 0.2 δAσσ ′ lk σσ ′ − rs ↑↑ −1.0 ↑↓ ↑↑ −5.0 ↑↓ 1 2 3 4 5rs −0.2 −0.1 0.0 0.1 0.2 0.3 C0 C2k2 F C′ 2k2 F FIG. S4: General polynomial...

  62. [64]

    cosθ], (S30) asp ↑↓ (θ,ϕ ) = cosϕ 2N ∗ F [(As 0 +Aa

  63. [65]

    cosθ] +As 0 − 3Aa 0 + 3(As 1 − 3Aa

  64. [66]

    cosθ (S31) where As,a l = F s,a l 1+F s,a l can be derived from the Landau parameter

  65. [67]

    Van Houcke, I

    K. Van Houcke, I. S. Tupitsyn, and N. V. Prokof’ev, Diagramma tic monte carlo and gw approximation for jellium and hydrogen chain, in Handbook of Materials Modeling , edited by W. Andreoni and S. Yip (Springer International Publi shing, Cham, 2020) pp. 435–452

  66. [68]

    Chen and K

    K. Chen and K. Haule, Nature communications 10, 1 (2019)

  67. [69]

    Haule and K

    K. Haule and K. Chen, Scientific reports 12, 2294 (2022)

  68. [70]

    P. Hou, T. Wang, D. Cerkoney, X. Cai, Z. Li, Y. Deng, L. Wang, an d K. Chen, An ai-powered technology stack for solving many-electron field theory (2025), arXiv:2403.18840 [hep-th]

  69. [71]

    Rossi, F

    R. Rossi, F. Werner, N. Prokof’ev, and B. Svistunov, Phys. Re v. B 93, 161102 (2016)

  70. [72]

    M. E. Peskin, An introduction to quantum field theory (CRC press, 2018)

  71. [73]

    Eliashberg, Sov

    G. Eliashberg, Sov. Phys. JETP 14, 886 (1962)

  72. [74]

    Landau, Sov

    L. Landau, Sov. Phys. JETP 8, 70 (1959)

  73. [75]

    A. J. Leggett, Phys. Rev. 140, A1869 (1965)

  74. [76]

    A. A. Abrikosov, L. P. Gorkov, and I. E. Dzyaloshinski, Methods of quantum field theory in statistical physics (Courier Corporation, 2012)

  75. [77]

    Silin, Sov

    V. Silin, Sov. Phys. JETP-USSR 6, 387 (1958)

  76. [78]

    Silin, Soviet Physics JETP 6, 33 (1958)

    V. Silin, Soviet Physics JETP 6, 33 (1958)

  77. [79]

    C. A. Kukkonen and A. W. Overhauser, Phys. Rev. B 20, 550 (1979)

  78. [80]

    Moroni, D

    S. Moroni, D. M. Ceperley, and G. Senatore, Phys. Rev. Lett. 75, 689 (1995)

  79. [81]

    Pfitzner, Journal of low temperature physics 61, 141 (1985)

    M. Pfitzner, Journal of low temperature physics 61, 141 (1985)

  80. [82]

    Hammer and R

    H.-W. Hammer and R. Furnstahl, Nuclear Physics A 678, 277 (2000)

Showing first 80 references.