Comment on "Electric conductivity of graphene: Kubo model versus a nonlocal quantum field theory model (arXiv:2403.02279v3)"
Pith reviewed 2026-05-22 00:37 UTC · model grok-4.3
The pith
A modification reconciling Kubo and quantum field theory conductivity in graphene violates gauge invariance.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The modification of the equality relating the conductivity and polarization expressions violates the requirement of gauge invariance and is therefore unacceptable. All results obtained within quantum field theory are physically well justified, whereas an application of the modified expression for the conductivity of graphene leads to the consequences of nonphysical character.
What carries the argument
Gauge invariance, the symmetry that any valid conductivity expression for graphene must preserve exactly.
If this is right
- Quantum field theory descriptions of graphene conductivity remain valid in both local and nonlocal regimes without needing adjustment.
- The modified conductivity expressions yield nonphysical predictions that conflict with fundamental symmetries.
- Direct comparisons between Kubo and quantum field theory models must retain the original relation between conductivity and polarization tensor.
Where Pith is reading between the lines
- Gauge invariance checks could serve as a quick test for proposed adjustments to conductivity formulas in other two-dimensional materials.
- Reconciling the two models may require revisiting the definition of conductivity itself rather than altering the polarization relation.
Load-bearing premise
Any valid expression for conductivity in graphene must preserve gauge invariance exactly.
What would settle it
A calculation or measurement showing that the modified conductivity formula produces observable nonphysical effects, such as violation of current conservation or unphysical response to electromagnetic fields, that the unmodified quantum field theory formula does not.
read the original abstract
Recently, Rodriguez-Lopez, Wang, and Antezza [Phys. Rev. B v.111, 115428 (2025)] compared the theoretical descriptions of electric conductivity of graphene given by the Kubo model and quantum field theory in terms of the polarization tensor. According to this article, in the spatially nonlocal case, the quantum field theoretical description contains ``hard inconsistencies". By modifying the equality, which relates the conductivity and polarization expressions, the predictions of quantum field theory were revised and brought in agreement with those following from the nonrelativistic Kubo model. Here, it is shown that this modification violates the requirement of gauge invariance and, thus, is unacceptable. By comparing both theoretical approaches, we demonstrate that all the results obtained within quantum field theory are physically well justified whereas an application of the modified expression for the conductivity of graphene leads to the consequences of nonphysical character.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This manuscript is a comment on Rodriguez-Lopez, Wang, and Antezza (Phys. Rev. B 111, 115428, 2025). It argues that the modification they proposed to the relation equating conductivity and polarization expressions in the spatially nonlocal regime violates the gauge-invariance requirement of quantum field theory. The authors compare the Kubo and QFT approaches and conclude that the original QFT results remain physically justified while the modified expressions produce nonphysical consequences.
Significance. If the central argument holds, the comment is significant for the mesoscopic physics of graphene because it upholds a standard symmetry principle that must be preserved in electromagnetic response functions. The work merits explicit credit for invoking gauge invariance without introducing free parameters, ad-hoc adjustments, or circular self-references, thereby providing a clean, falsifiable test of model validity.
minor comments (1)
- Abstract: the phrase 'consequences of nonphysical character' is vague; a single concrete example (e.g., a sign change in a response function or violation of a sum rule) would improve immediate readability.
Simulated Author's Rebuttal
We thank the referee for the careful reading of our manuscript, the positive assessment of its significance, and the recommendation to accept. The referee's summary correctly identifies the central claim that the proposed modification to the conductivity-polarization relation violates gauge invariance.
Circularity Check
No significant circularity
full rationale
The paper's central claim rests on the external, standard requirement of gauge invariance in electromagnetic response functions, which is invoked to reject the proposed modification to the conductivity-polarization relation. This principle is not constructed from the paper's own inputs, fitted parameters, or self-citations; it is a pre-existing symmetry constraint from QED. The comparison between the Kubo model and QFT polarization tensor is presented as revealing nonphysical consequences in the modified case, without any step that reduces by definition or statistical forcing to the paper's own assumptions. No self-definitional loops, ansatz smuggling, or renaming of known results occur. The derivation chain is therefore independent and self-contained against external physical benchmarks.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Gauge invariance must be preserved in any physically acceptable expression relating conductivity to the polarization tensor.
Reference graph
Works this paper leans on
-
[1]
P. Rodriguez-Lopez, J.-S. Wang, and M. Antezza, Electric con- ductivity in graphene: Kubo model versus a nonlocal quan- tum field theory model, arXiv:2403.02279v3; Phys. Rev. B111, 115428 (2025)
-
[2]
G. L. Klimchitskaya and V . M. Mostepanenko, Conductivity of pure graphene: Theoretical approach using the polarization tensor, Phys. Rev. B93, 245419 (2016)
work page 2016
-
[3]
G. L. Klimchitskaya and V . M. Mostepanenko, Quantum elec- trodynamic approach to the conductivity of gapped graphene, Phys. Rev. B 94, 195405 (2016)
work page 2016
-
[4]
G. L. Klimchitskaya, V . M. Mostepanenko, and V . M. Petrov, Conductivity of graphene in the framework of Dirac model: Interplay between nonzero mass gap and chemical potential, Phys. Rev. B 96, 235432 (2017)
work page 2017
-
[5]
G. L. Klimchitskaya and V . M. Mostepanenko, Kramers-Kronig relations and causality conditions for graphene in the frame- work of the Dirac model, Phys. Rev. D 97, 085001 (2018)
work page 2018
- [6]
-
[7]
I. V . Fialkovsky, V . N. Marachevsky, and D. V . Vassilevich, Finite-temperature Casimir e ffect for graphene, Phys. Rev. B 84, 035446 (2011)
work page 2011
- [8]
- [9]
-
[10]
I. V Fialkovskiy and D. V . Vassilevich, Quantum field theory in graphene, Int. J. Mod. Phys. A 27, 1260007 (2012)
work page 2012
-
[11]
I. V . Fialkovskiy and D. V . Vassilevich, Graphene through the looking glass of QFT, Mod. Phys. Lett. A 31, 1630047 (2016)
work page 2016
-
[12]
G. L. Klimchitskaya and V . M. Mostepanenko, Quantum field theoretical framework for the electromagnetic response of graphene and dispersion relations with implications to the Casimir effect, Phys. Rev. D 107, 105007 (2023)
work page 2023
- [13]
-
[14]
N. Khusnutdinov and D. V . Vassilevich, Impurities in graphene and their influence on the Casimir interaction, Phys. Rev. B109, 235420 (2024)
work page 2024
-
[15]
N. Khusnutdinov and N. Emelianova, The polarization tensor approach for Casimir effect, Int. J. Mod. Phys. A 40, 2543004 (2025)
work page 2025
-
[16]
P. K. Pyatkovsky, Dynamic polarization, screening, and plas- mons in gapped graphene, J. Phys.: Condens. Matter 21, 025506 (2009)
work page 2009
-
[17]
G. L. Klimchitskaya and V . M. Mostepanenko, Casimir and Casimir-Polder Forces in Graphene Systems: Quantum Field Theoretical Description and Thermodynamics, Universe 6, 150 (2020)
work page 2020
-
[18]
V . P. Gusynin, S. G. Sharapov, and J. P. Carbotte, Magnetoop- tical conductivity in graphene, J. Phys.: Condens. Matter 19, 026222 (2007)
work page 2007
-
[19]
L. D. Landau and E. M. Lifshitz, The Classical Theory of Fields (Elsevier, Amsterdam, 1980)
work page 1980
-
[20]
G. L. Klimchitskaya, C. C. Korikov, and V . M. Mostepa- nenko, Polarization tensor in spacetime of three dimensions and a quantum field-theoretical description of the nonequilibrium Casimir force in graphene systems, Phys. Rev. A 111, 012812 (2025)
work page 2025
-
[21]
L. D. Landau, E. M. Lifshitz, and L. P. Pitaevskii, L.P. Electro- dynamics of Continuous Media (Pergamon, Oxford, 1984)
work page 1984
-
[22]
L. A. Falkovsky and A. A. Varlamov, Space-time dispersion of graphene conductivity, Eur. Phys. J. B56, 281 (2007)
work page 2007
-
[23]
M. I. Katsnelson, The Physics of Graphene (Cambridge Uni- versity Press, Cambridge, 2020)
work page 2020
-
[24]
G ´omez-Santos, Thermal van der Waals interaction between graphene layers, Phys
G. G ´omez-Santos, Thermal van der Waals interaction between graphene layers, Phys. Rev. B 80, 245424 (2009)
work page 2009
-
[25]
M. Liu, Y . Zhang, G. L. Klimchitskaya, V . M. Mostepanenko, and U. Mohideen, Demonstration of an Unusual Thermal Ef- fect in the Casimir Force from Graphene, Phys. Rev. Lett. 126, 206802 (2021)
work page 2021
-
[26]
M. Liu, Y . Zhang, G. L. Klimchitskaya, V . M. Mostepanenko, and U. Mohideen, Experimental and theoretical investigation of the thermal effect in the Casimir interaction from graphene, Phys. Rev. B 104, 085436 (2021)
work page 2021
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.