Topological piezomagnetic effect in two-dimensional Dirac quadrupole altermagnets
Pith reviewed 2026-05-16 06:49 UTC · model grok-4.3
The pith
Dirac quadrupole altermagnets in two dimensions display a topological contribution to their orbital piezomagnetic polarizability.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The orbital piezomagnetic polarizability of Dirac quadrupole altermagnets possesses a topological contribution that is a direct consequence of strain acting on the quadrupole of Dirac points inherited from the parent semimetal phase.
What carries the argument
The quadrupole formed by Dirac points in momentum space, whose strain-induced distortion generates the topological piezomagnetic response via topological response theory.
Load-bearing premise
The essential low-energy electronic structure of these altermagnets is captured by the gapless Dirac quadrupole semimetal parent phase and by the two chosen minimal models.
What would settle it
Measurement of a nonzero topological contribution to the piezomagnetic coefficient in a candidate 2D material realizing the Lieb lattice with collinear Néel order under applied strain.
Figures
read the original abstract
Altermagnets provide a natural platform for studying and exploiting piezomagnetism. In this paper, we introduce a class of insulating altermagnets in two dimensions (2D) referred to as Dirac quadrupole altermagnets, and show based on microscopic minimal models that the orbital piezomagnetic polarizability of such altermagnets has a topological contribution described by topological response theory. The essential low-energy electronic structure of Dirac quadrupole altermagnets can be understood from a gapless parent phase (i.e., the Dirac quadrupole semimetal), which has important implications for their response to external fields. Focusing on the strain-induced response, here we demonstrate that the topological piezomagnetic effect is a consequence of the way in which strain affects the Dirac points forming a quadrupole. We consider two microscopic models: a spinless two-band model describing a band inversion of $s$ and $d$ states, and a Lieb lattice model with collinear N\'eel order. The latter is a prototypical minimal model for altermagnetism in 2D and is realized in a number of recently proposed material compounds, which are discussed.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper introduces Dirac quadrupole altermagnets as a class of 2D insulating altermagnets and demonstrates via two minimal models (spinless two-band s-d inversion and Lieb lattice with collinear Néel order) that the orbital piezomagnetic polarizability receives a topological contribution arising from the strain response of Dirac points in the gapless parent Dirac quadrupole semimetal phase, as derived from topological response theory.
Significance. If the central claim holds, the work provides a topological mechanism for strain-tunable piezomagnetism in altermagnets, connecting altermagnetic order to response theory in 2D systems and highlighting implications for proposed material compounds. The explicit minimal-model derivations and focus on the gapless parent phase constitute a clear theoretical advance.
major comments (2)
- [Models and abstract] The central claim that the topological contribution is robust rests on the assumption that the two minimal models capture the essential low-energy Dirac quadrupole physics without extraneous bands or interactions modifying the strain response; the manuscript should explicitly demonstrate (e.g., via symmetry analysis or band-structure comparison) that higher-order lattice effects or additional bands do not cancel the quadrupole-derived term.
- [Strain-induced response section] The derivation applies topological response theory to strain-modified Dirac points, but the abstract and main text provide no numerical evaluation, error estimates, or magnitude comparison between the topological term and possible non-topological contributions, leaving the quantitative strength of the effect untested within the models themselves.
minor comments (1)
- [Discussion] Add a brief table or paragraph comparing the symmetry-allowed strain couplings in the Lieb lattice model to those expected in the recently proposed material compounds mentioned in the abstract.
Simulated Author's Rebuttal
We thank the referee for the positive assessment of our work and the constructive comments. We address each major point below and will revise the manuscript accordingly to strengthen the presentation of the topological piezomagnetic effect.
read point-by-point responses
-
Referee: [Models and abstract] The central claim that the topological contribution is robust rests on the assumption that the two minimal models capture the essential low-energy Dirac quadrupole physics without extraneous bands or interactions modifying the strain response; the manuscript should explicitly demonstrate (e.g., via symmetry analysis or band-structure comparison) that higher-order lattice effects or additional bands do not cancel the quadrupole-derived term.
Authors: We agree that an explicit demonstration of robustness is valuable. The two minimal models are constructed to isolate the low-energy Dirac quadrupole physics protected by the altermagnetic symmetries. In the revised manuscript, we will add a dedicated symmetry analysis subsection showing that the topological orbital piezomagnetic polarizability is dictated by the quadrupole Dirac points and remains invariant under perturbations that preserve the relevant symmetries (e.g., C4 rotation combined with spin rotation). We will also provide a band-structure comparison between the minimal models and an extended Lieb lattice with next-nearest-neighbor hoppings, confirming that additional bands do not cancel the strain-induced topological term at low energy. revision: yes
-
Referee: [Strain-induced response section] The derivation applies topological response theory to strain-modified Dirac points, but the abstract and main text provide no numerical evaluation, error estimates, or magnitude comparison between the topological term and possible non-topological contributions, leaving the quantitative strength of the effect untested within the models themselves.
Authors: We acknowledge that quantitative benchmarks would better illustrate the dominance of the topological contribution. In the revised version, we will add numerical evaluations of the orbital piezomagnetic polarizability for both models. These will include direct computation of the full response tensor under strain, separation into topological and non-topological parts, and error estimates arising from finite-size effects or cutoff in the Brillouin zone integration. We will also compare magnitudes, showing that the topological term from the Dirac points accounts for the leading contribution in the low-strain regime. revision: yes
Circularity Check
Derivation applies standard topological response theory to minimal models without circular reduction
full rationale
The paper constructs two explicit microscopic minimal models (spinless s-d band-inversion and Lieb lattice with Néel order) from the gapless Dirac quadrupole semimetal parent phase, then applies standard topological response theory to the strain-induced shift of the Dirac points to obtain the orbital piezomagnetic polarizability. No parameter is fitted to the target response and then relabeled as a prediction; the topological term emerges directly from the response formalism applied to the model Hamiltonians. The derivation chain is therefore self-contained and does not reduce to self-definition, fitted-input renaming, or load-bearing self-citation.
Axiom & Free-Parameter Ledger
free parameters (1)
- strain coupling strength
axioms (1)
- domain assumption The low-energy electronic structure is captured by the gapless Dirac quadrupole semimetal parent phase.
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
we introduce a class of insulating altermagnets in two dimensions (2D) referred to as Dirac quadrupole altermagnets... orbital piezomagnetic polarizability... topological contribution described by topological response theory
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.
Reference graph
Works this paper leans on
-
[1]
R. B. Laughlin, Phys. Rev. B23, 5632 (1981)
work page 1981
-
[2]
B. I. Halperin, Phys. Rev. B25, 2185 (1982)
work page 1982
-
[3]
D. J. Thouless, M. Kohmoto, M. P. Nightingale, and M. d. Nijs, Phys. Rev. Lett.49, 405 (1982)
work page 1982
-
[4]
F. D. M. Haldane, Phys. Rev. Lett.61, 2015 (1988)
work page 2015
-
[5]
X.-L. Qi, T. L. Hughes, and S.-C. Zhang, Phys. Rev. B 78, 195424 (2008)
work page 2008
-
[6]
A. M. Essin, J. E. Moore, and D. Vanderbilt, Phys. Rev. Lett.102, 146805 (2009)
work page 2009
-
[7]
R. Li, J. Wang, X.-L. Qi, and S.-C. Zhang, Nat. Phys. 6, 284 (2010)
work page 2010
- [8]
- [9]
- [10]
-
[11]
F. D. M. Haldane, Phys. Rev. Lett.93, 206602 (2004)
work page 2004
-
[12]
B. A. Bernevig, T. L. Hughes, S. Raghu, and D. P. Arovas, Phys. Rev. Lett.99, 146804 (2007)
work page 2007
-
[13]
T. L. Hughes, E. Prodan, and B. A. Bernevig, Phys. Rev. B83, 245132 (2011)
work page 2011
- [14]
-
[15]
S. T. Ramamurthy and T. L. Hughes, Phys. Rev. B92, 085105 (2015)
work page 2015
-
[16]
S. T. Ramamurthy, Y. Wang, and T. L. Hughes, Phys. Rev. Lett.118, 146602 (2017)
work page 2017
-
[17]
F. d. Juan, A. G. Grushin, T. Morimoto, and J. E. Moore, Nat. Commun.8, 15995 (2017)
work page 2017
-
[18]
N. R. Cooper, B. I. Halperin, and I. M. Ruzin, Phys. Rev. B55, 2344 (1997). 6
work page 1997
- [19]
-
[20]
S. Ryu, J. E. Moore, and A. W. W. Ludwig, Phys. Rev. B85, 045104 (2012)
work page 2012
- [21]
- [22]
- [23]
-
[24]
J. E. Avron, R. Seiler, and P. G. Zograf, Phys. Rev. Lett. 75, 697 (1995)
work page 1995
- [25]
-
[26]
T. L. Hughes, R. G. Leigh, and E. Fradkin, Phys. Rev. Lett.107, 075502 (2011)
work page 2011
-
[27]
T. L. Hughes, R. G. Leigh, and O. Parrikar, Phys. Rev. D88, 025040 (2013)
work page 2013
-
[28]
O. Parrikar, T. L. Hughes, and R. G. Leigh, Phys. Rev. D90, 105004 (2014)
work page 2014
-
[29]
Y. You, G. Y. Cho, and T. L. Hughes, Phys. Rev. B94, 085102 (2016)
work page 2016
- [30]
-
[31]
J. C. Y. Teo and T. L. Hughes, Annu. Rev. Condens. Matter Phys.8, 1 (2016)
work page 2016
- [32]
-
[33]
M. R. Hirsbrunner, O. Dubinkin, F. J. Burnell, and T. L. Hughes, Phys. Rev. X14, 041060 (2024)
work page 2024
- [34]
- [35]
- [36]
- [37]
-
[38]
I. I. Mazin, K. Koepernik, M. D. Johannes, R. Gonz´ alez- Hern´ andez, and L.ˇSmejkal, Proceedings of the National Academy of Sciences118, e2108924118 (2021)
work page 2021
-
[39]
C. Song, H. Bai, Z. Zhou, L. Han, H. Reichlova, J. H. Dil, J. Liu, X. Chen, and F. Pan, Nat. Rev. Mater.10, 473 (2025)
work page 2025
-
[40]
T. Jungwirth, R. M. Fernandes, E. Fradkin, A. H. Mac- Donald, J. Sinova, and L. ˇSmejkal, Newton1, 100162 (2025)
work page 2025
-
[41]
T. Jungwirth, J. Sinova, R. M. Fernandes, Q. Liu, H. Watanabe, S. Murakami, S. Nakatsuji, and L. ˇSmejkal, Nature649, 837 (2026)
work page 2026
- [42]
-
[43]
H. Bai, Y. C. Zhang, Y. J. Zhou, P. Chen, C. H. Wan, L. Han, W. X. Zhu, S. X. Liang, Y. C. Su, X. F. Han, F. Pan, and C. Song, Phys. Rev. Lett.130, 216701 (2023)
work page 2023
-
[44]
L.-D. Yuan, Z. Wang, J.-W. Luo, and A. Zunger, Phys. Rev. Materials5, 014409 (2021)
work page 2021
- [45]
-
[46]
S. A. Egorov and R. A. Evarestov, The J. Phys. Chem. Letters12, 2363 (2021)
work page 2021
-
[47]
Y. Guo, H. Liu, O. Janson, I. C. Fulga, J. v. d. Brink, and J. I. Facio, Materials Today Physics32, 100991 (2023)
work page 2023
-
[48]
M. Naka, S. Hayami, H. Kusunose, Y. Yanagi, Y. Mo- tome, and H. Seo, Nat. Commun.10, 4305 (2019)
work page 2019
- [49]
- [50]
-
[51]
Gonz´ alez-Hern´ andez, L.ˇSmejkal, K
R. Gonz´ alez-Hern´ andez, L.ˇSmejkal, K. V´ yborn´ y, Y. Ya- hagi, J. Sinova, T. Jungwirth, and J. ˇZelezn´ y, Phys. Rev. Lett.126, 127701 (2021)
work page 2021
-
[52]
M. Naka, Y. Motome, and H. Seo, Phys. Rev. B103, 125114 (2021)
work page 2021
-
[53]
D.-F. Shao, S.-H. Zhang, M. Li, C.-B. Eom, and E. Y. Tsymbal, Nat. Commun.12, 7061 (2021)
work page 2021
-
[54]
H.-Y. Ma, M. Hu, N. Li, J. Liu, W. Yao, J.-F. Jia, and J. Liu, Nat. Commun.12, 2846 (2021)
work page 2021
-
[55]
A. Bose, N. J. Schreiber, R. Jain, D.-F. Shao, H. P. Nair, J. Sun, X. S. Zhang, D. A. Muller, E. Y. Tsymbal, D. G. Schlom, and D. C. Ralph, Nat. Electron.5, 267 (2022)
work page 2022
-
[56]
P. A. McClarty and J. G. Rau, Phys. Rev. Lett.132, 176702 (2024)
work page 2024
- [57]
-
[58]
C. R. W. Steward, R. M. Fernandes, and J. Schmalian, Phys. Rev. B108, 144418 (2023)
work page 2023
-
[59]
R. M. Fernandes, V. S. d. Carvalho, T. Birol, and R. G. Pereira, Phys. Rev. B109, 024404 (2024)
work page 2024
-
[60]
K. Takahashi, C. R. W. Steward, M. Ogata, R. M. Fer- nandes, and J. Schmalian, Phys. Rev. B111, 184408 (2025)
work page 2025
-
[61]
M. Naka, Y. Motome, T. Miyazaki, and H. Seo, J. Phys. Soc. Jpn.94, 083702 (2025)
work page 2025
-
[62]
M. Khodas, S. Mu, I. I. Mazin, and K. D. Belashchenko, arXiv (2025), 10.48550/arxiv.2506.06257
-
[63]
Phys. Rev. B112, 245115 (2025)
work page 2025
-
[64]
T. Thonhauser, D. Ceresoli, D. Vanderbilt, and R. Resta, Phys. Rev. Lett.95, 137205 (2005)
work page 2005
-
[65]
D. Xiao, J. Shi, and Q. Niu, Phys. Rev. Lett.95, 137204 (2005)
work page 2005
-
[66]
D. Ceresoli, T. Thonhauser, D. Vanderbilt, and R. Resta, Phys. Rev. B74, 024408 (2006)
work page 2006
-
[67]
J. Mitscherling, J. Priessnitz, and L. ˇSmejkal, arXiv (2025), 10.48550/arxiv.2512.09051
- [68]
-
[69]
D. S. Antonenko, R. M. Fernandes, and J. W. F. Vender- bos, Phys. Rev. Lett.134, 096703 (2025)
work page 2025
-
[70]
K. V. Yershov, V. P. Kravchuk, M. Daghofer, and J. v. d. Brink, Phys. Rev. B110, 144421 (2024)
work page 2024
- [71]
-
[72]
M. D¨ urrnagel, H. Hohmann, A. Maity, J. Seufert, M. Klett, L. Klebl, and R. Thomale, Phys. Rev. Lett. 135, 036502 (2025)
work page 2025
-
[73]
Z. Fu, M. Hu, A. Li, H. Duan, J. Liu, and F. Ouyang, arXiv (2025), 10.48550/arxiv.2507.22474
-
[74]
C.-C. Wei, X. Li, S. Hatt, X. Huai, J. Liu, B. Singh, K.-M. Kim, R. M. Fernandes, P. Cardon, L. Zhao, T. T. Tran, B. A. Frandsen, K. S. Burch, F. Liu, and H. Ji, Phys. Rev. Materials9, 024402 (2025)
work page 2025
-
[75]
P.-H. Chang, I. I. Mazin, and K. D. Belashchenko, arXiv (2025), 10.48550/arxiv.2508.04839
- [76]
- [77]
-
[78]
A. R. Chakraborty, F. Yang, T. Birol, and R. M. Fer- nandes, arXiv (2025), 10.48550/arxiv.2509.26596
-
[79]
M. Pan, F. Liu, and H. Huang, arXiv (2025), 10.48550/arxiv.2510.00509
-
[80]
Basic symmetry requirements suggest thatw y,k ≡0
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.