Nearly Complete Charge--Spin Conversion via Strain-Eliminated Fermi Pockets in d-Wave Altermagnets
Pith reviewed 2026-05-09 21:35 UTC · model grok-4.3
The pith
In-plane tensile strain eliminates residual elliptical Fermi pockets in d-wave altermagnets, driving charge-to-spin conversion efficiency up to 96% at 4% strain.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In d-wave altermagnets such as KV2Se2O, equibiaxial tensile strain systematically suppresses next-nearest-neighbor hoppings, eliminating parasitic elliptical Fermi pockets and restoring orthogonal flat Fermi surfaces, thereby increasing the charge-to-spin conversion efficiency from low values to approximately 96% at 4% strain. An effective tight-binding model confirms this evolution, and an unconventional out-of-plane spin current component emerges under tilted fields with nearly 55% CSE at optimal orientations.
What carries the argument
Strain-tuned reduction of next-nearest-neighbor hoppings that removes residual elliptical Fermi pockets and restores flat Fermi surfaces.
If this is right
- Charge-to-spin conversion efficiency rises monotonically with increasing in-plane tensile strain.
- Suppression of next-nearest-neighbor hoppings is the dominant process restoring high spin conductivity.
- Tilted electric fields generate an out-of-plane spin current component reaching nearly 55% conversion efficiency.
- Strain engineering provides a practical design route toward near-ideal spintronic devices in d-wave altermagnets.
Where Pith is reading between the lines
- The same strain-tuning principle could be examined in other metallic altermagnets to reach comparable efficiencies.
- The out-of-plane spin current may allow device geometries that avoid external magnetic fields for magnetization control.
- Angle-resolved photoemission spectroscopy performed under controlled strain would directly image the predicted pocket disappearance.
Load-bearing premise
The first-principles band structure and fitted tight-binding model stay accurate at 4% strain without new structural instabilities or correlation effects that would alter the Fermi pockets.
What would settle it
Direct measurement of the Fermi surface at 4% tensile strain that still shows elliptical pockets, or transport data that yields charge-to-spin conversion well below 90%, would disprove the predicted pocket-elimination mechanism.
Figures
read the original abstract
$d$-wave altermagnets possess nearly orthogonal flat Fermi surfaces, which in an idealized limit enable complete spin-channel separation and a theoretical charge-to-spin conversion efficiency (CSE) of 100%. The recently discovered metallic altermagnet $\mathrm{KV_2Se_2O}$ exemplifies this class, yet realistic samples host residual elliptical Fermi pockets that enhance charge conductivity while suppressing spin conductivity, drastically reducing the CSE. Here we show that in-plane equibiaxial tensile strain systematically eliminates these parasitic pockets, restoring the flat-band geometry. Our first-principles calculations reveal that the CSE increases monotonically with strain, reaching a record value of approximately 96% at 4% strain. An effective tight-binding model fitted to the computed band structure accurately captures the evolution of the Fermi surface and confirms that the suppression of the pockets -- governed by reduced next-nearest-neighbor hoppings -- is the dominant mechanism for the strain-enhanced CSE. We further identify an unconventional out-of-plane spin current component that emerges under tilted electric fields and achieves a CSE of nearly 55% at optimal orientations, offering a promising pathway for field-free perpendicular magnetization switching. Our findings establish strain engineering as a practical route to approach the ultimate conversion limit in $d$-wave altermagnets and provide a design principle for high-efficiency spintronic devices.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that equibiaxial tensile strain in the d-wave altermagnet KV2Se2O systematically eliminates residual elliptical Fermi pockets, causing the charge-to-spin conversion efficiency (CSE) to increase monotonically and reach ~96% at 4% strain. First-principles calculations are supplemented by a fitted effective tight-binding model that attributes the improvement to reduced next-nearest-neighbor hoppings; an unconventional out-of-plane spin-current component under tilted fields is also reported, reaching ~55% CSE at optimal orientations.
Significance. If the quantitative CSE values and Fermi-surface evolution prove robust, the work supplies a concrete strain-engineering route toward the theoretical 100% limit in d-wave altermagnets and identifies a field-free perpendicular-switching pathway. The combination of DFT band-structure results with a transparent TB analysis constitutes a clear mechanistic demonstration.
major comments (2)
- [Abstract and main results] Abstract and main results: the headline CSE value of ~96% at 4% equibiaxial tension rests on the assumption that the DFT Fermi surface remains free of pockets and that the conductivity tensors are unaltered by strain-induced structural changes. No phonon-dispersion, elastic-constant, or +U-sensitivity data under 4% tension are provided, leaving open the possibility that out-of-plane relaxation or buckling reintroduces pockets and invalidates the reported monotonic rise.
- [Tight-binding model section] Tight-binding model section: because the TB parameters are fitted directly to the strained DFT bands, the statement that pocket suppression is 'governed by reduced next-nearest-neighbor hoppings' is partly by construction. While the raw first-principles strain dependence is independent, the quantitative CSE numbers and the mechanistic attribution inherit the fitting step; an unfitted or parameter-free analysis would be required to confirm the dominance of this mechanism.
minor comments (2)
- [Results] No error bars or uncertainty estimates accompany the CSE percentages, and no direct comparison with available unstrained experimental transport data is presented.
- [Methods] Notation for the conductivity tensors and the definition of CSE should be stated explicitly in the main text rather than deferred to supplementary material.
Simulated Author's Rebuttal
We thank the referee for the positive evaluation of our work's significance and for providing detailed feedback. We respond to the major comments below and will incorporate revisions to address the valid concerns raised.
read point-by-point responses
-
Referee: Abstract and main results: the headline CSE value of ~96% at 4% equibiaxial tension rests on the assumption that the DFT Fermi surface remains free of pockets and that the conductivity tensors are unaltered by strain-induced structural changes. No phonon-dispersion, elastic-constant, or +U-sensitivity data under 4% tension are provided, leaving open the possibility that out-of-plane relaxation or buckling reintroduces pockets and invalidates the reported monotonic rise.
Authors: We agree that additional verification of structural stability under strain would enhance the reliability of our results. Our DFT calculations involve full relaxation of the out-of-plane lattice constant and atomic positions for each strained in-plane lattice. At 4% tension, the optimized geometry shows no evidence of buckling, and the Fermi surface from these DFT bands is free of the elliptical pockets. We will add phonon dispersion calculations demonstrating the absence of imaginary frequencies and the elastic constants for the strained unit cell in the revised supplementary information. We have also checked that the CSE trend is insensitive to moderate variations in the Hubbard U parameter. These revisions will confirm that the reported monotonic increase to ~96% CSE is robust against the concerns mentioned. revision: yes
-
Referee: Tight-binding model section: because the TB parameters are fitted directly to the strained DFT bands, the statement that pocket suppression is 'governed by reduced next-nearest-neighbor hoppings' is partly by construction. While the raw first-principles strain dependence is independent, the quantitative CSE numbers and the mechanistic attribution inherit the fitting step; an unfitted or parameter-free analysis would be required to confirm the dominance of this mechanism.
Authors: We concur that the TB model is fitted to the DFT data, making the mechanistic interpretation reliant on that fit. However, the CSE efficiency values are calculated exclusively from the first-principles DFT band structures and the associated conductivity tensors using the relaxation-time approximation in the Boltzmann transport framework; the TB model is not used for the quantitative CSE results. The TB fit is employed only to interpret why the pockets are suppressed. To provide a parameter-free confirmation of the mechanism, we will include an analysis based on Wannier function projections from the DFT calculations to extract the hopping parameters directly, without a global fit, showing the reduction in next-nearest-neighbor hoppings with increasing strain. This will be added to the revised manuscript. revision: partial
Circularity Check
TB fit to DFT bands renders mechanism confirmation tautological; main CSE result remains independent
specific steps
-
fitted input called prediction
[Abstract]
"An effective tight-binding model fitted to the computed band structure accurately captures the evolution of the Fermi surface and confirms that the suppression of the pockets -- governed by reduced next-nearest-neighbor hoppings -- is the dominant mechanism for the strain-enhanced CSE."
The model is explicitly fitted to the first-principles band structure; therefore its reproduction of the Fermi-surface evolution and its attribution of the effect to specific hopping terms are guaranteed by the fitting step rather than independently derived. This makes the 'confirmation' of the mechanism equivalent to the input data by construction.
full rationale
The central quantitative claim (CSE rising to ~96% at 4% strain) is stated as arising from first-principles calculations of the strained band structure and derived conductivities. The only load-bearing step that reduces to its inputs by construction is the subsequent fitting of an effective tight-binding model to those same bands, followed by using the fit parameters to 'confirm' that reduced next-nearest-neighbor hoppings suppress the pockets. This confirmation is statistically forced by the fitting procedure itself and does not constitute an independent derivation or prediction. No other patterns (self-citation chains, uniqueness theorems, or ansatz smuggling) appear in the provided text. The overall derivation chain therefore retains independent first-principles content for the headline result, warranting only a modest circularity score.
Axiom & Free-Parameter Ledger
free parameters (2)
- strain magnitude
- tight-binding hopping parameters
axioms (2)
- domain assumption Density-functional theory accurately captures the Fermi-surface evolution under strain
- domain assumption The effective tight-binding model reproduces the strain dependence of the pockets
Reference graph
Works this paper leans on
-
[1]
L. Šmejkal, R. González-Hernández, T. Jungwirth, and J. Sinova, Crystal time-reversal symmetry breaking and spon- taneous Hall effect in collinear antiferromagnets, Sci. Adv.6, eaaz8809 (2020)
work page 2020
-
[2]
Mazin, Editorial: Altermagnetism—A New Punch Line of Fundamental Magnetism, Phys
I. Mazin, Editorial: Altermagnetism—A New Punch Line of Fundamental Magnetism, Phys. Rev. X12, 040002 (2022)
work page 2022
-
[3]
L. Šmejkal, J. Sinova, and T. Jungwirth, Beyond Conventional Ferromagnetism and Antiferromagnetism: A Phase with Non- relativistic Spin and Crystal Rotation Symmetry, Phys. Rev. X 12, 031042 (2022)
work page 2022
-
[4]
L. Šmejkal, J. Sinova, and T. Jungwirth, Emerging Research LandscapeofAltermagnetism,Phys.Rev.X12,040501(2022)
work page 2022
-
[5]
L. Šmejkal, A. H. MacDonald, J. Sinova, S. Nakatsuji, and T. Jungwirth, Anomalous hall antiferromagnets, Nat. Rev. Mater.7, 482 (2022)
work page 2022
-
[6]
H.-Y. Ma, M. Hu, N. Li, J. Liu, W. Yao, J.-F. Jia, and J. Liu, Multifunctional antiferromagnetic materials with giant piezo- magnetism and noncollinear spin current, Nat. Commun.12, 2846 (2021)
work page 2021
-
[7]
J. Krempaský, L. Šmejkal, S. W. D’Souza, M. Hajlaoui, G. Springholz, K. Uhlířová, F. Alarab, P. C. Constantinou, V.Strocov,D.Usanov,W.R.Pudelko,R.González-Hernández, A. Birk Hellenes, Z. Jansa, H. Reichlová, Z. Šobáň, R. D. Gon- zalez Betancourt, P. Wadley, J. Sinova, D. Kriegner, J. Minár, J. H. Dil, and T. Jungwirth, Altermagnetic lifting of Kramers spi...
work page 2024
-
[8]
L.Bai,W.Feng,S.Liu,L.Šmejkal,Y.Mokrousov,andY.Yao, Altermagnetism: exploring new frontiers in magnetism and spintronics, Adv. Funct. Mater.34, 2409327 (2024)
work page 2024
-
[9]
P.Liu,J.Li,J.Han,X.Wan,andQ.Liu,Spin-GroupSymmetry in Magnetic Materials with Negligible Spin-Orbit Coupling, Phys. Rev. X12, 021016 (2022)
work page 2022
-
[10]
Y. Guo, H. Liu, O. Janson, I. C. Fulga, J. van den Brink, and J. I. Facio, Spin-split collinear antiferromagnets: A large-scale ab-initio study, Mater. Today Phys.32, 100991 (2023)
work page 2023
-
[11]
R. González-Hernández, L. Šmejkal, K. Výborný, Y. Yahagi, J. Sinova, T. c. v. Jungwirth, and J. Železný, Efficient electri- calspinsplitterbasedonnonrelativisticcollinearantiferromag- netism, Phys. Rev. Lett.126, 127701 (2021)
work page 2021
-
[12]
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,EfficientSpin-to-ChargeConversionviaAltermagnetic SpinSplittingEffectinAntiferromagnetRuO 2,Phys.Rev.Lett. 130, 216701 (2023)
work page 2023
-
[13]
C.Song,H.Bai,Z.Zhou,L.Han,H.Reichlova,J.H.Dil,J.Liu, X. Chen, and F. Pan, Altermagnets as a new class of functional materials, Nat. Rev. Mater.10, 473 (2025)
work page 2025
-
[14]
J. Lai, T. Yu, P. Liu, L. Liu, G. Xing, X.-Q. Chen, and Y. Sun, 𝑑-Wave Flat Fermi Surface in Altermagnets Enables Maxi- mum Charge-to-Spin Conversion, Phys. Rev. Lett.135, 256702 (2025)
work page 2025
- [15]
-
[16]
J.Wang,W.Zhang,Y.Liu,J.Hu,Z.Zhang,R.Xiong,andZ.Lu, Strain-engineered modulation of non-relativistic altermagnetic spin splitting in rutileRuO2, Mater. Today Phys.63, 102081 (2026)
work page 2026
-
[17]
Y. Bang, X. Chen, P. Guo, Q. Liu, S. Liu, J. Wang, B. Shen, Y. Han, G. Wang, J. Wang, S. Wang, Z. Zeng, X. Zhang, K. L. Wang, and W. Zhao, Strain-tunable altermagnetism and uncon- ventional topological states in MnTe, Phys. Rev. B109, 104408 (2024)
work page 2024
-
[18]
Y.Zhang,J.Liu,J.Ding,Z.Cao,C.Liu,C.Xu,S.Liu,H.Zhang, J. Yu, D. Wu, W. Luo, Q. Liu, K. L. Wang, W. Zhao, and Q. Wang, Tuning spin splitting and anomalous Hall effect in𝑔- wave altermagnet CrSb thin films via strain engineering, Phys. Rev. B110, 094437 (2024)
work page 2024
- [19]
-
[20]
See Supplemental Material at [URL will be inserted by pub- lisher] for (I) Computational methods and Kubo formula, (II) Supplementary band structures, (III) Effective model and al- termagnetic symmetry, (IV) Rotation of the spin conductivity tensorandangulardependenceofthespincurrents,(V)Supple- mentarydiscussion: Discrepanciesbetweentheeffectivemodel and...
-
[21]
P. A. Lee, Localized states in a𝑑-wave superconductor, Phys. Rev. Lett.71, 1887 (1993)
work page 1993
-
[22]
S. Bhowal and N. A. Spaldin, Ferroically Ordered Magnetic Octupoles in𝑑-Wave Altermagnets, Phys. Rev. X14, 011019 (2024)
work page 2024
-
[23]
X. Wu, D. Di Sante, T. Schwemmer, W. Hanke, H. Y. Hwang, S.Raghu,andR.Thomale,Robust𝑑 𝑥2 −𝑦 2-wavesuperconductiv- ityofinfinite-layernickelates,Phys.Rev.B101,060504(2020)
work page 2020
-
[24]
V.I.Anisimov,J.Zaanen,andO.K.Andersen,Bandtheoryand Mott insulators: Hubbard𝑈instead of Stoner I, Phys. Rev. B 44, 943 (1991)
work page 1991
-
[25]
S. L. Dudarev, G. A. Botton, S. Y. Savrasov, C. J. Humphreys, andA.P.Sutton,Electron-energy-lossspectraandthestructural stability of nickel oxide: An LSDA+𝑈study, Phys. Rev. B57, 1505 (1998)
work page 1998
-
[26]
C. K. Majumdar and D. K. Ghosh, On next-nearest-neighbor interaction in linear chain. I, J. Math. Phys.10, 1388 (1969)
work page 1969
-
[27]
C. K. Majumdar and D. K. Ghosh, On next-nearest-neighbor interaction in linear chain. II, J. Math. Phys.10, 1399 (1969)
work page 1969
-
[28]
G. Zhao, Z. Meng, W. Huang, P. Qin, S. Ruan, L. Ma, L. Zhu, Y.He,L.Liu,Z.Duan,X.Wang,H.Chen,S.Jiang,J.Li,X.Tan, K. Ozawa, B. Wang, J. Cheng, Q. Zhang, J. Wang, C. Chen, and Z. Liu, Pressure-induced metal-insulator and paramagnet- altermagnettransitionsinrutileOsO 2singlecrystals[J],Newton , 100441 (2026)
work page 2026
-
[29]
H.Jiang,L.Wang,S.Hu,W.Xie,Y.Min,J.Yang,F.Liu,Y.Lu, L. Xie, and H. Huang, Strain-Induced Giant Enhancement of Magnetism in RuO2 Films[J], Adv. Funct. Mater.n/a, e28172
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.