REVIEW 4 major objections 5 minor 87 references
Real-space first-principles approach to orbitronic phenomena in metallic multilayers
T0 review · 4 major / 5 minor · reviewed 2026-08-05 · deepseek-v4-flash
Pith's one-line read A real-space DFT method computes orbital and spin Hall transport and accumulation directly in transition-metal multilayers, showing substantial orbital accumulation even in centrosymmetric systems.
desk verdict A genuinely new real-space method for orbital/spin Hall transport, but the central numbers are unsecured until the orbital current operator is defined and benchmarked. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing objects are (i) the RS-LMTO-ASA real-space Hamiltonian in its orthogonal tight-binding representation (Eq. 1), built from potential parameters and structure constants, and (ii) the Chebyshev polynomial expansion of the Green's function used to evaluate the Kubo-Bastin formula. The Chebyshev recursion constructs moments and reconstructs LDOS and response functions with numerical stability and linear scaling; each nonequivalent atom needs one recursion. This replaces momentum-space DFT followed by Wannier or pseudo-atomic projection, keeping disorder, interfaces, and open boundaries as explicit real-space features. The orbital angular momentum current is defined within an intr
What would settle it
Compare the real-space intra-atomic orbital Hall conductivities for bulk transition metals such as Ti, Cr, or W against converged momentum-space DFT calculations that include the orbital dependence of the anomalous position; a mismatch beyond numerical precision would show the omitted inter-atomic contributions are not negligible. A second test is to measure layer-resolved orbital accumulation in a centrosymmetric Co/Ti or Ni/W stack with magneto-optical detection: the paper's central prediction is a clear in-plane orbital/spin signal, so a null result would refute it.
Extended reading notes
Core claim
The central claim is that a fully real-space first-principles calculation can capture orbital Hall transport and non-equilibrium orbital/spin accumulation in layered transition-metal systems. The RS-LMTO-ASA orthogonal Hamiltonian is kept in real space, and the Kubo-Bastin formula is evaluated with a Chebyshev expansion of the Green's functions. Layer-resolved results for ferromagnet/normal-metal stacks show substantial in-plane orbital and spin accumulation even in centrosymmetric geometries, driven by band-structure asymmetry and interfacial scattering. The paper further argues this accumulation can be steered by structural confinement to engineer orbital torque in transition-metal bilayer
Load-bearing premise
The calculation assumes each atom's orbital angular momentum lives entirely inside that atom's sphere, ignoring the inter-atomic pieces of the orbital motion that some analyses show contribute to the orbital Hall effect; if those inter-atomic pieces are significant, the predicted numbers change.
Editorial extensions
If this is right
- Orbital and spin Hall conductivities and accumulations can be computed for large, disordered, finite multilayers without Wannier projection, directly from the DFT Hamiltonian.
- Because the cost scales linearly with the number of nonequivalent atoms, full heterostructures with interface roughness or compositional disorder become tractable at first-principles level.
- Centrosymmetric metallic stacks are predicted to host substantial orbital and spin accumulation, so inversion symmetry alone does not suppress orbitronic effects.
- The interplay between orbital Hall generation and structural confinement in transition-metal bilayers is a handle for engineering orbital torque.
- The same Green's-function machinery yields layer-resolved profiles, tying transport quantities to individual atomic layers in the stack.
Reading between the lines
- If the centrosymmetric accumulation result survives inclusion of inter-atomic anomalous-position terms, it would open a design route for orbital-memory and torque devices based on symmetric stacks, which are easier to grow; the paper itself only notes the possibility of torque engineering.
- The same Chebyshev/Kubo-Bastin real-space pipeline could be applied to other linear-response functions, such as the orbital Edelstein effect, orbital Nernst response, or frequency-dependent conductivities, without changing the Hamiltonian, though the paper does not compute these.
- A direct numerical comparison of the intra-atomic orbital-current definition with calculations including the orbital dependence of the anomalous position would map the regime where the real-space method is quantitatively reliable.
- Varying interface roughness or alloy disorder systematically in these multilayers and comparing layer-resolved accumulation would help separate band-structure-driven from scattering-driven contributions.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper develops a real-space DFT-based method for orbitronic transport in metallic multilayers. It combines the RS-LMTO-ASA Hamiltonian with a Chebyshev polynomial expansion of the Green's functions and evaluates Kubo-Bastin linear response directly in real space. The method is applied to Co/Ti, Fe/Ti, Ni/Ti, Co/W, Fe/W, and Ni/W heterostructures, and the central claim is that substantial orbital (and spin) accumulation can appear even in centrosymmetric systems, driven by band-structure asymmetries and interfacial scattering. The authors also claim linear scaling with system size and the natural inclusion of disorder, finite-size effects, and interface roughness.
Significance. If fully validated, this approach would provide a valuable real-space alternative to Wannier/Kubo methods for orbital transport in large, inhomogeneous heterostructures, with no fitted parameters entering the transport calculation. The methodological skeleton is credible: Kubo-Bastin plus KPM is a well-established combination, and the RS-LMTO-ASA Hamiltonian is an independent first-principles construction. However, the key physical observables--the orbital current operator, the orbital accumulation definition, and the orbital angular momentum operator in the chosen basis--are never explicitly given, and no benchmark against established bulk orbital Hall conductivity values is shown. Without these, the quantitative results, including the central 'centrosymmetric accumulation' claim, remain unsecured.
major comments (4)
- [Sec. II] The orbital Hall conductivity and orbital accumulation are the central outputs, but the manuscript never defines the orbital angular momentum operator L, the orbital current operator J_orb, or the accumulation operator used in the Kubo-Bastin trace. Eq. (1) gives the Hamiltonian and Eq. (2) gives the LDOS expansion, but no formula such as J_orb^γ = {L^α, v^β}_+/2 or the corresponding Kubo-Bastin expression is displayed. The numerical results in Figs. 4-5 depend directly on this operator choice. Please provide these definitions explicitly.
- [Sec. III / bulk validation] No validation against known orbital Hall conductivity values for the same elemental materials is presented. For example, bulk Ti, W, and Pt have published first-principles OHE results from Wannier/Kubo methods; a single comparison for one of these would anchor the method and calibrate the magnitude and sign of the results. As written, the quantitative values of the orbital conductivities and accumulations rest on an unverified implementation of the current operator.
- [Sec. II, Ref. [53]] The manuscript cites Ref. [53] on the role of inter-atomic 'anomalous position' contributions to the orbital Hall effect, but does not state how that issue is handled in the present real-space framework. If the implementation uses an intra-atomic, site-diagonal L and neglects inter-atomic contributions, the resulting OHE values can be quantitatively inaccurate, especially for 5d metals where orbital texture is nonlocal. The authors should either justify this approximation for their specific systems or provide a concrete test of its magnitude.
- [Sec. III, Fig. 5] The orbital accumulation results are reported as layer-resolved in-plane components L_x and L_y, but no definition of 'orbital accumulation' is given. It is not stated whether this is a non-equilibrium expectation value of an intra-atomic L operator, how it is projected onto atomic layers, or what units are used (e.g., ħ per atom). This makes the central quantitative claim about substantial accumulation in centrosymmetric systems impossible to interpret or reproduce.
minor comments (5)
- [Eqs. (1)-(3)] Several mathematical symbols appear as placeholder glyphs in the displayed equations (e.g., the Hamiltonian and LDOS formulas). The typesetting needs to be fixed so that the equations are readable.
- [Abstract / Sec. I] The abstract states that the method 'naturally incorporates disorder, finite-size effects, and interface roughness,' but the visible results and discussions do not include any disordered system or explicit interface roughness calculation. Either add such a calculation or temper the claim.
- [Sec. II] The Kubo-Bastin formula is cited as [54-60], but the actual linear-response expression used for the conductivity and accumulation is not written out. Including the explicit Kubo-Bastin formula would also clarify how the Chebyshev moments enter.
- [Sec. II] The convergence of the Chebyshev expansion is reported only as a fixed 'N = 500'. A brief convergence test with respect to N would strengthen confidence in the numerical results.
- [Introduction] There is a typographical error: 'layered TM systems an a series of TM-based heterostructures' should read 'and a series.'
Circularity Check
No significant circularity: the transport and accumulation results follow from the self-consistent RS-LMTO-ASA Hamiltonian via a Kubo-Bastin/Chebyshev response calculation, with no fitted parameters and no load-bearing self-citation chain.
full rationale
The paper's derivation chain is self-contained with respect to its central physical claims. The electronic structure is obtained from the self-consistent RS-LMTO-ASA Hamiltonian of Eq. (1), the LDOS is computed via the Chebyshev expansion of Eq. (2), and the orbital/spin Hall transport and accumulations are then evaluated directly in real space through a Kubo-Bastin linear-response framework, as described in Sec. II. No parameter is fitted to the reported orbital or spin accumulations, and the predicted values are not defined in terms of the output; they emerge from the Hamiltonian and the response formula. The paper does cite prior work by the same authors for the RS-LMTO-ASA method and for real-space Kubo/Chebyshev transport implementations (e.g., Refs. [49-52,54-60]), but these citations establish the numerical methodology, not the target physical result, and they are independently developed and widely used tools rather than unverified premises that force the conclusion. There is no fitted input renamed as a prediction, no uniqueness theorem imported from the authors to rule out alternatives, and no ansatz smuggled in solely through self-citation. The skeptic's concern that the orbital current operator is not explicitly displayed, and that no bulk OHE benchmark is shown in the visible text, is a completeness or verifiability issue, not a circularity: an omitted operator definition or missing benchmark does not make the derivation equivalent to its inputs. Therefore the circularity burden is low and the honest finding is no significant circularity.
Assumptions & free parameters
free parameters (2)
- Number of Chebyshev moments N =
500
- Chebyshev rescaling parameters a, b and safety constant epsilon =
determined from extremal eigenvalues (Eq. 3), epsilon small
assumptions (4)
- standard math Chebyshev polynomial expansion and kernel polynomial method provide accurate approximations of Green's functions and response functions.
- standard math Kubo-Bastin formula correctly gives linear response orbital/spin conductivities and accumulations.
- domain assumption The RS-LMTO-ASA method with the orthogonal tight-binding representation yields sufficiently accurate Hamiltonians for transition-metal heterostructures.
- domain assumption An intra-atomic definition of the orbital angular momentum operator in the localized basis is sufficient to capture orbital transport.
Cite this review
Pith. "Pith review of Real-space first-principles approach to orbitronic phenomena in metallic multilayers." pith.science (2026). https://pith.science/paper/XOTNROVM
@misc{pith2026250814270,
author = {Pith},
title = {Pith review of: Real-space first-principles approach to orbitronic phenomena in metallic multilayers},
year = {2026},
howpublished = {\url{https://pith.science/paper/XOTNROVM}},
note = {Machine review of arXiv:2508.14270}
}
read the original abstract
We develop a real-space first-principles method based on density functional theory to investigate orbitronic phenomena in complex materials. Using the Real-Space Linear Muffin-Tin Orbital method within the Atomic Sphere Approximation (RS-LMTO-ASA) combined with a Chebyshev polynomial expansion of the Green's functions, we compute orbital (spin) Hall transport and orbital (spin) accumulation directly in real space. The approach scales linearly with system size and naturally incorporates disorder, finite-size effects, and interface roughness. We apply the method to transition-metal-based heterostructures and demonstrate the emergence of substantial orbital (spin) accumulation, even in centrosymmetric systems. Our methodology provides a scalable and flexible framework for realistic simulations of orbital transport phenomena in complex heterostructures.
Reference graph
Works this paper leans on
- [53]
-
[1]
D. Go, D. Jo, H.-W. Lee, M. Kläui, and Y. Mokrousov, Orbitronics: Orbital currents in solids, Europhysics Let- ters 135, 37001 (2021)
2021
-
[2]
D. Jo, D. Go, G.-M. Choi, and H.-W. Lee, Spintron- ics meets orbitronics: Emergence of orbital angular mo- mentum in solids, npj Spintronics2, 10.1038/s44306-024- 00023-6 (2024)
-
[3]
P. Wang, F. Chen, Y. Yang, S. Hu, Y. Li, W. Wang, D. Zhang, and Y. Jiang, Orbitronics: Mechanisms, materials and devices, Advanced Electronic Materials 10 10.1002/aelm.202400554 (2024)
-
[4]
T. Yoda, T. Yokoyama, and S. Murakami, Or- bital edelstein effect as a condensed-matter analog of solenoids, Nano Letters18, 916 (2018), pMID: 29373028, https://doi.org/10.1021/acs.nanolett.7b04300
-
[5]
A.Johansson,Theoryofspinandorbitaledelsteineffects, JournalofPhysics: CondensedMatter 36,423002(2024)
2024
-
[6]
S. A. Nikolaev, M. Chshiev, F. Ibrahim, S. Kr- ishnia, N. Sebe, J.-M. George, V. Cros, H. Jaf- frès, and A. Fert, Large chiral orbital texture and orbital edelstein effect in co/al heterostructure, Nano Letters 24, 13465 (2024), pMID: 39433297, https://doi.org/10.1021/acs.nanolett.4c01607
-
[7]
Chirolli, M
L. Chirolli, M. T. Mercaldo, C. Guarcello, F. Giazotto, and M. Cuoco, Colossal orbital edelstein effect in non- centrosymmetric superconductors, Phys. Rev. Lett.128, 217703 (2022)
2022
Show all 87 references
-
[8]
Sala and P
G. Sala and P. Gambardella, Giant orbital hall effect and orbital-to-spin conversion in��, ��, and �� metallic het- erostructures, Phys. Rev. Res.4, 033037 (2022)
2022
-
[9]
Go and H.-W
D. Go and H.-W. Lee, Orbital torque: Torque generation by orbital current injection, Phys. Rev. Res.2, 013177 (2020)
2020
-
[10]
D. Go, F. Freimuth, J.-P. Hanke, F. Xue, O. Gomonay, K.-J. Lee, S. Blügel, P. M. Haney, H.-W. Lee, and Y. Mokrousov, Theory of current-induced angular mo- mentum transfer dynamics in spin-orbit coupled systems, Phys. Rev. Res.2, 033401 (2020)
2020
-
[11]
A. Bose, F. Kammerbauer, R. Gupta, D. Go, Y. Mokrousov, G. Jakob, and M. Kläui, Detection of long-rangeorbital-halltorques,Phys.Rev.B 107,134423 (2023)
2023
-
[12]
Fukunaga, S
R. Fukunaga, S. Haku, H. Hayashi, and K. Ando, Orbital torque originating from orbital hall effect in zr, Phys. Rev. Res. 5, 023054 (2023)
2023
-
[13]
Santos, J
E. Santos, J. Abrão, D. Go, L. de Assis, Y. Mokrousov, J. Mendes, and A. Azevedo, Inverse orbital torque via spin-orbital intertwined states, Phys. Rev. Appl. 19, 014069 (2023)
2023
-
[14]
Lyalin and R
I. Lyalin and R. K. Kawakami, Interface transparency to orbital current, Phys. Rev. B110, 104418 (2024)
2024
-
[15]
D. Go, K. Ando, A. Pezo, S. Blügel, A. Manchon, and Y. Mokrousov, Orbital pumping by magnetization dy- namics in ferromagnets, Phys. Rev. B 111, L140409 (2025)
2025
-
[16]
Han, H.-W
S. Han, H.-W. Ko, J. H. Oh, H.-W. Lee, K.-J. Lee, and K.-W. Kim, Orbital pumping incorporating both orbital angular momentum and position, Phys. Rev. Lett.134, 036305 (2025)
2025
-
[17]
H.Hayashi, D.Go, S.Haku, Y.Mokrousov,andK.Ando, Observation of orbital pumping, Nature Electronics 7, 646–652 (2024)
2024
-
[18]
Santos, J
E. Santos, J. E. Abrão, A. S. Vieira, J. B. S. Mendes, R. L. Rodríguez-Suárez, and A. Azevedo, Exploring orbital-charge conversion mediated by interfaces with ��� � through spin-orbital pumping, Phys. Rev. B109, 014420 (2024)
2024
-
[19]
Wang, M.-G
H. Wang, M.-G. Kang, D. Petrosyan, S. Ding, R. Schlitz, L.J.Riddiford, W.Legrand,andP.Gambardella,Orbital pumping in ferrimagnetic insulators, Phys. Rev. Lett. 134, 126701 (2025)
2025
-
[20]
B. A. Bernevig, T. L. Hughes, and S.-C. Zhang, Orbi- tronics: The intrinsic orbital current in�-doped silicon, Phys. Rev. Lett.95, 066601 (2005)
2005
-
[21]
Kontani, T
H. Kontani, T. Tanaka, D. S. Hirashima, K. Yamada, and J. Inoue, Giant intrinsic spin and orbital hall effects in ��� � �� (� � �� , rh, mo), Phys. Rev. Lett.100, 096601 (2008)
2008
-
[22]
Kontani, T
H. Kontani, T. Tanaka, D. S. Hirashima, K. Yamada, and J. Inoue, Giant orbital hall effect in transition metals: Origin of large spin and anomalous hall effects, Phys. Rev. Lett. 102, 016601 (2009)
2009
-
[23]
Tanaka, H
T. Tanaka, H. Kontani, M. Naito, T. Naito, D. S. Hi- rashima, K. Yamada, and J. Inoue, Intrinsic spin hall ef- fect and orbital hall effect in�� and �� transition metals, Phys. Rev. B77, 165117 (2008)
2008
-
[24]
D. Go, D. Jo, C. Kim, and H.-W. Lee, Intrinsic spin and orbital hall effects from orbital texture, Phys. Rev. Lett. 121, 086602 (2018)
2018
-
[25]
Salemi and P
L. Salemi and P. M. Oppeneer, First-principles theory of intrinsic spin and orbital hall and nernst effects in metal- lic monoatomic crystals, Phys. Rev. Mater. 6, 095001 (2022)
2022
-
[26]
Y.-G. Choi, D. Jo, K.-H. Ko, D. Go, K.-H. Kim, H. G. Park, C. Kim, B.-C. Min, G.-M. Choi, and H.-W. Lee, Observation of the orbital hall effect in a light metal ti, Nature 619, 52–56 (2023)
2023
-
[27]
Lyalin, S
I. Lyalin, S. Alikhah, M. Berritta, P. M. Oppeneer, and R.K.Kawakami,Magneto-opticaldetectionoftheorbital hall effect in chromium, Phys. Rev. Lett. 131, 156702 (2023)
2023
-
[28]
G. Sala, H. Wang, W. Legrand, and P. Gambardella, Or- bital hanle magnetoresistance in a �� transition metal, Phys. Rev. Lett.131, 156703 (2023)
2023
-
[29]
J. E. Abrão, E. Santos, J. L. Costa, J. G. S. Santos, J. B.S. Mendes, andA. Azevedo, Anomalous spinand or- bital hall phenomena in antiferromagnetic systems, Phys. Rev. Lett. 134, 026702 (2025)
2025
-
[30]
Busch, I
O. Busch, I. Mertig, and B. Göbel, Orbital hall effect and orbital edge states caused by� electrons, Phys. Rev. Res. 5, 043052 (2023)
2023
-
[31]
Y. Yen, J. A. Krieger, M. Yao, I. Robredo, K. Manna, Q. Yang, E. C. McFarlane, C. Shekhar, H. Borrmann, S. Stolz, R. Widmer, O. Gröning, V. N. Strocov, S. S. P. Parkin, C. Felser, M. G. Vergniory, M. Schüler, and N. B. M. Schröter, Controllable orbital angular momen- tum monop...
1912
-
[32]
S. S. Brinkman, X. L. Tan, B. Brekke, A. C. Mathisen, O. Finnseth, R. J. Schenk, K. Hagiwara, M.-J. Huang, J. Buck, M. Kalläne, M. Hoesch, K. Rossnagel, K.-H. Ou Yang, M.-T. Lin, G.-J. Shu, Y.-J. Chen, C. Tusche, and H. Bentmann, Chirality-driven orbital angular mo- mentum and...
2024
-
[33]
R. B. Atencia, D. P. Arovas, and D. Culcer, Intrinsic torque on the orbital angular momentum in an electric field, Phys. Rev. B110, 035427 (2024)
2024
-
[34]
H. Liu, J. H. Cullen, D. P. Arovas, and D. Culcer, Quan- tum correction to the orbital hall effect, Phys. Rev. Lett. 134, 036304 (2025)
2025
-
[35]
Hagiwara, Y
K. Hagiwara, Y. Chen, D. Go, X. L. Tan, S. Grytsiuk, K. O. Yang, G. Shu, J. Chien, Y. Shen, X. Huang, I. Cojocariu, V. Feyer, M. Lin, S. Blügel, C. M. Schnei- der, Y. Mokrousov, and C. Tusche, Orbital topology of chiral crystals for orbitronics, Advanced Materials 37, 10.1002/...
2025 doi
-
[36]
L. M. Canonico, T. P. Cysne, A. Molina-Sanchez, R. B. Muniz, and T. G. Rappoport, Orbital hall insulating phase in transition metal dichalcogenide monolayers, Phys. Rev. B101, 161409 (2020)
2020
-
[37]
L. M. Canonico, T. P. Cysne, T. G. Rappoport, and R. B. Muniz, Two-dimensional orbital hall insulators, Phys. Rev. B101, 075429 (2020)
2020
-
[38]
Bhowal and S
S. Bhowal and S. Satpathy, Orbital gyrotropic magne- toelectric effect and its strain engineering in monolayer �� � �, Phys. Rev. B102, 201403 (2020)
2020
-
[39]
Bhowal and S
S. Bhowal and S. Satpathy, Intrinsic orbital and spin halleffectsinmonolayertransitionmetaldichalcogenides, Phys. Rev. B102, 035409 (2020)
2020
-
[40]
Bhowal and G
S. Bhowal and G. Vignale, Orbital hall effect as an al- ternative to valley hall effect in gapped graphene, Phys. Rev. B 103, 195309 (2021)
2021
-
[41]
T. P. Cysne, M. Costa, L. M. Canonico, M. B. Nardelli, R. B. Muniz, and T. G. Rappoport, Disentangling or- bital and valley hall effects in bilayers of transition metal dichalcogenides, Phys. Rev. Lett.126, 056601 (2021)
2021
-
[42]
T. P. Cysne, S. Bhowal, G. Vignale, and T. G. Rap- poport, Orbital hall effect in bilayer transition metal dichalcogenides: From the intra-atomic approximation to the bloch states orbital magnetic moment approach, Phys. Rev. B105, 195421 (2022)
2022
-
[43]
Costa, B
M. Costa, B. Focassio, L. M. Canonico, T. P. Cysne, G. R. Schleder, R. B. Muniz, A. Fazzio, and T. G. Rappoport, Connecting higher-order topology with the orbital hall effect in monolayers of transition metal dichalcogenides, Phys. Rev. Lett.130, 116204 (2023)
2023
-
[44]
A. Pezo, D. García Ovalle, and A. Manchon, Orbital hall physics in two-dimensional dirac materials, Phys. Rev. B 108, 075427 (2023)
2023
-
[45]
Z. Chen, R. Li, Y. Bai, N. Mao, M. Zeer, D. Go, Y. Dai, B. Huang, Y. Mokrousov, and C. Niu, Topology- engineered orbital hall effect in two-dimensional ferro- magnets, Nano Letters24, 4826 (2024), pMID: 38619844, https://doi.org/10.1021/acs.nanolett.3c05129
2024 doi
-
[46]
Veneri, T
A. Veneri, T. G. Rappoport, and A. Ferreira, Extrinsic orbital hall effect: Orbital skew scattering and crossover between diffusive and intrinsic orbital transport, Phys. Rev. Lett. 134, 136201 (2025)
2025
-
[47]
Faridi and R
A. Faridi and R. Asgari, Comparing the extrinsic orbital hall effect in centrosymmetric and noncentrosymmetric systems: Insights from bilayer transition metal dichalco- genides (2025), arXiv:2501.02996 [cond-mat.mes-hall]
2025 arXiv
-
[48]
Sun and G
H. Sun and G. Vignale, Orbital magnetic moment dy- namics and hanle magnetoresistance in multilayered two-dimensional materials, Phys. Rev. B111, L180408 (2025)
2025
-
[49]
Frota-Pessoâ, First-principles real-space linear-muffin- tin-orbital calculations of 3 d impurities in Cu, Phys
S. Frota-Pessoâ, First-principles real-space linear-muffin- tin-orbital calculations of 3 d impurities in Cu, Phys. Rev. B 46, 14570 (1992)
1992
-
[50]
A. B. Klautau and S. Frota-Pessôa, Magnetic properties of Co nanowires on Cu(001) surfaces, Phys. Rev. B70, 193407 (2004)
2004
-
[51]
Frota-Pessôa, L
S. Frota-Pessôa, L. A. de Mello, H. M. Petrilli, and A. B. Klautau, First-principles calculations for interstitial fe impurities in hcp sc, y, ti, and zr, Phys. Rev. Lett.71, 4206 (1993)
1993
-
[52]
A. B. Klautau and S. Frota-Pessôa, Orbital moments of 3d adatoms and Co nanostructures on Cu(001) surfaces, Surf. Sci. 579, 27 (2005)
2005
-
[54]
J.H.García, L.Covaci,andT.G.Rappoport,Real-Space Calculation of the Conductivity Tensor for Disordered Topological Matter, Physical Review Letters114, 116602 (2015), publisher: American Physical Society
2015
-
[55]
J. H. Garcia and T. G. Rappoport, Kubo–bastin ap- proach for the spin hall conductivity of decorated graphene, 2D Materials3, 024007 (2016)
2016
-
[56]
Ferreira and E
A. Ferreira and E. R. Mucciolo, Critical delocalization of chiral zero energy modes in graphene, Phys. Rev. Lett. 115, 106601 (2015)
2015
-
[57]
T. P. Cysne, T. G. Rappoport, A. Ferreira, J. M. V. P. Lopes, and N. M. R. Peres, Numerical calculation of the casimir-polder interaction between a graphene sheet with vacancies and an atom, Phys. Rev. B94, 235405 (2016)
2016
-
[58]
S. M. João, M. An\djelković, L. Covaci, T. G. Rap- poport, J. M. V. P. Lopes, and A. Ferreira, KITE: high- performance accurate modelling of electronic structure and response functions of large molecules, disordered crystals and heterostructures, Royal Society Open Sci- ence 7...
2020
-
[59]
J. P. Santos Pires, S. M. João, A. Ferreira, B. Amorim, and J. M. Viana Parente Lopes, Anomalous transport signatures in weyl semimetals with point defects, Phys. Rev. Lett. 129, 196601 (2022)
2022
-
[60]
S. G. de Castro, J. a. M. V. P. Lopes, A. Ferreira, and D. A. Bahamon, Fast fourier-chebyshev approach to real- space simulations of the kubo formula, Phys. Rev. Lett. 132, 076302 (2024)
2024
-
[61]
C. W. Groth, M. Wimmer, A. R. Akhmerov, and X. Waintal, Kwant: a software package for quantum transport, New Journal of Physics16, 063065 (2014)
2014
-
[62]
Y. O. Kvashnin, R. Cardias, A. Szilva, I. Di Marco, M. I. Katsnelson, A. I. Lichtenstein, L. Nordström, A. B. Klau- tau, and O. Eriksson, Microscopic origin of heisenberg and non-heisenberg exchange interactions in ferromag- netic bcc fe, Phys. Rev. Lett.116, 217202 (2016)
2016
-
[63]
Bergman, L
A. Bergman, L. Nordström, A. B. Klautau, S. Frota- Pessôa, and O. Eriksson, Magnetic interactions of Mn clusters supported on Cu, Phys. Rev. B 73, 174434 (2006)
2006
-
[64]
Bergman, L
A. Bergman, L. Nordström, A. Burlamaqui Klautau, S. Frota-Pessôa, and O. Eriksson, Magnetic structures of small fe, mn, and cr clusters supported on cu(111): Noncollinear first-principles calculations, Phys. Rev. B 75, 224425 (2007)
2007
-
[65]
Cardias, A
R. Cardias, A. Szilva, M. Bezerra-Neto, M. Ribeiro, A. Bergman, Y. O. Kvashnin, J. Fransson, A. Klau- tau, O. Eriksson, and L. Nordström, First-principles dzyaloshinskii–moriya interaction in a non-collinear framework, Sci. Rep.10, 1 (2020)
2020
-
[66]
Szilva, D
A. Szilva, D. Thonig, P. F. Bessarab, Y. O. Kvashnin, D. C. M. Rodrigues, R. Cardias, M. Pereiro, L. Nord- ström, A. Bergman, A. B. Klautau, and O. Eriksson, Theory of noncollinear interactions beyond Heisenberg exchange: Applications to bcc Fe, Phys. Rev. B 96, 144413 (2017)
2017
-
[67]
Brandão, P
J. Brandão, P. C. Carvalho, I. P. Miranda, T. J. A. Mori, F. Béron, A. Bergman, H. M. Petrilli, A. B. Klautau, and J. C. Cezar, Proximity-induced flipped spin state in 12 synthetic ferrimagnetic pt/co/gd heterolayers, Commu- nications Physics 8, 22 (2025)
2025
-
[68]
I. P. Miranda, A. B. Klautau, A. Bergman, D. Thonig, H. M. Petrilli, and O. Eriksson, Mechanisms behind large gilbert damping anisotropies, Phys. Rev. B103, L220405 (2021)
2021
-
[69]
R. N. Igarashi, A. B. Klautau, R. B. Muniz, B. Sanyal, and H. M. Petrilli, First-principles studies of complex magnetism in mn nanostructures on the fe(001) surface, Phys. Rev. B85, 014436 (2012)
2012
-
[70]
D. C. M. Rodrigues, A. Szilva, A. B. Klautau, A.Bergman, O.Eriksson,andC.Etz,Finite-temperature interatomic exchange and magnon softening in Fe over- layers on Ir(001), Phys. Rev. B94, 014413 (2016)
2016
-
[71]
M. S. Ribeiro, G. B. Corrêa, A. Bergman, L. Nordström, O. Eriksson, and A. B. Klautau, From collinear to vortex magnetic structures in mn corrals on pt(111), Phys. Rev. B 83, 014406 (2011)
2011
-
[72]
O. K. Andersen, Linear methods in band theory, Phys. Rev. B 12, 3060 (1975)
1975
-
[73]
P. C. Carvalho, I. P. Miranda, J. Brandão, A. Bergman, J. C. Cezar, A. B. Klautau, and H. M. Petrilli, Corre- lation of interface interdiffusion and skyrmionic phases, Nano Letters 23, 4854 (2023)
2023
-
[74]
Cardias, J
R. Cardias, J. d. S. Silva, A. Bergman, A. Szilva, Y. O. Kvashnin, J. Fransson, A. B. Klautau, O. Eriksson, A. Delin, and L. Nordström, Unraveling the connection between high-order magnetic interactions and local-to- global spin hamiltonian in noncollinear magnetic dimers, Phy...
2023
-
[75]
D. C. M. Rodrigues, A. Szilva, A. B. Klautau, A.Bergman, O.Eriksson,andC.Etz,Finite-temperature interatomic exchange and magnon softening in fe overlay- ers on ir(001), Phys. Rev. B94, 014413 (2016)
2016
-
[76]
I. P. Miranda, A. B. Klautau, A. Bergman, and H. M. Petrilli, Band filling effects on the emergence of magnetic skyrmions: Pd/fe and pd/co bilayers on ir(111), Phys. Rev. B 105, 224413 (2022)
2022
-
[77]
Cardias, M
R. Cardias, M. M. Bezerra-Neto, M. S. Ribeiro, A. Bergman, A. Szilva, O. Eriksson, and A. B. Klautau, Magnetic and electronic structure of mn nanostructures on ag(111) and au(111), Phys. Rev. B93, 014438 (2016)
2016
-
[78]
A. B. Klautau, S. B. Legoas, R. B. Muniz, and S. Frota- Pessôa, Magnetic behavior of thin cr layers sandwiched by fe, Phys. Rev. B60, 3421 (1999)
1999
-
[79]
M. M. Bezerra-Neto, M. S. Ribeiro, B. Sanyal, A. Bergman, R. B. Muniz, O. Eriksson, and A. B. Klau- tau, Complex magnetic structure of clusters and chains of Ni and Fe on Pt(111), Sci. Rep.3, 3054 (2013)
2013
-
[80]
Cardias, M
R. Cardias, M. M. Bezerra-Neto, M. S. Ribeiro, A. Bergman, A. Szilva, O. Eriksson, and A. B. Klau- tau, Magnetic and electronic structure of Mn nanostruc- tures on Ag(111) and Au(111), Phys. Rev. B93, 014438 (2016)
2016
-
[81]
Frota-Pessôa, A
S. Frota-Pessôa, A. B. Klautau, and S. B. Legoas, Influ- ence of interface mixing on the magnetic properties of Ni/Pt multilayers, Phys. Rev. B66, 132416 (2002)
2002
-
[82]
R. C. A. de Almeida,Electronic structure and exchange interactions from ab initio theory , Ph.D. thesis, Uppsala University (2018)
2018
-
[83]
Haydock, The recursive solution of the schrodinger equation (Academic Press, 1980) pp
R. Haydock, The recursive solution of the schrodinger equation (Academic Press, 1980) pp. 215–294
1980
-
[84]
Beer and D
N. Beer and D. Pettifor, The recursion method and the estimation of local densities of states, inThe Electronic Structure of Complex Systems (Springer, 1984) pp. 769– 777
1984
-
[85]
Weiße, G
A. Weiße, G. Wellein, A. Alvermann, and H. Fehske, The kernel polynomial method, Reviews of Modern Physics 78, 275 (2006), publisher: American Physical Society
2006
-
[86]
L.Salemi, M.Berritta,andP.M.Oppeneer,Quantitative comparison of electrically induced spin and orbital po- larizations in heavy-metal/��-metal bilayers, Phys. Rev. Mater. 5, 074407 (2021)
2021
-
[87]
Salemi and P
L. Salemi and P. M. Oppeneer, Theory of magnetic spin and orbital hall and nernst effects in bulk ferromagnets, Phys. Rev. B106, 024410 (2022)
2022
Reviewed August 5, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.