pith. sign in

arxiv: 2606.06980 · v2 · pith:WHLE53QHnew · submitted 2026-06-05 · ❄️ cond-mat.mtrl-sci

Electric-field induced trends of exchange interactions in transition-metal trilayers

Pith reviewed 2026-06-27 21:54 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords electric fieldexchange interactionsspin spiralsdensity functional theorytransition-metal trilayershigher-order exchangemagnetic ground stateFe trilayers
0
0 comments X

The pith

Electric fields induce linear changes in exchange constants of Fe trilayers while the magnetic ground state stays fixed.

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

The paper uses density functional theory to examine how external electric fields affect pairwise Heisenberg and higher-order multi-spin exchange interactions in unsupported trilayers with an Fe layer between 4d and 5d metals. Spin-spiral energy dispersions are computed for fields reaching 1 V/Å and then fitted to models to obtain the constants. The dispersions remain qualitatively similar and the ground state does not switch, yet the exchange values display linear dependence on the field up to 0.5 V/Å, with changes of a few percent for nearest neighbors and up to tens of percent for longer-range terms that also depend on the overlayer. A reader would care because the results indicate electric fields can adjust specific magnetic couplings in thin films while leaving the overall order intact.

Core claim

Density functional theory calculations of spin-spiral dispersions in Fe layers sandwiched between 4d (Ru, Rh, Pd) and 5d (Ir) metals show that both pairwise and higher-order exchange constants depend linearly on the applied electric field up to about 0.5 V/Å. The energy dispersions stay qualitatively the same and the magnetic ground state remains unchanged. Magnitudes shift by a few percent for nearest-neighbor terms and by up to tens of percent for beyond-nearest-neighbor terms, with the size of the shift sensitive to the 4d overlayer and its fcc or hcp stacking. Higher-order constants extracted from multi-Q states such as uudd and 3Q also follow a nearly linear field dependence with variat

What carries the argument

Fitting of DFT spin-spiral energy dispersions to Heisenberg and multi-spin models to extract field-dependent exchange constants.

If this is right

  • The magnetic ground state remains the same for electric fields up to 1 V/Å.
  • Nearest-neighbor exchange constants change by only a few percent while longer-range constants can change by tens of percent.
  • Higher-order exchange constants extracted from multi-Q states vary nearly linearly by up to ten percent.
  • The size of the field-induced changes depends on the specific 4d overlayer and its stacking.
  • The electric field experiences different spin-dependent screening in the three trilayer compositions.

Where Pith is reading between the lines

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

  • If the linear dependence persists when the trilayers are placed on substrates, electric fields could serve as a dial to adjust individual exchange strengths in magnetic devices.
  • The larger relative changes in beyond-nearest-neighbor and higher-order terms suggest they offer a more sensitive route to electric-field control of non-collinear spin structures.
  • Choosing different 4d overlayers or stackings could be used to amplify or reduce the electric-field response of the exchanges.
  • Direct comparison of the unsupported predictions with measurements on epitaxial films would clarify the role of substrate effects.

Load-bearing premise

Fitting the calculated spin-spiral energies to the interaction models accurately extracts how the electric field modifies the exchange constants, and the unsupported trilayer plus chosen DFT functional captures the dominant physics.

What would settle it

An experimental measurement on similar trilayers that finds either a sign reversal or clear deviation from linear dependence in the exchange constants at fields below 0.5 V/Å would falsify the reported trends.

read the original abstract

Using density functional theory, we have performed a systematic study of the Heisenberg pairwise exchange interaction and the beyond Heisenberg multi-spin higher-order exchange interactions in unsupported transition-metal trilayers in the presence of external electric fields. The systems consist of a hexagonal atomic Fe layer sandwiched between 4$d$ (Ru, Rh, and Pd) and 5$d$ (Ir) transition-metal layers. Both fcc and hcp stackings of the 4$d$ overlayer have been taken into account. To scan a large part of the magnetic phase space, we have calculated the energy dispersion of spin spirals without and with applied electric fields up to $\pm 1.0$ V/{\AA}. We find that the energy dispersion remains qualitatively the same upon applying the electric fields and the magnetic ground state remains unchanged. The exchange constants obtained by fitting the energy dispersions exhibit a linear dependence on the electric field up to values of about $\pm 0.5$ V/{\AA}. The sign of the calculated pairwise and higher-order exchange constants remain unchanged with electric field, however, their values and field induced variation are sensitive to the 4$d$ overlayer. The changes are on the order of a few percent for the nearest-neighbor exchange constant and up to a few ten percent for beyond nearest-neighbor constants. The higher-order exchange constants are calculated based on the total energies of multi-$Q$ states, such as the $uudd$ and the 3$Q$ state. Similar to the pairwise exchange constants, we find a nearly linear field dependence of the higher order constants at small electric fields and variations of up to ten percent. We study the spin-dependent screening of the electric field for the three trilayers based on the spin- and orbital-decomposed electronic states.

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

0 major / 3 minor

Summary. The paper uses density functional theory to study the influence of external electric fields on exchange interactions in unsupported transition-metal trilayers consisting of Fe sandwiched between 4d (Ru, Rh, Pd) and 5d (Ir) layers. By calculating spin spiral energy dispersions with and without electric fields and fitting them to Heisenberg and multi-spin models, the authors find that the exchange constants show a linear dependence on the electric field up to approximately ±0.5 V/Å. The signs of the constants remain the same, but their magnitudes change by a few percent for nearest-neighbor interactions and up to tens of percent for longer-range ones, with sensitivity to the 4d overlayer. Higher-order exchange constants from multi-Q states exhibit similar linear trends, and the work includes an analysis of spin-dependent screening.

Significance. This study provides valuable insights into how electric fields can modulate magnetic exchange interactions in trilayer systems. The finding of linear dependence and the differential sensitivity of different exchange terms could have implications for electric-field controlled spintronics. The use of spin-spiral calculations and multi-Q states to extract both pairwise and higher-order terms is a solid methodological approach, and the systematic variation over different 4d elements adds robustness to the conclusions.

minor comments (3)
  1. [Abstract] The phrase 'a few ten percent' in the abstract should be corrected to 'a few tens of percent' for grammatical clarity.
  2. [Methods/Computational Details] Include a brief discussion or supplementary table on convergence of the spin-spiral calculations with respect to k-point sampling and energy cutoff, as this would support the reliability of the reported small percentage changes in the exchange constants.
  3. [Results] The figures displaying the energy dispersions of spin spirals should overlay the curves from the fitted Heisenberg and multi-spin models to allow visual assessment of fit quality.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive summary, significance assessment, and recommendation of minor revision. No major comments were provided in the report.

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper computes spin-spiral energy dispersions and multi-Q state total energies directly via DFT for unsupported Fe/4d/5d trilayers under applied electric fields. Exchange constants (pairwise and higher-order) are extracted by post-hoc fitting of these independent first-principles energies to Heisenberg plus multi-spin models. The reported linear E-field dependence up to ~0.5 V/Å and the percentage variations are emergent outputs of the DFT data, not inputs or self-definitions. No load-bearing self-citations, uniqueness theorems, or ansatzes are used to force the trends; the unsupported geometry and fitting procedure are explicit modeling choices. The central claim remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

Only the abstract is available, so the full list of DFT approximations, fitting procedures, and numerical parameters cannot be audited. The work relies on standard assumptions of density-functional theory for itinerant magnets and the validity of mapping total energies to effective spin models.

axioms (2)
  • domain assumption Density functional theory with a chosen exchange-correlation functional accurately describes the magnetic interactions in these metallic trilayers.
    Invoked implicitly by the use of DFT to compute spin-spiral energies.
  • domain assumption The mapping of spin-spiral and multi-Q total energies to pairwise and higher-order exchange constants via fitting is unique and physically meaningful.
    Central to extracting the reported field-dependent constants.

pith-pipeline@v0.9.1-grok · 5862 in / 1547 out tokens · 29229 ms · 2026-06-27T21:54:19.839189+00:00 · methodology

discussion (0)

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

Reference graph

Works this paper leans on

78 extracted references

  1. [1]

    In contrast, the sign of the second nearest-neighbor constant (J 2) is negative, favoring the AFM coupling, and its magnitude is larger thanJ 1 by a factor of nearly

  2. [2]

    These competing interactions induce exchange frus- tration in the trilayer and stabilizes the RW-AFM state below the FM states, as shown in Fig. 6(a). On the other hand, the sign ofJ 1 for hcp-Ru/Fe/Ir is negative at zero field and its value is approximately 7 meV, which strongly favors the AFM coupling (Ta- ble III). BothJ 2 andJ 3 possess positive signs...

  3. [3]

    Bogdanov and A

    A. Bogdanov and A. Hubert, Thermodynamically stable magnetic vortex states in magnetic crystals, J. Magn. Magn. Mater.138, 255 (1994)

  4. [4]

    Nagaosa and Y

    N. Nagaosa and Y. Tokura, Topological properties and dynamics of magnetic skyrmions, Nat. Nanotechnol.8, 899 (2013)

  5. [5]

    Heinze, K

    S. Heinze, K. von Bergmann, M. Menzel, J. Brede, A. Ku- betzka, R. Wiesendanger, G. Bihlmayer, and S. Bl¨ ugel, Spontaneous atomic-scale magnetic skyrmion lattice in two dimensions, Nat. Phys.7, 713 (2011)

  6. [6]

    Romming, C

    N. Romming, C. Hanneken, M. Menzel, J. E. Bickel, B. Wolter, K. von Bergmann, A. Kubetzka, and R. Wiesendanger, Writing and Deleting Single Magnetic Skyrmions, Science341, 636 (2013)

  7. [7]

    Romming, A

    N. Romming, A. Kubetzka, C. Hanneken, K. von Bergmann, and R. Wiesendanger, Field-Dependent Size and Shape of Single Magnetic Skyrmions, Phys. Rev. Lett.114, 177203 (2015)

  8. [8]

    Hagemeister, N

    J. Hagemeister, N. Romming, K. von Bergmann, E. Y. Vedmedenko, and R. Wiesendanger, Stability of single skyrmionic bits, Nat. Commun.6, 8455 (2015)

  9. [9]

    Kubetzka, C

    A. Kubetzka, C. Hanneken, R. Wiesendanger, and K. von Bergmann, Impact of the skyrmion spin texture on mag- netoresistance, Phys. Rev. B95, 104433 (2017)

  10. [10]

    Hanneken, F

    C. Hanneken, F. Otte, A. Kubetzka, B. Dup´ e, N. Romming, K. von Bergmann, R. Wiesendanger, and S. Heinze, Electrical detection of magnetic skyrmions by tunneling non-collinear magnetoresistance, Nat. Nan- otechnol.10, 1039 (2015)

  11. [11]

    Meyer, M

    S. Meyer, M. Perini, S. von Malottki, A. Kubetzka, R. Wiesendanger, K. von Bergmann, and S. Heinze, Iso- lated zero field sub–10 nm skyrmions in ultrathin Co films, Nat. Commun.10, 3823 (2019)

  12. [12]

    Boulle, J

    O. Boulle, J. Vogel, H. Yang, S. Pizzini, D. de Souza Chaves, A. Locatelli, T. O. Mente¸ s, A. Sala, L. D. Buda- Prejbeanu, O. Klein, M. Belmeguenai, Y. Roussign´ e, A. Stashkevich, S. M. Ch´ erif, L. Aballe, M. Foerster, M. Chshiev, S. Auffret, I. M. Miron, and G. Gaudin, Room-temperature chiral magnetic skyrmions in ultra- thin magnetic nanostructures, ...

  13. [13]

    Moreau-Luchaire, C

    C. Moreau-Luchaire, C. Mouta S, N. Reyren, J. Sampaio, C. A. F. Vaz, N. Van Horne, K. Bouzehouane, K. Garcia, C. Deranlot, P. Warnicke, P. Wohlh¨ uter, J.-M. George, M. Weigand, J. Raabe, V. Cros, and A. Fert, Additive interfacial chiral interaction in multilayers for stabiliza- tion of small individual skyrmions at room temperature, Nat. Nano.11, 444 (2016)

  14. [14]

    S. Woo, K. Litzius, B. Kr¨ uger, M.-Y. Im, L. Caretta, K. Richter, M. Mann, A. Krone, R. M. Reeve, 20 M. Weigand, P. Agrawal, I. Lemesh, M.-A. Mawass, P. Fischer, M. Kl¨ aui, and G. S. D. Beach, Observation of room-temperature magnetic skyrmions and their current- driven dynamics in ultrathin metallic ferromagnets, Nat. Mater.15, 501 (2016)

  15. [15]

    Soumyanarayanan, M

    A. Soumyanarayanan, M. Raju, A. L. G. Oyarce, A. K. C. Tan, M.-Y. Im, A. P. Petrovi´ c, P. Ho, K. H. Khoo, M. Tran, C. K. Gan, F. Ernult, and C. Panagopou- los, Tunable room-temperature magnetic skyrmions in Ir/Fe/Co/Pt multilayers, Nat. Mater.16, 898 (2017)

  16. [16]

    G. Chen, A. Mascaraque, A. T. N’Diaye, and A. K. Schmid, Room temperature skyrmion ground state stabi- lized through interlayer exchange coupling, Appl. Phys. Lett.106, 242404 (2015)

  17. [17]

    M.-G. Han, J. A. Garlow, Y. Liu, H. Zhang, J. Li, D. DiMarzio, M. W. Knight, C. Petrovic, D. Jariwala, and Y. Zhu, Topological Magnetic-Spin Textures in Two- Dimensional van der Waals Cr 2Ge2Te6, Nano Lett.19, 7859 (2019)

  18. [18]

    B. Ding, Z. Li, G. Xu, H. Li, Z. Hou, E. Liu, X. Xi, F. Xu, Y. Yao, and W. Wang, Observation of Mag- netic Skyrmion Bubbles in a van der Waals Ferromagnet Fe3GeTe2, Nano Lett.20, 868 (2020)

  19. [19]

    T.-E. Park, L. Peng, J. Liang, A. Hallal, F. S. Yasin, X. Zhang, K. M. Song, S. J. Kim, K. Kim, M. Weigand, G. Sch¨ utz, S. Finizio, J. Raabe, K. Garcia, J. Xia, Y. Zhou, M. Ezawa, X. Liu, J. Chang, H. C. Koo, Y. D. Kim, M. Chshiev, A. Fert, H. Yang, X. Yu, and S. Woo, N´ eel-type skyrmions and their current-induced motion in van der Waals ferromagnet-bas...

  20. [20]

    Y. Wu, B. Francisco, Z. Chen, W. Wang, Y. Zhang, C. Wan, X. Han, H. Chi, Y. Hou, A. Lodesani, G. Yin, K. Liu, Y.-t. Cui, K. L. Wang, and J. S. Moodera, A Van der Waals Interface Hosting Two Groups of Mag- netic Skyrmions, Adv. Mater.34, 2110583 (2022)

  21. [21]

    Powalla, M

    L. Powalla, M. T. Birch, K. Litzius, S. Wintz, F. S. Yasin, L. A. Turnbull, F. Schulz, D. A. Mayoh, G. Bal- akrishnan, M. Weigand, X. Yu, K. Kern, G. Sch¨ utz, and M. Burghard, Seeding and Emergence of Compos- ite Skyrmions in a van der Waals Magnet, Adv. Mater. 35, 2208930 (2023)

  22. [22]

    S. S. P. Parkin, M. Hayashi, and L. Thomas, Mag- netic Domain-Wall Racetrack Memory, Science320, 190 (2008)

  23. [23]

    Tomasello, E

    R. Tomasello, E. Martinez, R. Zivieri, L. Torres, M. Car- pentieri, and G. Finocchio, A strategy for the design of skyrmion racetrack memories, Sci. Rep.4, 6784 (2014)

  24. [24]

    Zhang, M

    X. Zhang, M. Ezawa, and Y. Zhou, Magnetic skyrmion logic gates: conversion, duplication and merging of skyrmions, Sci. Rep.5, 9400 (2015)

  25. [25]

    W. Kang, Y. Huang, C. Zheng, W. Lv, N. Lei, Y. Zhang, X. Zhang, Y. Zhou, and W. Zhao, Voltage Controlled Magnetic Skyrmion Motion for Racetrack Memory, Sci. Rep.6, 23164 (2016)

  26. [26]

    Tomasello, V

    R. Tomasello, V. Puliafito, E. Martinez, A. Manchon, M. Ricci, M. Carpentieri, and G. Finocchio, Performance of synthetic antiferromagnetic racetrack memory: do- main wall versus skyrmion, J. Phys. D: Appl. Phys.50, 325302 (2017)

  27. [27]

    S. Luo, M. Song, X. Li, Y. Zhang, J. Hong, X. Yang, X. Zou, N. Xu, and L. You, Reconfigurable Skyrmion Logic Gates, Nano Lett.18, 1180 (2018)

  28. [28]

    Grollier, D

    J. Grollier, D. Querlioz, K. Y. Camsari, K. Everschor- Sitte, S. Fukami, and M. D. Stiles, Neuromorphic spin- tronics, Nat. Electron.3, 360 (2020)

  29. [29]

    K. M. Song, J.-S. Jeong, B. Pan, X. Zhang, J. Xia, S. Cha, T.-E. Park, K. Kim, S. Finizio, J. Raabe, J. Chang, Y. Zhou, W. Zhao, W. Kang, H. Ju, and S. Woo, Skyrmion-based artificial synapses for neuromor- phic computing, Nat. Electron.3, 148 (2020)

  30. [30]

    Psaroudaki and C

    C. Psaroudaki and C. Panagopoulos, Skyrmion Qubits: A New Class of Quantum Logic Elements Based on Nanoscale Magnetization, Phys. Rev. Lett.127, 067201 (2021)

  31. [31]

    Psaroudaki and C

    C. Psaroudaki and C. Panagopoulos, Skyrmion helicity: Quantization and quantum tunneling effects, Phys. Rev. B106, 104422 (2022)

  32. [32]

    Iwasaki, M

    J. Iwasaki, M. Mochizuki, and N. Nagaosa, Universal current-velocity relation of skyrmion motion in chiral magnets, Nat. Commun.4, 1463 (2013)

  33. [33]

    Sampaio, V

    J. Sampaio, V. Cros, S. Rohart, A. Thiaville, and A. Fert, Nucleation, stability and current-induced motion of iso- lated magnetic skyrmions in nanostructures, Nat. Nan- otechnol.8, 839 (2013)

  34. [34]

    A. Fert, V. Cros, and J. Sampaio, Skyrmions on the track, Nat. Nanotechnol.8, 152 (2013)

  35. [35]

    Chernyshov, M

    A. Chernyshov, M. Overby, X. Liu, J. K. Furdyna, Y. Lyanda-Geller, and L. P. Rokhinson, Evidence for re- versible control of magnetization in a ferromagnetic ma- terial by means of spin-orbit magnetic field, Nat. Phys. 5, 656 (2009)

  36. [36]

    I. M. Miron, G. Gaudin, S. Auffret, B. Rodmacq, A. Schuhl, S. Pizzini, J. Vogel, and P. Gambardella, Current-driven spin torque induced by the Rashba ef- fect in a ferromagnetic metal layer, Nat. Mater.9, 230 (2010)

  37. [37]

    I. M. Miron, K. Garello, G. Gaudin, P.-J. Zermatten, M. V. Costache, S. Auffret, S. Bandiera, B. Rodmacq, A. Schuhl, and P. Gambardella, Perpendicular switching of a single ferromagnetic layer induced by in-plane cur- rent injection, Nature476, 189 (2011)

  38. [38]

    J. Zang, M. Mostovoy, J. H. Han, and N. Nagaosa, Dy- namics of Skyrmion Crystals in Metallic Thin Films, Phys. Rev. Lett.107, 136804 (2011)

  39. [39]

    Matano, M

    K. Matano, M. Kriener, K. Segawa, Y. Ando, and G. qing Zheng, Spin-rotation symmetry breaking in the supercon- ducting state of Cu xBi2Se3, Nat. Phys.12, 852 (2016)

  40. [40]

    Jiang, X

    W. Jiang, X. Zhang, G. Yu, W. Zhang, X. Wang, M. B. Jungfleisch, J. E. Pearson, X. Cheng, O. Heinonen, K. L. Wang, Y. Zhou, A. Hoffmann, and S. G. E. te Velthuis, Direct observation of the skyrmion hall effect, Nat. Phys. 13, 162 (2017)

  41. [41]

    P.-J. Hsu, A. Kubetzka, A. Finco, N. Romming, K. von Bergmann, and R. Wiesendanger, Electric-field-driven switching of individual magnetic skyrmions, Nat. Nan- otechnol.12, 123 (2017)

  42. [42]

    Schott, A

    M. Schott, A. Bernand-Mantel, L. Ranno, S. Pizzini, J. Vogel, H. B´ ea, C. Baraduc, S. Auffret, G. Gaudin, and D. Givord, The Skyrmion Switch: Turning Magnetic Skyrmion Bubbles on and off with an Electric Field, Nano Lett.17, 3006 (2017)

  43. [43]

    M. A. Goerzen, S. von Malottki, G. J. Kwiatkowski, P. F. Bessarab, and S. Heinze, Atomistic spin simula- tions of electric-field-assisted nucleation and annihilation of magnetic skyrmions in Pd/Fe/Ir(111), Phys. Rev. B 105, 214435 (2022). 21

  44. [44]

    Paul and S

    S. Paul and S. Heinze, Electric-field driven stability con- trol of skyrmions in an ultrathin transition-metal film, npj Comput. Mater.8, 105 (2022)

  45. [45]

    C. Ma, X. Zhang, J. Xia, M. Ezawa, W. Jiang, T. Ono, S. N. Piramanayagam, A. Morisako, Y. Zhou, and X. Liu, Electric Field-Induced Creation and Directional Motion of Domain Walls and Skyrmion Bubbles, Nano Lett.19, 353 (2019)

  46. [46]

    Srivastava, M

    T. Srivastava, M. Schott, R. Juge, V. Kˇ riˇ z´ akov´ a, M. Belmeguenai, Y. Roussign´ e, A. Bernand-Mantel, L. Ranno, S. Pizzini, S.-M. Ch´ erif, A. Stashkevich, S. Auffret, O. Boulle, G. Gaudin, M. Chshiev, C. Bara- duc, and H. B´ ea, Large-Voltage Tuning of Dzyaloshinskii- Moriya Interactions: A Route toward Dynamic Control of Skyrmion Chirality, Nano L...

  47. [47]

    Y. Wang, L. Wang, J. Xia, Z. Lai, G. Tian, X. Zhang, Z. Hou, X. Gao, W. Mi, C. Feng, M. Zeng, G. Zhou, G. Yu, G. Wu, Y. Zhou, W. Wang, X.-x. Zhang, and J. Liu, Electric-field-driven non-volatile multi-state switching of individual skyrmions in a multiferroic het- erostructure, Nat. Commun.11, 3577 (2020)

  48. [48]

    Y. Ba, S. Zhuang, Y. Zhang, Y. Wang, Y. Gao, H. Zhou, M. Chen, W. Sun, Q. Liu, G. Chai, J. Ma, Y. Zhang, H. Tian, H. Du, W. Jiang, C. Nan, J.-M. Hu, and Y. Zhao, Electric-field control of skyrmions in multifer- roic heterostructure via magnetoelectric coupling, Nat. Commun.12, 322 (2021)

  49. [49]

    B. Dai, D. Wu, S. A. Razavi, S. Xu, H. He, Q. Shu, M. Jackson, F. Mahfouzi, H. Huang, Q. Pan, Y. Cheng, T. Qu, T. Wang, L. Tai, K. Wong, N. Kioussis, and K. L. Wang, Electric field manipulation of spin chirality and skyrmion dynamic, Sci. Adv.9, eade6836 (2023)

  50. [50]

    M.-G. Han, J. D. Thomsen, J. P. Philbin, J. Mun, E. Park, F. Camino, L. Dˇ ekanovsk´ y, C. Liu, Z. Sofer, P. Narang, F. M. Ross, and Y. Zhu, Electric Field Con- trol of Magnetic Skyrmion Helicity in a Centrosymmetric 2D van der Waals Magnet, Nano Letters25, 5174 (2025)

  51. [51]

    S. Paul, S. Haldar, S. von Malottki, and S. Heinze, Role of higher-order exchange interactions for skyrmion stability, Nat. Commun.11, 4756 (2020)

  52. [52]

    Upadhyaya, G

    P. Upadhyaya, G. Yu, P. K. Amiri, and K. L. Wang, Electric-field guiding of magnetic skyrmions, Phys. Rev. B92, 134411 (2015)

  53. [53]

    H. T. Fook, W. L. Gan, and W. S. Lew, Gateable skyrmion transport via field-induced potential barrier modulation, Sci. Rep.6, 21099 (2016)

  54. [54]

    Nakatani, M

    Y. Nakatani, M. Hayashi, S. Kanai, S. Fukami, and H. Ohno, Electric field control of Skyrmions in magnetic nanodisks, Appl. Phys. Lett.108, 152403 (2016)

  55. [55]

    M. Oba, K. Nakamura, T. Akiyama, T. Ito, M. Weinert, and A. J. Freeman, Electric-Field-Induced Modification of the Magnon Energy, Exchange Interaction, and Curie Temperature of Transition-Metal Thin Films, Phys. Rev. Lett.114, 107202 (2015)

  56. [56]

    H. Yang, O. Boulle, V. Cros, A. Fert, and M. Chshiev, Controlling Dzyaloshinskii-Moriya Interaction via Chi- rality Dependent Atomic-Layer Stacking, Insulator Cap- ping and Electric Field, Sci Rep8, 12356 (2018)

  57. [57]

    Desplat, S

    L. Desplat, S. Meyer, J. Bouaziz, P. M. Buhl, S. Lounis, B. Dup´ e, and P.-A. Hervieux, Mechanism for ultrafast electric-field driven skyrmion nucleation, Phys. Rev. B 104, L060409 (2021)

  58. [58]

    Li, X.-P

    C.-K. Li, X.-P. Yao, and G. Chen, Writing and delet- ing skyrmions with electric fields in a multiferroic het- erostructure, Phys. Rev. Res.3, L012026 (2021)

  59. [59]

    Muckel, S

    F. Muckel, S. von Malottki, C. Holl, B. Pestka, M. Pratzer, P. F. Bessarab, S. Heinze, and M. Mor- genstern, Experimental identification of two distinct skyrmion collapse mechanisms, Nature Physics17, 395 (2021)

  60. [60]

    Romming, H

    N. Romming, H. Pralow, A. Kubetzka, M. Hoffmann, S. von Malottki, S. Meyer, B. Dup´ e, R. Wiesendan- ger, K. von Bergmann, and S. Heinze, Competition of Dzyaloshinskii-Moriya and Higher-Order Exchange Inter- actions in Rh/Fe Atomic Bilayers on Ir(111), Phys. Rev. Lett.120, 207201 (2018)

  61. [61]

    Dup´ e, M

    B. Dup´ e, M. Hoffmann, C. Paillard, and S. Heinze, Tai- loring magnetic skyrmions in ultra-thin transition metal films, Nat. Commun.5, 4030 (2014)

  62. [62]

    von Malottki, B

    S. von Malottki, B. Dup´ e, P. F. Bessarab, A. Delin, and S. Heinze, Enhanced skyrmion stability due to exchange frustration, Sci. Rep.7, 12299 (2017)

  63. [63]

    Gutzeit, S

    M. Gutzeit, S. Haldar, S. Meyer, and S. Heinze, Trends of higher-order exchange interactions in transition metal trilayers, Phys. Rev. B104, 024420 (2021). [62]www.flapw.de

  64. [64]

    P. Kurz, F. F¨ orster, L. Nordstr¨ om, G. Bihlmayer, and S. Bl¨ ugel,Ab initiotreatment of noncollinear magnets with the full-potential linearized augmented plane wave method, Phys. Rev. B69, 024415 (2004)

  65. [65]

    Heide, G

    M. Heide, G. Bihlmayer, and S. Bl¨ ugel, Describing Dzyaloshinskii-Moriya spirals from first principles, Phys. B: Condens. Matter404, 2678 (2009)

  66. [66]

    Zimmermann, M

    B. Zimmermann, M. Heide, G. Bihlmayer, and S. Bl¨ ugel, First-principles analysis of a homochiral cycloidal mag- netic structure in a monolayer Cr on W(110), Phys. Rev. B90, 115427 (2014)

  67. [67]

    S. H. Vosko, L. Wilk, and M. Nusair, Accurate spin- dependent electron liquid correlation energies for local spin density calculations: a critical analysis, Can. J. Phys.58, 1200 (1980)

  68. [68]

    Hoffmann and S

    M. Hoffmann and S. Bl¨ ugel, Systematic derivation of re- alistic spin models for beyond-Heisenberg solids, Phys. Rev. B101, 024418 (2020)

  69. [69]

    A. H. MacDonald, S. M. Girvin, and D. Yoshioka, t U expansion for the Hubbard model, Phys. Rev. B37, 9753 (1988)

  70. [70]

    Takahashi, Half-filed Hubbard model at low temper- ature, J

    M. Takahashi, Half-filed Hubbard model at low temper- ature, J. Phys. C: Solid State Phys.10, 1289 (1977)

  71. [71]

    Hardrat, A

    B. Hardrat, A. Al-Zubi, P. Ferriani, S. Bl¨ ugel, G. Bihlmayer, and S. Heinze, Complex magnetism of iron monolayers on hexagonal transition metal surfaces from first principles, Phys. Rev. B79, 094411 (2009)

  72. [72]

    Kr¨ onlein, M

    A. Kr¨ onlein, M. Schmitt, M. Hoffmann, J. Kemmer, N. Seubert, M. Vogt, J. K¨ uspert, M. B¨ ohme, B. Alonazi, J. K¨ ugel, H. A. Albrithen, M. Bode, G. Bihlmayer, and S. Bl¨ ugel, Magnetic Ground State Stabilized by Three- Site Interactions: Fe/Rh(111), Phys. Rev. Lett.120, 207202 (2018)

  73. [73]

    P. Kurz, G. Bihlmayer, K. Hirai, and S. Bl¨ ugel, Three- Dimensional Spin Structure on a Two-Dimensional Lat- tice: Mn/Cu(111), Phys. Rev. Lett.86, 1106 (2001)

  74. [74]

    Spethmann, S

    J. Spethmann, S. Meyer, K. von Bergmann, R. Wiesen- danger, S. Heinze, and A. Kubetzka, Discovery of Mag- netic Single- and Triple-qStates in Mn/Re(0001), Phys. Rev. Lett.124, 227203 (2020)

  75. [75]

    Nickel, A

    F. Nickel, A. Kubetzka, S. Haldar, R. Wiesendanger, S. Heinze, and K. von Bergmann, Coupling of the triple- 22 q state to the atomic lattice by anisotropic symmetric exchange, Phys. Rev. B108, L180411 (2023)

  76. [76]

    Weinert, G

    M. Weinert, G. Schneider, R. Podloucky, and J. Redinger, FLAPW: applications and implemen- tations, J. Phys.: Condens. Matter21, 084201 (2009)

  77. [77]

    M. Hoffmann,Ab initio Studie komplexer magnetis- cher Strukturen an Oberfl¨ achen: Einfluss atomarer Ad- lagen und elektrischer Felder, Masterarbeit, Christian- Albrechts-Universit¨ at zu Kiel, Institut f¨ ur Theoretische Physik und Astrophysik, Kiel, Germany (2013)

  78. [78]

    D. S. G. Bauer,Development of a relativistic full- potential first-principles multiple scattering Green func- tion method applied to complex magnetic textures of nano structures at surfaces, Ph.D. thesis, J¨ ulich (2013)