2026
|
Schneider, M.; Butcher, T. A.; Wagner, S.; Metternich, D.; Klose, C.; Malm, E.; Battistelli, R.; Deinhart, V.; Fuchs, J.; Wittrock, S.; Karaman, T.; Joy, K. Puzhekadavil; Patra, M.; Büttner, F.; Wintz, S.; Weigand, M.; Günther, C. M.; Engel, D.; Gaal, P.; Schwarzkopf, J.; Pfau, B.; Eisebitt, S. Linear dichroic soft x-ray microscopy of ferroelectric stripe domains in epitaxial K0.6Na0.4NbO3 Journal Article Phys. Rev. B 114, L231401 (2026), datadoi: 10.5281/zenodo.22250213.. @article{schneiderLinearDichroicSoft2026,
title = {Linear dichroic soft x-ray microscopy of ferroelectric stripe domains in epitaxial K_{0.6}Na_{0.4}NbO_{3}},
author = {M. Schneider and T. A. Butcher and S. Wagner and D. Metternich and C. Klose and E. Malm and R. Battistelli and V. Deinhart and J. Fuchs and S. Wittrock and T. Karaman and K. Puzhekadavil Joy and M. Patra and F. Büttner and S. Wintz and M. Weigand and C. M. Günther and D. Engel and P. Gaal and J. Schwarzkopf and B. Pfau and S. Eisebitt},
url = {https://link.aps.org/doi/10.1103/kcjc-dtj6},
doi = {10.1103/kcjc-dtj6},
year = {2026},
date = {2026-10-02},
urldate = {2026-10-01},
journal = {Phys. Rev. B},
volume = {114},
number = {23},
pages = {L231401},
publisher = {American Physical Society},
abstract = {Functional properties of ferroelectric thin films are governed by domains that can be engineered by epitaxial strain. Soft x-ray microscopy can image domain structures with elemental and electronic sensitivity, but hitherto its application to strain-stabilized domains has been hindered by the absorption of soft x-rays in epitaxial substrates. Here, it is demonstrated how this limitation can be overcome by locally back-thinning the (110) TbScO3 substrate of epitaxial K0.6Na0.4NbO3 ferroelectric thin films to achieve soft x-ray transparency at the O K-edge around 530 eV. Strain-induced ferroelectric stripe domains with periods down to 44 nm were resolved by scanning transmission x-ray microscopy and coherent diffractive imaging by exploiting the x-ray linear dichroism of hybridized O 2𝑝–Nb 4𝑑 states, providing sensitivity to in-plane polarization components under normal incidence. The results establish soft x-ray microscopy for nanoscale imaging of epitaxial ferroelectric domain structures and open perspectives for time-resolved studies thereof.},
note = {datadoi: 10.5281/zenodo.22250213.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Functional properties of ferroelectric thin films are governed by domains that can be engineered by epitaxial strain. Soft x-ray microscopy can image domain structures with elemental and electronic sensitivity, but hitherto its application to strain-stabilized domains has been hindered by the absorption of soft x-rays in epitaxial substrates. Here, it is demonstrated how this limitation can be overcome by locally back-thinning the (110) TbScO3 substrate of epitaxial K0.6Na0.4NbO3 ferroelectric thin films to achieve soft x-ray transparency at the O K-edge around 530 eV. Strain-induced ferroelectric stripe domains with periods down to 44 nm were resolved by scanning transmission x-ray microscopy and coherent diffractive imaging by exploiting the x-ray linear dichroism of hybridized O 2𝑝–Nb 4𝑑 states, providing sensitivity to in-plane polarization components under normal incidence. The results establish soft x-ray microscopy for nanoscale imaging of epitaxial ferroelectric domain structures and open perspectives for time-resolved studies thereof. |  |
Toyoda, S.; Kocsis, V.; Tokunaga, Y.; Kézsmárki, I.; Taguchi, Y.; Arima, T.; Tokura, Y.; Ogawa, N. All-optical control of antiferromagnetic domains via an inverse optical magnetoelectric effect Journal Article Nat. Mater. 25, 1572 (2026), datadoi: 10.1038/s41563-026-02608-4. @article{toyodaAllopticalControlAntiferromagnetic2026,
title = {All-optical control of antiferromagnetic domains via an inverse optical magnetoelectric effect},
author = {S. Toyoda and V. Kocsis and Y. Tokunaga and I. Kézsmárki and Y. Taguchi and T. Arima and Y. Tokura and N. Ogawa},
url = {https://doi.org/10.1038/s41563-026-02608-4},
doi = {10.1038/s41563-026-02608-4},
year = {2026},
date = {2026-05-15},
urldate = {2026-05-01},
journal = {Nat. Mater.},
volume = {25},
pages = {1572},
abstract = {All-optical control of antiferromagnetic order is essential for realizing next-generation energy-efficient spintronic and high-speed memory applications. However, the optical writing of antiferromagnetic domains remains a fundamental challenge, because conventional opto-magnetic recording techniques rely on net magnetization, which is absent in antiferromagnets. In certain multiferroic antiferromagnets, the magnetic toroidal moment provides an additional degree of freedom through its inherent magnetoelectric coupling, which manifests as directional asymmetry in light propagation. Here we demonstrate the all-optical writing of antiferromagnetic domains using the inverse optical magnetoelectric effect in ferrotoroidic LiNiPO4, driven solely by reversing the light propagation direction. This directional control arises from a strong coupling between the photon linear momentum and the magnetic toroidal moment, enabling non-volatile, deterministic and repeatable switching between time-reversed domains with arbitrary light polarization. Our findings establish an inverse optical magnetoelectric effect as a distinct mechanism for manipulating antiferromagnetic order, opening a new paradigm in opto-magnetism driven by photon momentum.},
note = {datadoi: 10.1038/s41563-026-02608-4},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
All-optical control of antiferromagnetic order is essential for realizing next-generation energy-efficient spintronic and high-speed memory applications. However, the optical writing of antiferromagnetic domains remains a fundamental challenge, because conventional opto-magnetic recording techniques rely on net magnetization, which is absent in antiferromagnets. In certain multiferroic antiferromagnets, the magnetic toroidal moment provides an additional degree of freedom through its inherent magnetoelectric coupling, which manifests as directional asymmetry in light propagation. Here we demonstrate the all-optical writing of antiferromagnetic domains using the inverse optical magnetoelectric effect in ferrotoroidic LiNiPO4, driven solely by reversing the light propagation direction. This directional control arises from a strong coupling between the photon linear momentum and the magnetic toroidal moment, enabling non-volatile, deterministic and repeatable switching between time-reversed domains with arbitrary light polarization. Our findings establish an inverse optical magnetoelectric effect as a distinct mechanism for manipulating antiferromagnetic order, opening a new paradigm in opto-magnetism driven by photon momentum. |  |
Liefferink, R.; Körber, L.; Gerlinger, K.; Pfau, B.; Büttner, F.; Mentink, J. H. Effective Theory of Ultrafast Skyrmion Nucleation Journal Article Phys. Rev. Lett. 136, 146705 (2026), datadoi: 10.34973/5168-bn56. @article{liefferinkEffectiveTheoryUltrafast2026,
title = {Effective Theory of Ultrafast Skyrmion Nucleation},
author = {R. Liefferink and L. Körber and K. Gerlinger and B. Pfau and F. Büttner and J. H. Mentink},
url = {https://link.aps.org/doi/10.1103/brnt-2m9l},
doi = {10.1103/brnt-2m9l},
issn = {0031-9007, 1079-7114},
year = {2026},
date = {2026-04-10},
urldate = {2026-04-10},
journal = {Phys. Rev. Lett.},
volume = {136},
number = {14},
pages = {146705},
note = {datadoi: 10.34973/5168-bn56},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
|  |
Koraltan, S.; Sunny, J.; Karaman, T.; Peremadathil‐Pradeep, R.; Darwin, E.; Büttner, F.; Suess, D.; Hug, H. J.; Albrecht, M. Magnetic Force Microscopy Signatures of Higher‐Order Skyrmions and Antiskyrmions Journal Article Adv. Funct. Mater. 36, (2026). @article{koraltanMagneticForceMicroscopy2026,
title = {Magnetic Force Microscopy Signatures of Higher‐Order Skyrmions and Antiskyrmions},
author = {S. Koraltan and J. Sunny and T. Karaman and R. Peremadathil‐Pradeep and E. Darwin and F. Büttner and D. Suess and H. J. Hug and M. Albrecht},
url = {http://dx.doi.org/10.1002/adfm.202525716},
doi = {10.1002/adfm.202525716},
year = {2026},
date = {2026-03-13},
urldate = {2026-03-13},
journal = {Adv. Funct. Mater.},
volume = {36},
number = {41},
publisher = {Wiley},
abstract = {Higher-order skyrmions and antiskyrmions are topologically protected spin textures with integer topological charges beyond
±1, typically nucleating from vertical Bloch lines in domain walls. Until now, they have been reported only in ferromagnetic multilayers by Lorentz transmission electron microscopy (LTEM), which requires growth on ultrathin membranes and complicates their integration into spintronic devices. Moreover, LTEM often yields contrast patterns that are difficult to unambiguously assign to specific topological charges. Here, we demonstrate that magnetic force microscopy (MFM) operated under vacuum conditions provides a robust route to identify and distinguish higher-order spin textures in Co/Ni multilayers at room temperature. Supported by micromagnetic simulations, we show that MFM can resolve vertical Bloch lines as well as skyrmions and antiskyrmions with arbitrary charge. Our results establish advanced MFM as a powerful technique for the qualitative classification of complex spin textures, paving the way for their exploration and utilization in future skyrmionic device concepts.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Higher-order skyrmions and antiskyrmions are topologically protected spin textures with integer topological charges beyond
±1, typically nucleating from vertical Bloch lines in domain walls. Until now, they have been reported only in ferromagnetic multilayers by Lorentz transmission electron microscopy (LTEM), which requires growth on ultrathin membranes and complicates their integration into spintronic devices. Moreover, LTEM often yields contrast patterns that are difficult to unambiguously assign to specific topological charges. Here, we demonstrate that magnetic force microscopy (MFM) operated under vacuum conditions provides a robust route to identify and distinguish higher-order spin textures in Co/Ni multilayers at room temperature. Supported by micromagnetic simulations, we show that MFM can resolve vertical Bloch lines as well as skyrmions and antiskyrmions with arbitrary charge. Our results establish advanced MFM as a powerful technique for the qualitative classification of complex spin textures, paving the way for their exploration and utilization in future skyrmionic device concepts. |  |
2025
|
Zhou, S.; Litzius, K.; Büttner, F.; Caretta, L. Statistical Signatures of Topology and Chirality in the Annihilation Field Distributions of Magnetic Thin Films Journal Article Adv. Funct. Mater. 36, (2025). @article{zhouStatisticalSignaturesTopology2025,
title = {Statistical Signatures of Topology and Chirality in the Annihilation Field Distributions of Magnetic Thin Films},
author = {S. Zhou and K. Litzius and F. Büttner and L. Caretta},
url = {http://dx.doi.org/10.1002/adfm.202526052},
doi = {10.1002/adfm.202526052},
year = {2025},
date = {2025-12-17},
urldate = {2025-12-01},
journal = {Adv. Funct. Mater.},
volume = {36},
number = {19},
publisher = {Wiley},
abstract = {Magnetic skyrmions are winding spin textures whose proposed stability underpins their promise for next-generation spintronic devices. While this topological stabilization is widely theorized to suppress collapse and disorder-driven annihilation, direct experimental validation has remained challenging, often requiring complex imaging techniques or indirect electrical probes. Here, a simple and general method is introduced to probe skyrmion topology statistically by analyzing annihilation field distributions in large skyrmion bubble arrays using wide-field Kerr microscopy. By systematically applying in-plane (IP) magnetic fields, the skyrmion topology is continuously tuned, enabling transitions from topologically nontrivial to trivial states. It is found that this topological transition drives a clear shift in annihilation behavior: from broad, thermally activated distributions (stochastic collapse) to narrow, sharply defined distributions (deterministic collapse), confirmed by micromagnetic simulations. This direct correlation between topological state and statistical stability provides a new route for chirality detection and skyrmion state control. This method enables accessible identification of skyrmion topology and opens new possibilities for device concepts: deterministic collapse for synchronized skyrmion deletion in memory, and topology-tunable stochasticity for probabilistic computing and random bit generation.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Magnetic skyrmions are winding spin textures whose proposed stability underpins their promise for next-generation spintronic devices. While this topological stabilization is widely theorized to suppress collapse and disorder-driven annihilation, direct experimental validation has remained challenging, often requiring complex imaging techniques or indirect electrical probes. Here, a simple and general method is introduced to probe skyrmion topology statistically by analyzing annihilation field distributions in large skyrmion bubble arrays using wide-field Kerr microscopy. By systematically applying in-plane (IP) magnetic fields, the skyrmion topology is continuously tuned, enabling transitions from topologically nontrivial to trivial states. It is found that this topological transition drives a clear shift in annihilation behavior: from broad, thermally activated distributions (stochastic collapse) to narrow, sharply defined distributions (deterministic collapse), confirmed by micromagnetic simulations. This direct correlation between topological state and statistical stability provides a new route for chirality detection and skyrmion state control. This method enables accessible identification of skyrmion topology and opens new possibilities for device concepts: deterministic collapse for synchronized skyrmion deletion in memory, and topology-tunable stochasticity for probabilistic computing and random bit generation. |  |
Kovács, A.; Weber, J. T.; Charilaou, M.; Kong, D.; Prodan, L.; Tsurkan, V.; Schröder, A.; Kiselev, N. S.; Kézsmárki, I.; Dunin-Borkowski, R. E.; Tavabi, A. H.; Schäfer, S. All-optical stochastic switching of magnetisation textures in Fe3Sn2 Journal Article Commun. Mater. 6, 223 (2025). @article{kovacs_all-optical_2025,
title = {All-optical stochastic switching of magnetisation textures in Fe_{3}Sn_{2}},
author = {A. Kovács and J. T. Weber and M. Charilaou and D. Kong and L. Prodan and V. Tsurkan and A. Schröder and N. S. Kiselev and I. Kézsmárki and R. E. Dunin-Borkowski and A. H. Tavabi and S. Schäfer},
url = {https://doi.org/10.1038/s43246-025-00974-1},
doi = {10.1038/s43246-025-00974-1},
year = {2025},
date = {2025-10-14},
urldate = {2025-10-01},
journal = {Commun. Mater.},
volume = {6},
number = {1},
pages = {223},
abstract = {The all-optical control of magnetisation at room temperature broadens the scope of applications of spin degrees-of-freedom in data storage, spintronics, and quantum computing. Topological magnetic spin structures, such as skyrmions, are of particular interest due to their particle-like properties, small size and inherent stability. Controlling skyrmion states without strong magnetic fields or large current densities would create new possibilities for their application. In this work, we utilize femtosecond optical pulses to alter the helicity of the spin configuration in dipolar skyrmions formed in the kagome magnet Fe3Sn2 in the absence of an external magnetic field and at room temperature. In situ Lorentz transmission electron microscopy is used to visualise the light-induced stochastic switching process of chiral Néel caps, while the internal Bloch component of the dipolar skyrmions remains unchanged. In addition to this switching process, we observe the interconversion between type I skyrmionic and type II bubble configurations depending on the external magnetic field and illumination conditions. To corroborate the spin states and the light-induced magnetisation dynamics, micromagnetic modelling and simulations of the resulting electron phase shift maps are conducted to elucidate the spin rearrangement induced by individual femtosecond optical pulses.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
The all-optical control of magnetisation at room temperature broadens the scope of applications of spin degrees-of-freedom in data storage, spintronics, and quantum computing. Topological magnetic spin structures, such as skyrmions, are of particular interest due to their particle-like properties, small size and inherent stability. Controlling skyrmion states without strong magnetic fields or large current densities would create new possibilities for their application. In this work, we utilize femtosecond optical pulses to alter the helicity of the spin configuration in dipolar skyrmions formed in the kagome magnet Fe3Sn2 in the absence of an external magnetic field and at room temperature. In situ Lorentz transmission electron microscopy is used to visualise the light-induced stochastic switching process of chiral Néel caps, while the internal Bloch component of the dipolar skyrmions remains unchanged. In addition to this switching process, we observe the interconversion between type I skyrmionic and type II bubble configurations depending on the external magnetic field and illumination conditions. To corroborate the spin states and the light-induced magnetisation dynamics, micromagnetic modelling and simulations of the resulting electron phase shift maps are conducted to elucidate the spin rearrangement induced by individual femtosecond optical pulses. |  |
Ghara, S.; Winkler, M.; Schmid, S. W.; Prodan, L.; Geirhos, K.; Tsurkan, V.; Ge, Wenbo; Wu, Weida; Halbritter, A.; Krohns, S.; Kézsmárki, I. Nonvolatile electric control of antiferromagnetic states on nanosecond timescales Journal Article Phys. Rev. Lett. 135, 126704 (2025), datadoi: 10.5281/zenodo.16949831. @article{gharaNonvolatileElectricControl2025,
title = {Nonvolatile electric control of antiferromagnetic states on nanosecond timescales},
author = {S. Ghara and M. Winkler and S. W. Schmid and L. Prodan and K. Geirhos and V. Tsurkan and Wenbo Ge and Weida Wu and A. Halbritter and S. Krohns and I. Kézsmárki},
url = {https://link.aps.org/doi/10.1103/yzrk-h3rz},
doi = {10.1103/yzrk-h3rz},
year = {2025},
date = {2025-09-18},
urldate = {2025-09-18},
journal = {Phys. Rev. Lett.},
volume = {135},
number = {12},
pages = {126704},
abstract = {Electrical manipulation of antiferromagnetic (AFM) states, a cornerstone of AFM spintronics, is a great challenge, requiring novel material platforms. Here we report the full control over AFM states by voltage pulses in the insulating Co3O4 spinel well below its Néel temperature. We show that the strong linear magnetoelectric effect is fully governed by the orientation of the Néel vector. As a unique feature of Co3O4, the magnetoelectric energy can easily overcome the weak magnetocrystalline anisotropy; thus, the Néel vector can be manipulated on demand, either rotated smoothly or reversed suddenly, by combined electric and magnetic fields. We achieve the nonvolatile switching within a few tens of nanoseconds between time-reversed AFM states in macroscopic volumes by voltage pulses. These observations render quasicubic antiferromagnets, like Co3O4, an ideal platform for the ultrafast (picosecond to nanosecond) manipulation of microscopic AFM domains and may pave the way for the realization of AFM spintronic devices.},
note = {datadoi: 10.5281/zenodo.16949831},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Electrical manipulation of antiferromagnetic (AFM) states, a cornerstone of AFM spintronics, is a great challenge, requiring novel material platforms. Here we report the full control over AFM states by voltage pulses in the insulating Co3O4 spinel well below its Néel temperature. We show that the strong linear magnetoelectric effect is fully governed by the orientation of the Néel vector. As a unique feature of Co3O4, the magnetoelectric energy can easily overcome the weak magnetocrystalline anisotropy; thus, the Néel vector can be manipulated on demand, either rotated smoothly or reversed suddenly, by combined electric and magnetic fields. We achieve the nonvolatile switching within a few tens of nanoseconds between time-reversed AFM states in macroscopic volumes by voltage pulses. These observations render quasicubic antiferromagnets, like Co3O4, an ideal platform for the ultrafast (picosecond to nanosecond) manipulation of microscopic AFM domains and may pave the way for the realization of AFM spintronic devices. |  |
Szaller, D.; Prodan, L.; Geirhos, K.; Felea, V.; Skourski, Y.; Gorbunov, D.; Förster, T.; Helm, T.; Nomura, T.; Miyata, A.; Zherlitsyn, S.; Wosnitza, J.; Tsirlin, A. A.; Tsurkan, V.; Kézsmárki, I. Coexistence of antiferromagnetism and ferrimagnetism in adjacent honeycomb layers Journal Article Phys. Rev. B 111, 184404 (2025). @article{szaller_coexistence_2025,
title = {Coexistence of antiferromagnetism and ferrimagnetism in adjacent honeycomb layers},
author = {D. Szaller and L. Prodan and K. Geirhos and V. Felea and Y. Skourski and D. Gorbunov and T. Förster and T. Helm and T. Nomura and A. Miyata and S. Zherlitsyn and J. Wosnitza and A. A. Tsirlin and V. Tsurkan and I. Kézsmárki},
url = {https://link.aps.org/doi/10.1103/PhysRevB.111.184404},
doi = {10.1103/PhysRevB.111.184404},
year = {2025},
date = {2025-05-02},
urldate = {2025-05-02},
journal = {Phys. Rev. B},
volume = {111},
number = {18},
pages = {184404},
abstract = {Ferro-/ferri- and antiferromagnetically ordered phases are typically exclusive in nature, thus, their coexistence in atomic-scale proximity is expected only in heterostructures. Breaking this paradigm and broadening the range of unconventional magnetic states, we report here on the observation of a new, atomic-scale hybrid spin state. This ordering is stabilized in three-dimensional crystals of the polar antiferromagnet Co2Mo3O8 by magnetic fields applied perpendicular to the Co honeycomb layers and possesses a spontaneous in-plane ferromagnetic moment. Our microscopic spin model, capturing the observed field dependence of the longitudinal and transverse magnetization as well as the magnetoelectric/elastic properties, reveals that this novel spin state is composed of an alternating stacking of antiferromagnetic and ferrimagnetic honeycomb layers. The strong intralayer and the weak interlayer exchange couplings together with competing anisotropies at octahedral and tetrahedral Co sites are identified as the key ingredients to stabilize antiferromagnetic and ferrimagnetic layers in such close proximity. We show that the proper balance of magnetic interactions can extend the stability range of this hybrid phase down to zero magnetic field. The possibility to realize a layer-by-layer stacking of such distinct spin orders via suitable combinations of microscopic interactions opens a new dimension toward the nanoscale engineering of magnetic states.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Ferro-/ferri- and antiferromagnetically ordered phases are typically exclusive in nature, thus, their coexistence in atomic-scale proximity is expected only in heterostructures. Breaking this paradigm and broadening the range of unconventional magnetic states, we report here on the observation of a new, atomic-scale hybrid spin state. This ordering is stabilized in three-dimensional crystals of the polar antiferromagnet Co2Mo3O8 by magnetic fields applied perpendicular to the Co honeycomb layers and possesses a spontaneous in-plane ferromagnetic moment. Our microscopic spin model, capturing the observed field dependence of the longitudinal and transverse magnetization as well as the magnetoelectric/elastic properties, reveals that this novel spin state is composed of an alternating stacking of antiferromagnetic and ferrimagnetic honeycomb layers. The strong intralayer and the weak interlayer exchange couplings together with competing anisotropies at octahedral and tetrahedral Co sites are identified as the key ingredients to stabilize antiferromagnetic and ferrimagnetic layers in such close proximity. We show that the proper balance of magnetic interactions can extend the stability range of this hybrid phase down to zero magnetic field. The possibility to realize a layer-by-layer stacking of such distinct spin orders via suitable combinations of microscopic interactions opens a new dimension toward the nanoscale engineering of magnetic states. |  |
Kern, L. -M.; Kuchkin, V. M.; Deinhart, V.; Klose, C.; Sidiropoulos, T.; Auer, M.; Gaebel, S.; Gerlinger, K.; Battistelli, R.; Wittrock, S.; Karaman, T.; Schneider, M.; Günther, C. M.; Engel, D.; Will, I.; Wintz, S.; Weigand, M.; Büttner, F.; Höflich, K.; Eisebitt, S.; Pfau, B. Controlled Formation of Skyrmion Bags Journal Article Adv. Mater. 2501250 (2025), (contributed). @article{kern_controlled_2025,
title = {Controlled Formation of Skyrmion Bags},
author = {L. -M. Kern and V. M. Kuchkin and V. Deinhart and C. Klose and T. Sidiropoulos and M. Auer and S. Gaebel and K. Gerlinger and R. Battistelli and S. Wittrock and T. Karaman and M. Schneider and C. M. Günther and D. Engel and I. Will and S. Wintz and M. Weigand and F. Büttner and K. Höflich and S. Eisebitt and B. Pfau},
url = {https://advanced.onlinelibrary.wiley.com/doi/abs/10.1002/adma.202501250},
doi = {10.1002/adma.202501250},
year = {2025},
date = {2025-04-28},
urldate = {2025-04-01},
journal = {Adv. Mater.},
pages = {2501250},
abstract = {Abstract Topologically non-trivial magnetic solitons are complex spin textures with a distinct single-particle nature. Although magnetic skyrmions, especially those with unity topological charge, have attracted substantial interest due to their potential applications, more complex topological textures remain largely theoretical. In this work, the stabilization of isolated higher-order skyrmion bags beyond the prototypical π-skyrmion in ferromagnetic thin films is experimentally demonstrate, which has posed considerable challenges to date. Specifically, controlled generation of skyrmionium (2π-skyrmion), target skyrmion (3π-skyrmion), and skyrmion bags (with variable topological charge) are achieved through the introduction of artificially engineered anisotropy defects via local ion irradiation. They act as preferential sites for the field- or laser-induced nucleation of skyrmion bags. Remarkably, ultrafast laser pulses achieve a substantially higher conversion rate transforming skyrmions into higher-order skyrmion bags compared to their formation driven by magnetic fields. High-resolution x-ray imaging enables direct observation of the resulting skyrmion bags. Complementary micromagnetic simulations reveal the pivotal role of defect geometry–particularly diameter–in stabilizing closed-loop domain textures. The findings not only broaden the experimental horizon for skyrmion research, but also suggest strategies for exploiting complex topological spin textures within a unified material platform for practical applications.},
note = {(contributed)},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Abstract Topologically non-trivial magnetic solitons are complex spin textures with a distinct single-particle nature. Although magnetic skyrmions, especially those with unity topological charge, have attracted substantial interest due to their potential applications, more complex topological textures remain largely theoretical. In this work, the stabilization of isolated higher-order skyrmion bags beyond the prototypical π-skyrmion in ferromagnetic thin films is experimentally demonstrate, which has posed considerable challenges to date. Specifically, controlled generation of skyrmionium (2π-skyrmion), target skyrmion (3π-skyrmion), and skyrmion bags (with variable topological charge) are achieved through the introduction of artificially engineered anisotropy defects via local ion irradiation. They act as preferential sites for the field- or laser-induced nucleation of skyrmion bags. Remarkably, ultrafast laser pulses achieve a substantially higher conversion rate transforming skyrmions into higher-order skyrmion bags compared to their formation driven by magnetic fields. High-resolution x-ray imaging enables direct observation of the resulting skyrmion bags. Complementary micromagnetic simulations reveal the pivotal role of defect geometry–particularly diameter–in stabilizing closed-loop domain textures. The findings not only broaden the experimental horizon for skyrmion research, but also suggest strategies for exploiting complex topological spin textures within a unified material platform for practical applications. |  |
Metternich, D.; Litzius, K.; Wintz, S.; Gerlinger, K.; Petz, S.; Engel, D.; Sidiropoulos, T.; Battistelli, R.; Steinbach, F.; Weigand, M.; Wittrock, S.; Schmising, C. Korff; Büttner, F. Defects in magnetic domain walls after single-shot all-optical switching Journal Article Struct. Dyn. 12, 024504 (2025), datadoi: (10.5281/zenodo.14499566). @article{metternichDefectsMagneticDomain2025,
title = {Defects in magnetic domain walls after single-shot all-optical switching},
author = {D. Metternich and K. Litzius and S. Wintz and K. Gerlinger and S. Petz and D. Engel and T. Sidiropoulos and R. Battistelli and F. Steinbach and M. Weigand and S. Wittrock and C. Korff Schmising and F. Büttner},
url = {https://doi.org/10.1063/4.0000287},
doi = {10.1063/4.0000287},
year = {2025},
date = {2025-04-18},
urldate = {2025-04-01},
journal = {Struct. Dyn.},
volume = {12},
number = {2},
pages = {024504},
abstract = {Helicity-independent all-optical switching (HI-AOS) is the fastest known way to switch the magnetic order parameter. While the switching process of extended areas is well understood, the formation of domain walls enclosing switched areas remains less explored. Here, we study domain walls around all-optically nucleated magnetic domains using x-ray vector spin imaging and observe a high density of vertical Bloch line defects. Surprisingly, the defect density appears to be independent of optical pulse parameters, significantly varies between materials, and is only slightly higher than in domain walls generated by field cycling. A possible explanation is given by time-resolved Kerr microscopy, which reveals that magnetic domains considerably expand after the initial AOS process. During this expansion, and likewise during field cycling, domain walls propagate at speeds above the Walker breakdown. Micromagnetic simulations suggest that at such speeds, domain walls accumulate defects when moving over magnetic pinning sites, explaining similar defect densities after two very different switching processes. The slightly larger defect density after AOS compared to field-induced switching indicates that some defects are created already when the domain wall comes into existence. Our work shows that engineered low-pinning materials are a key ingredient to uncover the intrinsic dynamics of domain wall formation during ultrafast all-optical switching.},
note = {datadoi: (10.5281/zenodo.14499566)},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Helicity-independent all-optical switching (HI-AOS) is the fastest known way to switch the magnetic order parameter. While the switching process of extended areas is well understood, the formation of domain walls enclosing switched areas remains less explored. Here, we study domain walls around all-optically nucleated magnetic domains using x-ray vector spin imaging and observe a high density of vertical Bloch line defects. Surprisingly, the defect density appears to be independent of optical pulse parameters, significantly varies between materials, and is only slightly higher than in domain walls generated by field cycling. A possible explanation is given by time-resolved Kerr microscopy, which reveals that magnetic domains considerably expand after the initial AOS process. During this expansion, and likewise during field cycling, domain walls propagate at speeds above the Walker breakdown. Micromagnetic simulations suggest that at such speeds, domain walls accumulate defects when moving over magnetic pinning sites, explaining similar defect densities after two very different switching processes. The slightly larger defect density after AOS compared to field-induced switching indicates that some defects are created already when the domain wall comes into existence. Our work shows that engineered low-pinning materials are a key ingredient to uncover the intrinsic dynamics of domain wall formation during ultrafast all-optical switching. |  |
Battistelli, R.; Körber, L.; Litzius, K.; Grelier, M.; Joy, K. P.; Schneider, M.; Wittrock, S.; Metternich, D.; Karaman, T.; Kern, L. -M.; Klose, C.; Finizio, S.; Fuchs, J.; Günther, C. M.; Butcher, T. A.; Prokeš, K.; Boltje, R.; Patra, M.; Wintz, S.; Weigand, M.; Petz, S.; Popescu, H.; Raabe, J.; Jaouen, N.; Eisebitt, S.; Cros, V.; Pfau, B.; Mentink, J. H.; Reyren, N.; Büttner, F. A fluctuation-free pathway for a topological magnetic phase transition Unpublished (2025), arXiv:2512.22947
datadoi: 10.5281/zenodo.18004538. @unpublished{battistelliFluctuationfreePathwayTopological2025,
title = {A fluctuation-free pathway for a topological magnetic phase transition},
author = {R. Battistelli and L. Körber and K. Litzius and M. Grelier and K. P. Joy and M. Schneider and S. Wittrock and D. Metternich and T. Karaman and L. -M. Kern and C. Klose and S. Finizio and J. Fuchs and C. M. Günther and T. A. Butcher and K. Prokeš and R. Boltje and M. Patra and S. Wintz and M. Weigand and S. Petz and H. Popescu and J. Raabe and N. Jaouen and S. Eisebitt and V. Cros and B. Pfau and J. H. Mentink and N. Reyren and F. Büttner},
url = {https://arxiv.org/abs/2512.22947},
doi = {10.48550/arXiv.2512.22947},
year = {2025},
date = {2025-12-28},
urldate = {2025-12-01},
abstract = {Topological magnetic textures are particle-like spin configurations stabilized by competing interactions. Their formation is commonly attributed to fluctuation-driven, first-order nucleation processes requiring activation over a topological energy barrier. Here, we demonstrate an alternative barrier- and fluctuation-free pathway for nucleating topological magnetic textures, triggered in our experiments by an excitation-induced spin reorientation transition. By combining x-ray imaging, scattering and micromagnetic simulations, we show that the system follows a deterministic cascade of symmetry-breaking phase transitions after excitation. First, the system undergoes a second-order phase transition from a homogeneous state to weak stripe domains, then a first-order transition to topologically trivial bubbles, and finally a topological switching event into skyrmionic textures. Through simulations, we generalize our findings and demonstrate that this pathway is active in a vast range of low-anisotropy materials. This previously unrecognized, spontaneous transition pathway suggests strategies for rapid, low-energy generation of topological spin textures and points to a general role of intrinsic modulational instabilities in phase transitions beyond magnetism.},
note = {arXiv:2512.22947
datadoi: 10.5281/zenodo.18004538},
keywords = {},
pubstate = {published},
tppubtype = {unpublished}
}
Topological magnetic textures are particle-like spin configurations stabilized by competing interactions. Their formation is commonly attributed to fluctuation-driven, first-order nucleation processes requiring activation over a topological energy barrier. Here, we demonstrate an alternative barrier- and fluctuation-free pathway for nucleating topological magnetic textures, triggered in our experiments by an excitation-induced spin reorientation transition. By combining x-ray imaging, scattering and micromagnetic simulations, we show that the system follows a deterministic cascade of symmetry-breaking phase transitions after excitation. First, the system undergoes a second-order phase transition from a homogeneous state to weak stripe domains, then a first-order transition to topologically trivial bubbles, and finally a topological switching event into skyrmionic textures. Through simulations, we generalize our findings and demonstrate that this pathway is active in a vast range of low-anisotropy materials. This previously unrecognized, spontaneous transition pathway suggests strategies for rapid, low-energy generation of topological spin textures and points to a general role of intrinsic modulational instabilities in phase transitions beyond magnetism. |  |
Metternich, D.; Schneider, M.; Mercurio, G.; Hegstad, T.; Möller, M.; Battistelli, R.; Klose, C.; Wittrock, S.; Patra, M. R.; Joy, K. P.; Deinhart, V.; Petz, S.; Prokes, K.; Wintz, S.; Weigand, M.; Engel, W. -D.; Sidiropoulos, T.; Will, I.; Eisebitt, S.; Carley, R. E.; Mercadier, L.; Schlappa, J.; Teichmann, M.; Scherz, A.; Zayko, S.; Sorokin, B. V.; Bagschik, K.; Ropers, C.; Mentink, J. H.; Pfau, B.; Büttner, F. Picosecond localization dynamics following ultrafast nanoscale magnetic switching Unpublished (2025), arXiv:2512.17643. @unpublished{metternichPicosecondLocalizationDynamics2025,
title = {Picosecond localization dynamics following ultrafast nanoscale magnetic switching},
author = {D. Metternich and M. Schneider and G. Mercurio and T. Hegstad and M. Möller and R. Battistelli and C. Klose and S. Wittrock and M. R. Patra and K. P. Joy and V. Deinhart and S. Petz and K. Prokes and S. Wintz and M. Weigand and W. -D. Engel and T. Sidiropoulos and I. Will and S. Eisebitt and R. E. Carley and L. Mercadier and J. Schlappa and M. Teichmann and A. Scherz and S. Zayko and B. V. Sorokin and K. Bagschik and C. Ropers and J. H. Mentink and B. Pfau and F. Büttner},
url = {https://arxiv.org/abs/2512.17643},
doi = {https://doi.org/10.48550/arXiv.2512.17643},
year = {2025},
date = {2025-12-19},
urldate = {2025-12-01},
abstract = {Ultrashort laser pulses provide the fastest known way to switch magnetic order. Such excitation commonly creates nanometer-scale domains, even after homogeneous illumination when the position of nucleated domains is not externally defined. However, the physics of domain localization during such ultrafast phase transitions remains unresolved. Here, we use shot-resolved pump-probe resonant x-ray scattering together with a material featuring a periodically modulated magnetic anisotropy landscape to track, in real time, the laser-driven nucleation and localization of nanometer-scale spin textures. We find that nucleation and localization are two distinct processes. Nucleation occurs homogeneously via fluctuations at early times, whereas spatially periodic structures emerge only later and, under suitable conditions, localize in less than one nanosecond. Real-space simulations show that this localization is governed by strong lateral variations in spin-texture lifetimes. Our results demonstrate that ultrafast phase-transition dynamics fundamentally differ from conventional transitions, yet still can be controlled through moderate nanometer-scale tailoring of the energy landscape.},
note = {arXiv:2512.17643},
keywords = {},
pubstate = {published},
tppubtype = {unpublished}
}
Ultrashort laser pulses provide the fastest known way to switch magnetic order. Such excitation commonly creates nanometer-scale domains, even after homogeneous illumination when the position of nucleated domains is not externally defined. However, the physics of domain localization during such ultrafast phase transitions remains unresolved. Here, we use shot-resolved pump-probe resonant x-ray scattering together with a material featuring a periodically modulated magnetic anisotropy landscape to track, in real time, the laser-driven nucleation and localization of nanometer-scale spin textures. We find that nucleation and localization are two distinct processes. Nucleation occurs homogeneously via fluctuations at early times, whereas spatially periodic structures emerge only later and, under suitable conditions, localize in less than one nanosecond. Real-space simulations show that this localization is governed by strong lateral variations in spin-texture lifetimes. Our results demonstrate that ultrafast phase-transition dynamics fundamentally differ from conventional transitions, yet still can be controlled through moderate nanometer-scale tailoring of the energy landscape. |  |