France



Magnetic nanowires (MNWs) have been proposed for nanobarcoding and biolabeling for decades, but surprisingly, they have never been successfully realized for these applications due to the lack of reliable decoding strategies. Here, several types of MNWs were electrodeposited into track-etched polycarbonate templates for application as nanobarcodes. The coercivity (H&lt;sub&gt;c&lt;/sub&gt;) and interaction fields (H&lt;sub&gt;u&lt;/sub&gt;) of the MNWs were engineered using the composition, dimensions, and spatial distributions to tune the remanence spectra&lt;sup&gt;1&lt;/sup&gt; of each barcode. This remanence spectrum is the irreversible switching field distribution measured at zero applied field after applying a pre-defined field sequence. It is therefore a complex function of both coercivity and interaction field. An automated algorithm was also introduced to reliably decode unknown remanence spectra measured in unknown combinations of the magnetic nanobarcodes&lt;sup&gt;2,3&lt;/sup&gt;.&lt;br/&gt;Up-to-date, H&lt;sub&gt;c&lt;/sub&gt; and H&lt;sub&gt;u&lt;/sub&gt; distributions themselves have been the most popular magnetic signatures using in decoding, usually measured using the first-order reversal curve (FORC) method&lt;sup&gt;1,4&lt;/sup&gt;. Despite numerous works on tuning H&lt;sub&gt;c&lt;/sub&gt; and H&lt;sub&gt;u&lt;/sub&gt;, these parameters can only be independently decoded for a limited number of unique signatures. For instance, H&lt;sub&gt;u&lt;/sub&gt; for arrays of non-interacting MNWs is always zero, which limits signatures to simply H&lt;sub&gt;c&lt;/sub&gt; and its distribution. Typical decoding is even harder when both non-interacting and highly interacting magnetic nanobarcodes are at the readout simultaneously&lt;sup&gt;3&lt;/sup&gt;. Although the H&lt;sub&gt;c&lt;/sub&gt; distribution may be inherently distinct for each MNW; fully decoupling the interaction field effects from the coercivity distribution is a very tedious procedure&lt;sup&gt;5&lt;/sup&gt;. Our recently proposed approach of decoding via the remanence spectra&lt;sup&gt;6&lt;/sup&gt; has overcome these limitations while also using orders of magnitude fewer measurement points compared to FORC leading to a significantly faster decoding procedure.&lt;br/&gt;Figure 1 shows the remanence spectra of a combined measurement with two barcodes: 30nm-diameter Ni MNWs and 100nm-diameter Ni MNWs. The automated algorithm makes a best fit assuming the number of barcodes presence are 1, then 2, then 3. The root-mean-square (RMS) error between the fit and the measurement is calculated at each step. At “n” steps (here 3), the RMS error is not significantly improved, so the number of barcodes is determined to be “n-1” (here 2). This presentation will demonstrate how to expand the number of magnetic nanobarcodes remanence spectra using coercivity and interaction field as independent encoding parameters tuned through various strategies. We will also describe our automated algorithm to reliably and rapidly decode unknown remanence spectra, which is also capable to decode other nanobarcodes including magneto-optic nanobarcodes.&lt;br/&gt;In summary, remanence spectra are promising for decoding nanobarcodes for three reasons. First, the coercivity and interaction field can be tailored individually to expand the number of remanence spectra encoded magnetic nanobarcodes. Second, the decoding can reliably be done even when one of these parameters is zero or negligible and also when the number of nanobarcodes presence is unknown. Third, remanence spectra are much faster to measure and less tedious to decouple than standard signatures.

**References:**

1 Y. G. Velázquez, A. L. Guerrero, J. M. Martínez, E. Araujo, M. R. Tabasum, B. Nysten, L. Piraux and A. Encinas, &lt;i&gt;Sci. Rep.&lt;/i&gt;, 2020, 10, 21396.&lt;br/&gt;2 M. R. Zamani Kouhpanji and B. Stadler, &lt;i&gt;Part. Part. Syst. Charact.&lt;/i&gt;, 2020, 2000227.&lt;br/&gt;3 M. R. Zamani Kouhpanji and B. J. H. Stadler, &lt;i&gt;Nanoscale Adv.&lt;/i&gt;, 2021, DOI:10.1039/D0NA00924E.&lt;br/&gt;4 D. A. Gilbert, G. T. Zimanyi, R. K. Dumas, M. Winklhofer, A. Gomez, N. Eibagi, J. L. Vicent and K. Liu, &lt;i&gt;Sci. Rep.&lt;/i&gt;, 2014, 4, 1–5.&lt;br/&gt;5 C.-I. Dobrotă and A. Stancu, &lt;i&gt;J. Appl. Phys.&lt;/i&gt;, 2013, 113, 043928.&lt;br/&gt;6 M. R. Zamani Kouhpanji, A. Ghoreyshi, P. B. Visscher and B. J. H. Stadler, &lt;i&gt;Sci. Rep.&lt;/i&gt;, 2020, 10, 15482.

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/fae2d498dd387a1e4ac20feae07613b1.jpg)
Figure 1: shows encoding and decoding remanence spectra of magnetic nanowires (MNWs) for nanobarcoding, (a) depicts the normalized backward remanence (BRM) spectra of the individual MNWs “encoded” using their dimensions, and (b-d) illustrate the decoding of an unknown BRM spectrum composed of Ni MNWs with diameters of 30nm and 100nm. The reduction percentage of the root-mean-square (RMS) error is the convergence criteria for identifying the number and type of magnetic nanobarcodes in the unknown BRM spectra.



INTERMAG 2021

 A roadmap toward expanding magnetic nanobarcodes signatures

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Magnetic nanowires (MNWs) have been proposed for nanobarcoding and biolabeling for decades, but surprisingly, they have never been successfully realized for these applications due to the lack of reliable decoding strategies. Here, several types of MNWs were electrodeposited into track-etched polycarbonate templates for application as nanobarcodes. The coercivity (Hc) and interaction fields (Hu) of the MNWs were engineered using the composition, dimensions, and spatial distributions to tune the remanence spectra1 of each barcode. This remanence spectrum is the irreversible switching field distribution measured at zero applied field after applying a pre-defined field sequence. It is therefore a complex function of both coercivity and interaction field. An automated algorithm was also introduced to reliably decode unknown remanence spectra measured in unknown combinations of the magnetic nanobarcodes2,3. Up-to-date, Hc and Hu distributions themselves have been the most popular magnetic signatures using in decoding, usually measured using the first-order reversal curve (FORC) method1,4. Despite numerous works on tuning Hc and Hu, these parameters can only be independently decoded for a limited number of unique signatures. For instance, Hu for arrays of non-interacting MNWs is always zero, which limits signatures to simply Hc and its distribution. Typical decoding is even harder when both non-interacting and highly interacting magnetic nanobarcodes are at the readout simultaneously3. Although the Hc distribution may be inherently distinct for each MNW; fully decoupling the interaction field effects from the coercivity distribution is a very tedious procedure5. Our recently proposed approach of decoding via the remanence spectra6 has overcome these limitations while also using orders of magnitude fewer measurement points compared to FORC leading to a significantly faster decoding procedure. Figure 1 shows the remanence spectra of a combined measurement with two barcodes: 30nm-diameter Ni MNWs and 100nm-diameter Ni MNWs. The automated algorithm makes a best fit assuming the number of barcodes presence are 1, then 2, then 3. The root-mean-square (RMS) error between the fit and the measurement is calculated at each step. At “n” steps (here 3), the RMS error is not significantly improved, so the number of barcodes is determined to be “n-1” (here 2). This presentation will demonstrate how to expand the number of magnetic nanobarcodes remanence spectra using coercivity and interaction field as independent encoding parameters tuned through various strategies. We will also describe our automated algorithm to reliably and rapidly decode unknown remanence spectra, which is also capable to decode other nanobarcodes including magneto-optic nanobarcodes. In summary, remanence spectra are promising for decoding nanobarcodes for three reasons. First, the coercivity and interaction field can be tailored individually to expand the number of remanence spectra encoded magnetic nanobarcodes. Second, the decoding can reliably be done even when one of these parameters is zero or negligible and also when the number of nanobarcodes presence is unknown. Third, remanence spectra are much faster to measure and less tedious to decouple than standard signatures.

**References:**

1 Y. G. Velázquez, A. L. Guerrero, J. M. Martínez, E. Araujo, M. R. Tabasum, B. Nysten, L. Piraux and A. Encinas, Sci. Rep., 2020, 10, 21396. 2 M. R. Zamani Kouhpanji and B. Stadler, Part. Part. Syst. Charact., 2020, 2000227. 3 M. R. Zamani Kouhpanji and B. J. H. Stadler, Nanoscale Adv., 2021, DOI:10.1039/D0NA00924E. 4 D. A. Gilbert, G. T. Zimanyi, R. K. Dumas, M. Winklhofer, A. Gomez, N. Eibagi, J. L. Vicent and K. Liu, Sci. Rep., 2014, 4, 1–5. 5 C.-I. Dobrotă and A. Stancu, J. Appl. Phys., 2013, 113, 043928. 6 M. R. Zamani Kouhpanji, A. Ghoreyshi, P. B. Visscher and B. J. H. Stadler, Sci. Rep., 2020, 10, 15482.

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/fae2d498dd387a1e4ac20feae07613b1.jpg)
Figure 1: shows encoding and decoding remanence spectra of magnetic nanowires (MNWs) for nanobarcoding, (a) depicts the normalized backward remanence (BRM) spectra of the individual MNWs “encoded” using their dimensions, and (b-d) illustrate the decoding of an unknown BRM spectrum composed of Ni MNWs with diameters of 30nm and 100nm. The reduction percentage of the root-mean-square (RMS) error is the convergence criteria for identifying the number and type of magnetic nanobarcodes in the unknown BRM spectra.

technical paper

Cylindrical magnetic nanowires (NWs) are promising candidates for building blocks of 3D nanoarchitectures and 3D nanotechnologies [1,2]. They present great potential for 3D applications, offering responses to many external (electrical, magnetic, mechanical, thermal, etc.) stimuli [3]. The emerging interest toward cylindrical magnetic NWs is related to the fact that their geometry promotes topologically non-trivial 3D magnetic structures such as Bloch-point domain walls, complex configurations that connect vortex domains with opposite chirality, vortices or skyrmion tubes [4,5]. Here, we present a study on multisegmented NWs formed by ferromagnetic (FM) segments separated either by a different FM material or a non-magnetic (NM) one. On one hand we have alternating CoNi/Ni segments (Fig. 1 (a)), where the domain structure can be tailored by alternating magnetocrystalline anisotropy and the length of each segment. On other hand, FeCo ferromagnetic layers separated by thin Cu NM layers (Fig. 1 (c)). The multisegmented NWs were prepared by electroplating filling the pores of anodic aluminum oxide membranes. The HRTEM analysis confirms the multisegmented morphology with a uniform diameter, and periodic and sharp interfaces. Quantitative analysis reveals that the diameter of CoNi/Ni NWs is about 140 nm with lengths between 0.6 μm and 1.4 μm for CoNi and 1 μm for Ni segments while FeCo/Cu wires with 165 nm in diameter are formed by FeCo segments with 250 nm in length separated by 50 nm Cu layers. XMCD-PEEM imaging of multisegmented CoNi/Ni NWs reveals that the magnetic structure in Ni segment is in a dominantly axial magnetic state while in CoNi segments it depends on their length. In NWs with the shortest CoNi segments (0.6 μm), we observed single vortex domains, in longer segments of 1.2 μm we observed one to three vortex domain states (Fig. 1 (a)), while in the NWs with the longest CoNi segments either multi-vortex or multi-transverse domains were observed. The micromagnetic simulations show that the remanent magnetic structure of CoNi segments depends on the direction of the previously applied field. If the direction is perpendicular to both the NW and the magnetization easy axis, the vortex domains simply expand inside the segment following the structures formed at the interfaces and resulting in one vortex domain for short segments and two or more vortex structures for longer segments. In turn, when the field is applied perpendicular to the NW but along the magnetization easy axis, transverse domains are formed. They are separated by vortex domain structures with core at the surface pointing perpendicular to it. Furthermore, although Ni segments are in an almost single-domain state, they are not completely saturated, and present a small magnetization curling on the NW surface. Their chirality is formed prior to formation of magnetic structures in CoNi and imprints the chirality along the next CoNi segments (Fig. 1 (b)) [5]. The second investigated multisegmented system, FeCo/Cu (Fig. 1 (c-d)), presents a tilt at the interface between FM/NM layer. From the XMCD-PEEM images (Fig. 1 (c)) we determined that each FeCo segment presents a single vortex state which switches its magnetization under the influence of perpendicular magnetic fields. This switching is sequential and each segment has a slightly different switching field. The simulations (Fig. 1 (d)) unveil the main differences between magnetization states when the field is applied along different directions with respect to the NW axis. The tilt between adjacent segments breaks the rotational symmetry providing different magnetic potentials for vortices moving in a certain direction under the influence of applied magnetic field. The proper design of segments anisotropy and geometry (e.g., surface tilting) in cylindrical multisegmented nanowires opens multiple opportunities for advanced nanotechnologies in 3D magnetic nanostructures.

**References:**

[1] Fernández-Pacheco, A.; Streubel, R.; Fruchart, O.; Hertel, R.; Fischer, P.; Cowburn, R. P. , Nat. Commun. 2017, 8, 15756. [2] Hertel, R, Spin 2013, 03 (03), 1340009. [3] “Magnetic Nano- and Microwires: Design, Synthesis, Properties and Applications”, Elsevier 2020, edited by M.Vazquez. [3] Da Col, S.; Jamet, S.; Rougemaille, N.; Locatelli, A.; Mentes, T. O.; Burgos, B. S.; Afid, R.; Darques, M.; Cagnon, L.; Toussaint, J. C.; et al. , Phys. Rev. B 2014, 89 (18), 180405. [4] Fernandez-Roldan, J. A.; Perez del Real, R.; Bran, C.; Vazquez, M.; Chubykalo-Fesenko, O., Nanoscale 2018, 10 (13), 5923–5927. [5] Bran, C.; Fernandez-Roldan, J.A.; P Del Real, R.; Asenjo, A.; Chen, Y.-S.; Zhang, J.; Zhang, X.; Fraile Rodríguez, A.; Foerster, M.; Aballe, L.; et al. , ACS Nano 2020, 14, 12819.

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/9345e275af7517d8247f940544434392.jpg)
Figure 1. Schematic illustrations of multisegmented NWs (top panels) (a) Chemical contrast and XMCD-PEEM images of a CoNi (1.2 μm)/Ni(1 μm) multisegmented NWs (b) Modelled magnetization state of the CoNi/Ni NW presented in (a), (c) XMCD-PEEM images of FeCo/Cu NWs measured in remanence after perpendicular magnetic fields were applied, (d) Simulated magnetization configurations of FeCo/Cu NW before (upper panel) and after (bottom panel) magnetic fields were applied in y-direction. Scale bar 1μm.

 Controlled magnetization by magnetic fields in multisegmented cylindrical nanowires

Cylindrical magnetic nanostructures are attracting much interest in a wide range of applications (biomedical imaging, drug delivery, 3D memory storage devices, sensors, etc.). The ability to tune their magnetic properties by changing the geometry (disks, dots, wires, tubes), combined with low-cost and high-yield template fabrication methods, makes these nanostructures highly attractive for implementation in emerging technologies. However, most applications require a full understanding of the magnetization reversal mechanisms. Although it is a well-known topic, thoroughly studied for the past two decades, recent advances in characterization and micromagnetic simulation techniques renewed the attention of the scientific community towards the complete understanding of such magnetic 3D nano-elements [Bran2016, Fernández-Pacheco2017, Charilaou2018, Ruiz-Gómez2020]. In particular, Ni nanowires have been the most reported nanostructures fabricated in nanoporous alumina templates so far [Sousa2014, Proenca2012]. But, nanodisks and low-aspect ratio nanowires are still less explored, particularly regarding the full understanding of the magnetization reversal mechanisms. In this work, we have analyzed the magnetization response of cylindrical Ni nanostructures with 15 to 100 nm in diameter and 12 to 230 nm in length and compared our results with experimental data for periodic arrays. Our simulations show the presence of a critical diameter (d ≈ 30 nm) that determines the type of domain wall nucleated (transverse or vortex/skyrmion tube); and a critical length (L ≈ 100 nm) that limits the number of domain walls formed (one or two). By adjusting the diameter/length of the Ni nanocylinders, different magnetic remanent states and reversal mechanisms were observed (Figure 1). Moreover, vortex DWs were found to originate from 3D skyrmion tubes, which have been reported as one of the best configurations for magnetic storage devices. By increasing the diameter and aspect ratio (L/d) of nanowires with L &gt; 100 nm, three distinct reversal modes were observed: i) simultaneous propagation of two vortex DWs with opposite chirality; ii) propagation of only one vortex DW, or iii) spiral rotation of both DWs through the “corkscrew” mechanism (Figure 2). Only for very low aspect ratio structures (nanodisks), no skyrmion tubes were observed and reversal occurred by spiral rotation of one vortex DW. The broad range of dimensions studied in this work allowed the creation of the first complete magnetic phase diagram in cylindrical nanostructures [Proenca2021]. This universal phase diagram will be highly important for the future choice of nanoscaled dimensions in the development of novel nano-devices. This work has been supported by the European Union's Horizon 2020 research and innovation program under the Marie Sklodowska-Curie Grant Agreement No. 734801; by the Portuguese Fundação para a Ciência e Tecnologia (FCT) through the Investigador FCT program (Contract No. IF/01159/2015); by FCT and COMPETE 2020 (FEDER) under the projects POCI-01-0145-FEDER-028676, POCI-01-0145-FEDER-031302, POCI-01-0145-FEDER-032527, POCI-01-0145-FEDER-032257 and UIDB/04968/2020; and by the Spanish Ministerio de Ciencia e Innovación under the project MAT2017-87072-C4-3-P.

**References:**

C. Bran, E. Berganza, E. M. Palmero, et al., J. Mater. Chem. C, Vol. 4, p.978 (2016) A. Fernández-Pacheco, R. Streubel, O. Fruchart, et al., Nat. Commun., Vol. 8, p15756 (2017) M. Charilaou, H. B. Braun and J. F. Löffler, Phys. Rev. Lett., Vol. 121, p.97202 (2018) S. Ruiz-Gómez, C. Fernández-González, E. Martínez, et al., Nanoscale, Vol. 12, p.17880 (2020) C. T. Sousa, D. C. Leitao, M. P. Proenca, et al., Appl. Phys. Rev., Vol. 1, p.031102 (2014) M. P. Proenca, C. T. Sousa, J. Ventura, et al., Electrochim. Acta, Vol. 72, p.215 (2012) M. P. Proenca, J. Rial, J. P. Araujo and C. T. Sousa, Magnetic reversal modes in cylindrical nanostructures: from disks to wires, submitted (2021)

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/224d41da086e562fd530d5cd1dca0bff.jpg)
Figure 1: Phase diagram of the magnetization reversal modes in individual Ni nanocylinders with different lengths and diameters, when applying the magnetic field along the nanocylinder’s length (parallel direction). Insets show selected cross-sectional representations of the magnetic configuration during reversal.

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/458fea4fee1b4edbee176c880e9b95e1.png)
Figure 2: 3D representation of the magnetic configuration during reversal of the simulated Ni nanowire with 100 nm in diameter and 130 nm in length illustrating the spiral rotation of two vortex domain walls (skyrmion tubes) through the “corkscrew” mechanism when applying the magnetic field along the z-direction (parallel to the nanowires’ long axis).

 Phase Diagram of Magnetization Reversal Modes in Cylindrical Ni Nanowires

Three-dimensional (3D) nanomagnets provide a great potential to be implemented in future spintronic devices for high-density magnetic memories, nano-sensing or logic. Among these appealing architectures, ferromagnetic nanotubes (NTs) are currently being investigated for their fast and low-power domain wall conduit properties [1]. The development of novel 3D nanostructures typically requires complex synthetic methods. Moving forward in this challenging task, Focused Electron Beam Induced Deposition (FEBID) has been explored for the growth of 3D ferromagnetic NTs. This unique one-step nanolithography technique, based on the decomposition of organometallic precursor gas molecules in the vicinity of a substrate [2,3], has demonstrated great versatility in terms of shape, composition and magnetic properties [4]. Following the strategy developed for the fabrication of core-shell nanowires [5], the growth of 3D Co NTs by FEBID has been performed for the first time [6]. The heterostructured design is composed by a vertical Pt-C nanowire (≤100 nm in diameter) acting as a core, and a Co coating forming the shell with a thickness down to ~11 nm. These are exotic magnetic nanostructures in which unconventional domain walls are formed, presenting high domain wall velocities without Walker breakdown phenomenon and where great stability during propagation has been predicted. Furthermore, Transmission Electron Microscopy (TEM) experiments reveal that these NTs present a nanocrystalline structure and a metallic content of ~70 at. %. In addition, a coercivity of ~16 mT has been obtained by Magneto-Optical Kerr Effect magnetometry, and magnetic characterization performed by Electron Holography evidences the ferromagnetic behaviour, estimating a remanent magnetic induction up to 1.3 T and detecting complex head-to-head magnetic domain walls. The application of magnetic fields inside the TEM has allowed the pinning and imaging of domain walls in these nanostructures. Finally, micromagnetic simulations have been performed for a deeper understanding of the magnetization dynamics [6].

**References:**

[1] R. Hertel, J. Phys.: Condens. Matter, 28, 483002 (2016). [2] J. Pablo-Navarro, S. Sangiao, C. Magén, et. al., Nanofabrication: Nanolithography techniques and their applications. Edited by J. M. De Teresa, IOP Publishing (2020). [3] A. Fernández-Pacheco, L. Skoric, J. M. De Teresa, et. al., Materials, 13, 3774 (2020). [4] J. Pablo-Navarro, D. Sanz-Hernández, C. Magén, et al., J. Phys. D. Appl. Phys., 50, 18LT01 (2017). [5] J. Pablo-Navarro, C. Magén and J. M. De Teresa, Nanotechnology, 27, 285302 (2016). [6] J. Pablo-Navarro, et al., manuscript in preparation.

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/fee42b13b0eb696628dd941a85be6a72.jpg)
Fig. 1. (a) HAADF-STEM image of a Co-FEBID NT cross-section. (b,c) Experimental and simulated magnetic phase shift around a domain wall obtained by Electron Holography and micromagnetic simulations, respectively. (d) Spin configuration obtained from micromagnetic simulations.

 Ferromagnetism of Single Vertical Cobalt Nanotubes Grown by Focused Electron Beam Induced Deposition

Bringing nanomagnetism into the third dimension is of growing interest due to many advantages that three-dimensional (3D) structures provide. The introduction of 3D geometrical effects such as curvature and chirality1, as well as the high density and enhanced device connectivity, lead to many opportunities for new physics and applications2,3. When we combine this promising field of 3D nanomagnetism with the well-established field of spintronics, a number of proposals ranging from the ultra-high-density 3D racetrack memory4 to 3D interconnected memristors for neuromorphic computing5 appear. However, before we can fully exploit the promise of 3D spintronics, significant advances in both the integration of 3D nanomagnets into 2D microelectronic circuits，and the understanding of the influence of a 3D geometry on the magnetotransport properties, are required. The implementation of 3D nanomagnetic circuits faces great challenges regarding the fabrication of a 3D nanostructure and its interconnectivity to the electronic components. Until recently, most magnetotransport experiments have concerned cylindrical nanowires, with complex micromanipulations needed to electrically contact them6. In this work, we employ 3D nano-printing capabilities provided by Focused Electron Beam Induced Deposition (FEBID)7, to directly fabricate a high-quality 3D Cobalt nanobridge with well-defined leads on pre-synthesized electrical contacts (Figure 1a). The SEM image shown in Figure 1b demonstrates the successful integration of this complex, high-aspect-ratio 3D nanostructure onto lithographically patterned electrodes. This printed 3D nanomagnetic circuit allows four-probe transport measurements with which we can probe the magnetotransport properties of the 3D nanostructure - and determine the influence of the three-dimensionality on these properties. To fully characterise the magnetotransport (MT) properties of the 3D magnetic nanobridge, we measured MT hysteresis loops for fields applied in different directions in three-dimensions (Figure 2a, b). These magnetotransport measurements, in combination with macrospin and finite element simulations, reveal that the three-dimensional structure of the nanobridge directly affects the magnetotransport in several ways. Firstly, the non-collinear current path in the 3D geometry results in a complex superposition of different MT effects, leading to an unusual angular dependence of well-known effects such as the Anomalous Hall effect. Secondly, we also identify a significant angular-dependence of the magnetoelectric signal due to the magnon magnetoresistance. This strong angular dependence occurs due to the strong influence of the demagnetising field within the non-collinear regions of the 3D geometry, highlighting the importance of magnetostatics in 3D nanostructures8. These new insights into the influence of a 3D geometry on the magnetotransport effects reported in this work provide the basis for the future study of new spintronic effects in 3D magnetic nanostructures, as well as the realization of 3D spintronic technologies. This methodology shown here combining FEBID 3D printing and standard planar lithography can be extended to more complicated geometries and other materials, opening the door to the fundamental study of new phenomena that exploit the interplay between 3D geometry and magnetotransport and may find applications in the future of areas such as magnonics, frustrated magnetic systems, and magnetic neural networks.

**References:**

 (1) R. Streubel, P. Fischer and F. Kronast, J Phys D Appl Phys., Vol. 49, p.363001(2016) (2) A. Fernández-Pacheco, R. Streubel and O. Fruchart, Nat Commun., Vol. 8, p.15756 (2017) (3) P. Fischer, D. Sanz-Hernández and R. Streubel, Apl Mater., Vol. 8, p.15756 (2017) (4) S. Parkin, M. Hayashi and L. Thomas, Science., Vol. 320, p.190-194 (2008) (5) A. May, M. Hunt and A. Berg, Commun Phys., Vol. 2, p.13 (2019) (6) M. Schöbitz, A. Riz and S. Martin, Phys Rev Lett ., Vol. 123, p.217201 (2019) (7) L. Skoric, D. Sanz-Hernández and F. Meng, Nano Lett ., Vol. 20, p.184-191 (2019) (8) F. Meng, C. Donnelly and C. Abert, Arxiv., arXiv:2011.09199 (2020)

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/f82793d4777c5e628b8b37e46d66e2d7.jpg)
Fig.1 (a) 3D nano-printing of the bridge via Focused Electron Beam Induced Deposition (FEBID) on pre-patterned electrical contacts. (b) The SEM image of the as-fabricated nanomagnetic circuit. (c) Four-probe magnetotransport measurement configuration. (d) The SEM image of the top view of the nanobridge.

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/ba14c1bac15d9b830f10e775d14b93fe.jpg)
Fig.2 (a) The schematic shows how the field was applied relative to the 3D nanobridge, θ is the angle between the applied field and the substrate (b) Magnetotransport hysteresis loop obtained from -4 T to 4 T and 4 T to -4 T for each field angle θ, from θ = 0° to θ = 90° (from violet to red).

 Non-planar geometrical effects on the magnetoelectrical signal in a 3D nanomagnetic circuit

Magnetocuring of carbon and glass fibers was performed using Curie temperature tuned magnetic nanoparticles (CNP) embedded in adhesives, aka magnetoadhesive. Interestingly, these fibers were cured under alternating magnetic field (AMF) within a few minutes. In-situ heating of the magnetoadhesive were controlled by CNP loading and AMF strength. The heating of the CNP switches off above its Curie temperature, which prevents overheating. For the first time, custom made AC-magnetorheometry was employed to understand the kinetics of curing of the magnetoadhesive under AMF. The storage modulus of the magnetocured adhesive exceeded 10 MPa at shear strain of &lt; 10%. Introduction: Magnetic field activated adhesive curing, aka magnetocuring have recently been reported[1]. Magnetocuring overcomes the limitations of available curing techniques e.g. photocuring[2], snap-curing[3], and electrocuring[4], etc, it allows the adhesive to be activated on-demand when an alternating magnetic field is applied. Carbon fiber is increasingly being used to make lighter and stronger parts in many industries including aviation, automobile, marine, sports, defence, IT, etc.[5] However, in most of the applications, these fibers need to bond with suitable thermosets/thermoplastics in order to achieve high stiffness, for which thermal curing is required. Magnetocuring of carbon and glass fibers can be applied in a range of commercial applications. The present work addresses the design and application of one-pot epoxy adhesives by the ‘modifier’ methodology for on-demand contactless curing under alternating magnetic field (AMF). Material and Methods: Curie nanoparticles (CNP) were synthesized by the hydrothermal method and functionalized using oleic acid and epoxy [1]. Functionalized CNP were mixed into commercial 1C epoxy adhesive and cured under an alternating magnetic field (AMF, 400 kHz, 140 Oe). The kinetic parameters, real-time properties of the adhesive and composite were evaluated using a custom made AC magneto-rheometry setup. Results and Conclusions: Magnetoadhesive applied carbon and glass fibers were passed through the magnetic field generated solenoid coil and cured within 5 min (Fig. 1A). This fast curing is important for in-line manufacturing of fiber based components. The magnetoadhesive property under AMF and at room temperature were studied using AC-magnetorheometry. The gelation point of the magnetoadhesive with 30wt.% CNP was achieved within 70 s of AMF exposure (Fig. 1B and 1C). On applying the magnetic field, a decrease in the loss modulus (G’) and increase in the storage modulus (G’’) was observed due to the initiation of crosslinking and composite hardening. The storage modulus of the magnetocured adhesive was observed to be &gt;10 MPa at shear strain of &lt; 10% (Fig. 1C). These results suggest that magnetocuring is an attractive technology for in the sports goods, automotive, aerospace and medical industries. It offers an energy efficient, remote, and wireless method of on-demand adhesion by exploiting self-regulating Curie nanoparticles (CNP). Real time magnetorheology measurements were used to determine the properties, fast gelation within 70 s was observed.. Acknowledgement: Authors acknowledge the financial support from the Agency for Science, Technology and Research (A*Star) for the grant IRG17283008 “Microprocessor- based methods of composite curing.

**References:**

[1] R. Chaudhary, V. Chaudhary, R.V. Ramanujan, T.W.J. Steele, Applied Materials Today 21, 100824 (2020). [2] S.C. Ligon-Auer, M. Schwentenwein, C. Gorsche, J. Stampfl, R. Liska, Polymer Chemistry 7, 257-286 (2016). [3] X.K. Hillewaere, R.F. Teixeira, L.T.T. Nguyen, J.A. Ramos, H. Rahier, F.E. Du Prez, Advanced Functional Materials 24, 5575-5583 (2014). [4] J. Ping, F. Gao, J.L. Chen, R.D. Webster, T.W. Steele, Nature communications 6, 1-9 (2015). [5] C. Soutis, Materials Science and Engineering: A 412, 171-176 (2005).

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/d53ed9987bc3b153986b15a11f93643b.jpg)
Fig.1 Magnetocuring and AC-magnetorheology of composites. (A) Magnetocuring of carbon and glass fibers for in-linemanufacturing, (B-C) Oscillation and amplitude sweep of 30wt.% CNP within epoxy adhesive.

 Magnetocuring and Magnetorheology of Composites

Investigation of magnetic properties of nanostructured ferromagnets, such as oriented arrays of carbon nanotubes (CNTs) containing ferromagnetic nanoparticles (FNPs), is still relevant. In addition to attractive applications in magnetoelectronics, CNTs with embedded FNPs are also a very useful model object for studying magnetic interaction of the latter through a conducting medium. For this, it is important to establish a relation between macroscopic and microscopic parameters of the system. In nanostructured ferromagnets, this dependence is described within the random magnetic anisotropy model (RAM), in which the spin system and, consequently, the main macroscopic characteristics (coercivity, susceptibility, saturation magnetization) are determined by such microscopic parameters as the exchange interaction constant, FNP magnetization, local magnetic anisotropy constant and grain size 2Rc [1]. Recently, magnetic parameters like the exchange and anisotropy fields, effective magnetic anisotropy constant, Bloch and exchange constants in aligned CNT arrays containing FNPs were determined within the RAM by analyzing law of the approach to saturation magnetization and corresponding modeling of the correlation functions of the magnetic anisotropy axes of the FNPs [2,3]. Presence of the interplay between the exchange interaction and magnetic anisotropy, as well as the contribution of not only random, but also coherent anisotropy, was established [3]. In addition, the important role of magnetoelastic anisotropy in the case when a single FNP is localized inside a CNT has been revealed. [4]. It was shown also that aligned CNT arrays with a low concentration of FNPs embedded only inside CNT have relatively high values of exchange fields, random and coherent anisotropy. They are manifested in CNT arrays, in which the average distance between the FNPs significantly exceeds the size of the latter, reaching hundreds of nanometers. These effects, which do not currently have a convincing explanation, are mainly associated with the presence of the exchange interaction between FNPs through the CNT matrix. However, there is still no reasonable mechanism of the long-range exchange interaction in CNT arrays. In our work [5], it was assumed that these effects are related to the indirect exchange coupling of the RKKY type via the conducting electrons of CNTs. The obtained preliminary estimations have shown that the RKKY exchange interaction is enhanced by the presence of spin-orbit coupling (SOC) and could propagate up to a micrometer scale [5]. In this contribution a multiwall CNT (MWCNT) with embedded FNPs is considered. We present the results of modeling of the RKKY interaction in MWCNT depending on its diameter, chirality, chemical potential and SOC constant within the Klinovaya-Loss model [6]. The influence of the external longitudinal magnetic field is also studied. It is assumed that the main contribution to the RKKY interaction is caused by the conduction electrons of the inner wall of CNTs which is in contact with the FNP. In addition, spin-orbit interaction (SOI) in CNT is also considered. The SOI in a nanotube can occur due to the curvature effect, which significantly increases its contribution in comparison with a flat graphene. It can also be enhanced by FNP, CNT defects or impurity states. The spin susceptibility of CNT conduction electrons χ/χ0 is evaluated (χ0=a2kG/hυF, where υF is the Fermi velocity, kG is the circumferential direction, a is the lattice constant). Fast oscillations are excluded and only slowly changing envelopes of spin susceptibility are considered. The chemical potential is tuned inside the gap opened by SOI. It is shown that the decay of the amplitude of the χ/χ0 oscillations depends strongly on the chemical potential: the higher the Fermi energy of the CNT (εF), the more significant is the decay. The frequency of spin susceptibility oscillations increases with the increase of the εF (Fig. 1). This is due to the fact that with the increase of the Fermi energy of CNTs, the discrepancy between the gap opened by SOI and the value of chemical potential increases. Finally, the proposed approach allows evaluating the energy of the exchange interaction between FNPs belonging to the same CNT. The work is supported by the COST Action CA19118.

**References:**

[1] E.M. Chudnovsky, J. Appl. Phys., Vol. 64, p. 5770 (1988). [2] A.L. Danilyuk, A.L. Prudnikava, I.V. Komissarov, et al. Carbon, Vol. 68, p. 337 (2014). [3] A.L. Danilyuk, I.V. Komissarov, V.A. Labunov, et al. New J. Phys. Vol. 17, p. 023073 (2015). [4] S.L. Prischepa, A.L. Danilyuk, A.V. Kukharev, et al. IEEE Trans. Magn. Vol. 55, p. 2300304 (2019). [5] A.L. Danilyuk, I.V. Komissarov, A.V. Kukharev, et al. Europhys. Lett. Vol. 117, p. 27007 (2017). [6] J. Klinovaja and D. Loss D, Phys. Rev. B, Vol. 87, p. 045422 (2013).

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/29f3738a3c00cb89dafac5b18dcdb897.jpg)
Fig. 1. Decay of the oscillation amplitude of the spin susceptibility χ/χ0 along the axis of the semiconductor CNT of diameter of 25 nm with chiral indices (235,129) and εF=18 (blue) and 30 (red) meV. The chirality angle is 39.54° and kG =0.053 nm-1.

 Long-Range Exchange Interaction between Ferromagnetic Nanoparticles Embedded in Carbon Nanotubes

Superparamagnetic nanoparticles are drawing increasing interests because of their special physical properties and potential applications in magnetic-supporting catalysts, water purification, ferrofluids, and medical diagnostics [1,2]. For most applications, an accurate determination of the particle size distribution is required since the magnetic properties of the particles directly depend on the particle size. Transmission electron microscopy (TEM) and X-ray diffraction (XRD) are widely used to determine the particle size. However, both methods have limitations. For TEM, normally only a limited amount of particles contribute to the result, and the precise determination of extremely small particles is difficult due to the limit of the TEM image contrast and resolution. For XRD, the evaluation is based on the Scherrer equation, the result of which is the average size of the particles, more detailed information of the size distribution is not available. Furthermore, this method assumes that the peak broadening is solely due to the crystallite size, other effects such as microstrain are neglected. Besides, neither TEM nor XRD are suitable for embedded nanoparticles. Above the blocking temperature TB, the magnetic moment versus external magnetic field curve (m-H curve) of superparamagnetic particles is described by m=mSL(x), with x=μ0mp(d)H/kBT, where m is the magnetic moment, mS is the saturation magnetic moment, μ0 is the vacuum permeability, mp is the magnetic moment of one particle of size d, H is the external field, kB is the Boltzmann constant, T is the temperature in Kelvin, L(x) is the Langevin function: L(x)=coth(x)-1/x. Since the m-H curve is dependent on the size d, the particle size could be determined by fitting the measured m-H curve with the Langevin function. Note that the realistic particle size normally includes a distribution. In 1978, Chantrell et al. [3] presented a method to determine the mean value and standard deviation of the particle size distribution. This method fits the measured m-H curve to a weighted sum of Langevin functions using a pre-assumed lognormal size distribution. Since then, this method has been used in many works for decades [4-6]. However, the assumption that the size distribution is always lognormal might not be accurate for particles synthesized by all the techniques. In this work, we present a fitting method without a pre-assumed distribution. The measured m-H curve is fitted to a superposition of Langevin functions with corresponding fractions, and the combination of these fractions is the size distribution. In the fitting procedure, three constraints are considered: 1) The method of least squares is used to obtain a well fitted m-H curve; 2) The smoothness of the distribution is a criterion to judge whether the fit is valid, since a realistic distribution should be relatively smooth; 3) Saturation magnetic moment should be fitted since the small particles cannot be saturation magnetized. To obtain a fitted distribution under all these three constraints with optimized weights, we apply the method of Lagrange multipliers. This fitting method is used to determine the size distribution of five different superparamagnetic γ-Fe2O3/SiO2 core-shell nanoparticle samples. The m-H curves were measured by VSM and then fitted with a supperposition of Langevin functions. The fitting results of selected samples are shown in Fig. 1 and Fig. 2. The fitted mean values and standard deviations of the particle size distributions agree well with the results of TEM and XRD [1].

**References:**

[1] C. Zambrzycki, R. Shao, A. Misra, C. Streb, U. Herr, R. Güttel, Catalysts. 2021; 11(1):72. [2] V. Wu, E. Huynh, S. Tang, V Uskoković, Acta biomaterialia 88 (2019): 422-447. [3] R. Chantrell, J. Popplewell, S. Charles, IEEE Transactions on Magnetics 14.5 (1978): 975-977. [4] E. Ferrari, F. Da Silva, M. Knobel, Physical Review B 56.10 (1997): 6086. [5] F. C. Fonseca, et al., Physical review B 66.10 (2002): 104406. [6] D. Henrard, et al., Journal of Nanomaterials 2019 (2019).

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/6279613868c29c4338baf60488d7fb64.jpg)
Fig. 1: Core size distributions of two selected as-made γ-Fe2O3/SiO2 core-shell particle samples fitted from corresponding m-H curves with a superposition of Langevin functions.

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/826ddadf83bfd7ab6d66c2fb0a51f531.jpg)
Fig. 2: m-H curve of as-made 5.4nm γ-Fe2O3/SiO2 core-shell particles measured by VSM together with fitted curve with a superposition of Langevin functions.

 Advanced Size Distribution Determination of Superparamagnetic Nanoparticles

Magnetic nanoparticles reveal unique magnetic properties making them relevant for data storage, electronic and mechanical engineering, and biomedical applications. Despite the considerable technological relevance and fundamental importance, a key challenge in magnetic nanoparticle research remains in the quantitative interpretation of the three-dimensional magnetic configuration and the nanoscale distribution of magnetization and spin disorder. Disorder effects - being intrinsic to nanomaterials - crucially determine the magnetization properties such as the heating performance of magnetic nanoparticles [1-4]. In this regard, the main aspects of fundamental interest are the effective magnetic anisotropy and the magnetization distribution within individual nanoparticles. Polarized, magnetic contrast-enhanced small-angle neutron scattering (SANS) is a versatile technique to investigate the chemical morphology and magnetization with nanoscale spatial resolution [5]. Addressing structural and magnetic inhomogeneities on the nanoscopic length scales of 1-300 nm, magnetic SANS is highly relevant for a variety of materials classes ranging from permanent magnets, magnetic steels and alloys to vortex lattices, skyrmions, and ferrofluids. For monodisperse nanoparticles, magnetic SANS has the unique potential to isolate core and surface-related effects of magnetization and spin disorder. In this contribution, we will present our recent results on the spin disorder in ferrite nanoparticles induced during synthesis. For the synthesis of iron oxide nanoparticles via thermal decomposition of iron oleates [7], the initial formation of FeO nanoparticles followed by topotaxial oxidation to magnetite and maghemite is well established [8,9]. Polarized SANS offers a great potential for the understanding of the microstructure in such heterostructured nanoparticles and allows to disentangle the magnetic field response of core and shell magnetization. For cobalt ferrite nanoparticles, our polarized SANS study reveals even in the wuestite-like nanoparticle core a significant magnetization contribution at ambient temperature (Fig. 1), in contrast to the conventionally assumed paramagnetic or AFM behavior. This FiM@FiM core-shell morphology explains the origin of the low-temperature exchange-bias phenomenon. Despite the overall homogeneous Co:Fe distribution within the nanoparticles, the sensitivity of SANS to nanoscale density variations enables us to verify the chemical core-shell morphology for as-prepared cobalt ferrite nanoparticles. We analyze the progressive oxidation of the core and the aging process into single-phase ferrite nanoparticles with nearly homogeneous magnetization distribution. This process occurs within years and does not compromise the size distribution or stability of the dispersion. In an idealized picture, one would consider such single-crystalline magnetic nanoparticles as defect-free nanocrystals with a collinearly magnetized core. In real systems, however, the internal spin structure exhibits a greater complexity, e.g., at the surface where compositional and structural defects are ubiquitous. As a result, the surface region is described as a shell of magnetically disordered surface spins. Polarized SANS has the necessary sensitivity to resolve the spatial distribution of spin disorder in fine detail. We have recently shown that the magnetization configuration inside magnetic nanoparticles may not be static – as often presumed – but rather susceptible to magnetic fields with the occurrence of field-dependent magnetization processes [6]. We have established a significant field-induced growth of the total particle moment by a magnetic ordering transition at the structurally disordered surface (Fig. 2). In our study, polarized SANS extends the traditional macroscopic magnetic characterization and reveals the local magnetization response. This approach allows us to quantitatively separate surface-spin disorder from intra-particle disorder contributions. Finally, we have elucidated the intra-particle spin-disorder energy, giving indirect insight into the structural defect profile in magnetic nanoparticles.

**References:**

[1] P. Bender et al., J. Phys. Chem. C, 122, 3068 (2018). [2] A. Lak et al., Nano Lett., 18, 6856 (2018). [3] A. Lappas et al., Phys. Rev. X, 9, 041044. [4] A. Lak, S. Disch, P. Bender, Adv. Science, accepted (2020). [5] S. Mühlbauer, D. Honecker, S. Disch, A. Michels et al., Rev. Mod. Phys., 91, 015004 (2019). [6] D. Zákutná, D. Honecker, S. Disch et al., Phys. Rev. X, 10, 031019 (2020). [7] T. Hyeon, Chem. Comm., 927 (2003). [8] E. Wetterskog et al., ACS Nano, 7, 7132 (2013). [9] R. Ichikawa et al., Small, 14, 1800804 (2018).

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/512f07f4eb799d5c5563531026bd63e4.jpg)
Fig. 1: Polarized SANS reveals distinct magnetization in the wuestite-like core (green) and spinel-type shell (red) of as-synthesized ferrite nanoparticles. The volume average magnetization (orange) is in excellent agreement with macroscopic magnetization (blue). Ageing (right panel) leads to the single-phase behavior of homogeneous ferrite nanoparticles.

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/2df2e75052850c79d8f659ba5207bc1c.jpg)
Fig. 2: In a strong magnetic field, the collinearly magnetized cores of ferrite nanoparticles grow due to the gradual alignment of initially disordered surrounding spins [6].

 Revealing Magnetic Morphologies and Spin Disorder in Ferrite Nanoparticles using polarized SANS

I. INTRODUCTION Although ferromagnetic particles can nowadays be grown in various size and shapes, controlling the crystallinity and microstructure parameters have remained challenging.[1,2] Nanomagnets with single-crystalline structures are particularly important because they typically exhibit reduced crystalline defects. Motivated by these prospects, our group has been established efforts in producing single-crystal and single-domain nanowires (NWs) through chemical process.[3-5] The single-domain structure led to changes in the magnetization reversal mechanism from the complicated domain-wall-motion-related process to a magnetic moment rotation mechanism that found to results in record high coercivity. Having a technique at hand that could extend growth to oriented magnetic NW array films would be highly desirable. Thin films of magnetic materials with high perpendicular anisotropy and coercivity have great application potential in ultrahigh-density perpendicular magnetic recording, permanent magnets, and spintronic and magnetoresistance sensors.[6] However, to synthesize and organize magnetic NWs to a vertically oriented structure is still a challenging task because of its dipolar interaction between neighboring NWs. In this work, we demonstrate bottom-up epitaxial solution growth of ferromagnetic Co NW arrays on crystalline metal surfaces. It is found that the coercivity of the NW arrays is strongly related to the wire diameter, film thickness, and orientation. This study provides a simple procedure to achieve recording media with ultra-high-recording densities. II. EXPERIMENTAL SECTION Single step chemical approach was used to fabricate the vertically aligned Co NW array films. In a typical synthesis, silicon substrates sputtered with Pt (111) film were kept in the solution of 1,2-butanediol, cobalt (II) laurate, and hexadecylamine (HDA). The growth was allowed for 12 h at 180 C in a Teflon-lined stainless-steel hydrothermal reactors. The diameter of Co NWs was controlled by varying the Pt film thickness from sub-10 nm to 100 nm. III. RESULTS AND DISCUSSION Figures 1a-c show top view scanning electron microscopy image of Co NW arrays having wire diameter of 12-20 nm. The NW array film is highly dense, and nanowires are uniformly distributed over large wafer-scale area (25 x 25 mm) with an areal density up to 5.6 × 1012 wires/in2. The cross-sectional view (inset of Figures 1a-c) of the as-grown film demonstrates that the NWs are vertically aligned. High-resolution TEM imaging and X-ray diffraction (XRD) measurements demonstrate the epitaxial growth of cobalt on platinum, with c-axis along the long-axis of NWs (i.e perpendicular to the film). As one would expect, the 6-fold symmetry of the Pt(111) surface favors Co crystal growth along the hexagonal (0001) wire basal planes and hence with a single in-plane orientation. Figures 1d-e shows the room temperature magnetic hysteresis loops of the Co NWs arrays of wire diameters 12-20 nm. It is found that the coercivity for the NW arrays along the wires axis () increases from 3.4 kOe to 7 kOe with the decrease of diameter. In addition, it can also be seen from Figures 1d-e that the squareness in hysteresis loop and coercivity in the parallel direction of NWs are larger than those in the perpendicular direction, which reveals that the easy axis of the Co NWs is parallel to the wire axis. Although the NW array film shows a typical perpendicular anisotropic behavior with high coercivity along NW axis, the squareness ratio of MR/MS &lt; 0.9. The low value of squareness could be due to the closely packed NW array, which induces a demagnetizing field along the plane of the film. The effective magnetic anisotropy of the NWs in an array film can results from the interplay of three major effects:1) the macroscopic demagnetization field, Hd = -6πMsp, where p is the porosity of the film and Ms is bulk value of the saturation magnetization for Co; 2) the shape anisotropy of individual nanowire Hsh= 2πMs; and 3) magnetocrystalline anisotropy field, Hm = -2K1/Ms, where K1 is the magnetocrystalline anisotropy constant for Co.[7] Thus, the theoretical effective coercive field of the nanowires is given by = Hd + Hsh + Hm. The calculated effective anisotropy field for Co NWs is ~12.5 kOe, which is much higher than the experimental coercivity values. The observed low coercivity in the prepared Co NW arrays is due to the strong magnetostatic coupling among the NWs, which is in agreement with those reported in the literature.[8] IV. CONCLUSIONS In conclusion, highly ordered Co NW arrays with coercivity comparable to magnetocrystalline anisotropy have been successfully fabricated via a simple chemical synthesis process. Magnetic measurements show that the as-prepared Co NWs with different diameters display magnetic anisotropy with the easy magnetization direction parallel to the axis of Co NW. The coercivity measured along the wire axis increases with decreasing nanowires diameter, which reveals the role of shape anisotropy in enhancing coercivity. In addition, this study opens an interesting option in tuning the magnetic properties of NW arrays and their applications in perpendicular recording media.

**References:**

[1] Y. Soumare, C. Garcia, T. Maurer, G. Chaboussant, F. Ott, F. Fiévet, J. Y. Piquemal, G. Viau, Adv. Funct. Mater. 2009, 19, 1971. [2] A. Ramazani, M. Almasi Kashi, A. H. Montazer, J. Appl. Phys. 2014, 115, 113902. [3] K. Gandha, K. Elkins, N. Poudyal, X. Liu, J. P. Liu, Sci. Rep. 2014, 4. [4] K. Gandha, J. Mohapatra, J. P. Liu, J. Magn. Magn. Mater. 2017, 438, 41. [5] J. Mohapatra, M.Y. Xing, J. Elkins, J. Beatty, J. P. Liu, Adv. Funct. Mater. 2021, doi:10.1002/adfm.202010157. [6] N. Liakakos, T. Blon, C. Achkar, V. Vilar, B. Cormary, R. P. Tan, O. Benamara, G. Chaboussant, F. Ott, B. Warot-Fonrose, E. Snoeck, B. Chaudret, K. Soulantica, M. Respaud, Nano Letters 2014, 14, 3481. [7] J. Mohapatra, J. P. Liu, in Handbook of Magnetic Materials, Vol. 27 (Ed: E. Brück), Elsevier, 2018, 1. [8] A. Encinas-Oropesa, M. Demand, L. Piraux, I. Huynen, U. Ebels, Phys. Rev. B 2001, 63, 104415.

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/1c5af62198df1058b18cbbe023632c49.jpg)
Figure 1 (a,b.c) SEM images of Co/CoO NWs array film with different wire diameters prepared via hydrothermal decomposition of cobalt carboxylate and inset shows the cross-section view of the nanowire array film. (d,e,f) The respective room temperature hysteresis loops by applying the magnetic field parallel (‖) and perpendicular (⊥) to the NW axis.

 Epitaxially Grown Single-Crystalline Cobalt Nanowires with High Coercivity

The FeRh alloy in CsCl-type (B2) phase is well-known for its metamagnetic transition from antiferromagnetic (AFM) to ferromagnetic (FM) state when the temperature increases over 370 °C, which comes with a volume expansion of 1% [1,2]. Nowadays, magneto-structural transition near room temperature are of great interest for potential applications to the control of nanostructures, magnetocaloric refrigeration and antiferromagnetic spintronics [3,4]. However, there are still open questions at nanoscale, including the finite size effects on magnetic FeRh phase transition, which require to continue efforts. The aim of this work is to explore the magnetic behavior of a 150 nm-thick FeRh nano-structured film prepared from Low Energy Cluster Beam Deposition (LECBD). Using a laser vaporization source, the initial diameter of the deposited FeRh nanoparticles is ranging from 2 nm to 10 nm in a log-normal distribution according to previous transmission electron microscopy observations [5]. The sample was annealed at 700 °C for 3 hours under vacuum in order to achieve the chemically ordered B2 phase. Then X-ray Diffraction spectrum reveals all α’-bcc peaks with a lattice parameter of 2.98 Å as expected in the B2-FeRh phase for a concentration of 48%-56% of Rh. The full width at half maximum (FWHM) of the α’(001) peak gives us an estimated crystallite size of about 30 nm in agreement with a limited coalescence upon annealing, leading to a surface granular thick-sample as observed from Atomic Force Microscope observations (Fig. 1). To study the magnetic behavior, various SQUID magnetometry measurements have been performed, including thermal dependence magnetization m(T) in the heating and cooling mode, for different values of applied magnetic field. As reported in Fig. 2, one can observe a broad and asymmetric metamagnetic transition with a significant fraction of residual magnetization at low temperature. This persistent FM state is attributed to the presence of non-switchable FM Grains. By increasing the external field, the metamagnetic transition is pushed to lower temperature following a linear correlation which is observed from the temperatures of maximum and minimum magnetization evolution as a function of field (insert Fig. 2). From Hysteresis magnetization m(H) loops a decreasing coercive field as the temperature increases has also been observed sustaining the evidence of FM regions down to low temperature. This behavior supports the coexistence of these two magnetic orders in thick nanogranular B2-like FeRh film. Moreover, field cooling - zero field cooling (FC-ZFC) susceptibility measurements have revealed the presence of single FM domains with a superparamagnetic (SPM) like-transition at temperatures higher than 130K. But because there is no exchange bias measured in m(H) loops at low temperature, there is no strong FM-AFM exchange coupling as could be expected for FM core@AFM shell morphology. In this work, the magnetic behavior of such thick nanogranular B2-like FeRh film will be described as a competition between different magnetic orders as a function of nanoparticle size, temperature and applied magnetic field. Several thermal regimes in the heating and cooling modes will be proposed as 1) Low temperature regime for T&lt;50K where small persistent FM nanoparticles co-exist with large AFM nanoparticles, 2) Intermediate regime with AFM-FM switching events and 3) at T&gt;300K the whole film is in the FM state. In the cooling mode, the FM dragging effect will be related to the applied magnetic field. A simple model could be considered with two distinct nanoparticles populations: one with smaller nanoparticles (FM/SPM) where relaxation effects avoid reaching AFM states at low temperature, and one with larger nanoparticles with AFM-compressed core@FM-relaxed shell morphology up to room temperature. To go a step further, X-ray magnetic circular dichroism results on mass-selected FeRh nanoparticles embedded in matrix recently measured at DEIMOS-SOLEIL will be discussed to illustrate finite size and surface/interface effects on metamagnetic FeRh transition.

**References:**

[1] V. L. Moruzzi and P. M. Marcus. Antiferromagnetic-ferromagnetic transition in FeRh. Phys. Rev. B 46, 2864 (1992) [2] M. R. Ibarra and P. A. Algarabel. Giant volume magnetostriction in the FeRh alloy. Phys. Rev. B 50, 4196 (1994) [3] Y. Liu, L. Phillips, R. Mattana et al. Large reversible caloric effect in FeRh thin films via a dual-stimulus multicaloric cycle. Nat. Commun. 7, 11614 (2016). [4] Y. Wang, M. M. Decker, T. N. G. Meier et al. Spin pumping during the antiferromagnetic–ferromagnetic phase transition of iron–rhodium. Nat. Commun. 11, 275 (2020). [5] V. Dupuis, A. Hillion, G. Khadra., N. Blanc, D. Le Roy, F. Tournus, C. Albin, O. boisron and A. Tamion. Cubic chemically ordered FeRh and FeCo nanomagnets prepared by mass-selected low-energy cluster-beam deposition: a comparative study. Beilstein J. Nanotechnol. 7, 1850 (2016).

**Images:**

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/d409a03b7297f8100cc511db7bddf17b.jpg)
Fig 1: Atomic Force Microscope image of the FeRh 150nm sample taken on tapping mode.

![](https://s3.eu-west-1.amazonaws.com/underline.prod/uploads/markdown_image/1/image/47e000de87e62064d603a08ea4fcdd8f.jpg)
Fig 2: Magnetization as function of the temperature for FeRh 150 nm at different external field. Inserted the temperature of maximum magnetization which follow T=338.1 K-9.11*Hμ0 K/T (blue), and temperature of minimum magnetization which follow T=321.6 K-9.11*Hμ0 K/T (yellow).

A roadmap toward expanding magnetic nanobarcodes signatures

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A roadmap toward expanding magnetic nanobarcodes signatures

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