Femtosecond X-ray magnetic circular dichroism absorption spectroscopy at an X-ray free electron laser
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Higley, Daniel J.↗
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Results for “MAGNETIC FILM”
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Annealing temperature and thickness dependence of magnetic properties in epitaxial L1{sub 0}-Mn{sub 1.4}Ga films
Mn{sub 1.4}Ga films with high perpendicular magnetic anisotropy and high crystalline quality were grown on MgO substrates with Cr buffer layer using molecular beam epitaxy. The crystalline structure and the surface morphology of the films have been systematically investigated as functions of in-situ annealing temperature (T{sub a}) and film thickness. It is found that the magnetic properties can be largely tuned by adjusting T{sub a}. As T{sub a} increases, both saturation magnetization (M{sub s}) and uniaxial perpendicular magnetic anisotropy constant (K{sub u}) increase to the maximum values of 612 emu/cc and 18 Merg/cc at 300 °C, respectively, and then decrease. The morphology also changes with T{sub a}, showing a minimum roughness of 2.2 Å at T{sub a} = 450 °C. On the other hand, as the thickness increases, M{sub s} and K{sub u} increase while coercivity decreases, which indicates there is a magnetic dead layer with a thickness of about 1.5 nm at the interfaces. The detailed examination on the surface morphology of the films with various thicknesses shows a complicated film growth process, which can be understood from the relaxation mechanism of the interfacial strain.
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗
Study of Gd-doped Bi{sub 2}Te{sub 3} thin films: Molecular beam epitaxy growth and magnetic properties
Incorporation of magnetic dopants into topological insulators to break time-reversal symmetry is a prerequisite for observing the quantum anomalous Hall (QAHE) effect and other novel magnetoelectric phenomena. GdBiTe{sub 3} with a Gd:Bi ratio of 1:1 is a proposed QAHE system, however, the reported solubility limit for Gd doping into Bi{sub 2}Te{sub 3} bulk crystals is between ∼0.01 and 0.05. We present a magnetic study of molecular beam epitaxy grown (Gd{sub x}Bi{sub 1–x}){sub 2}Te{sub 3} thin films with a high Gd concentration, up to x ≈ 0.3. Magnetometry reveals that the films are paramagnetic down to 1.5 K. X-ray magnetic circular dichroism at the Gd M{sub 4,5} edge at 1.5 K reveals a saturation field of ∼6 T, and a slow decay of the magnetic moment with temperature up to 200 K. The Gd{sup 3+} ions, which are substitutional on Bi sites in the Bi{sub 2}Te{sub 3} lattice, exhibit a large atomic moment of ∼7 μ{sub B}, as determined by bulk-sensitive superconducting quantum interference device magnetometry. Surface oxidation and the formation of Gd{sub 2}O{sub 3} lead to a reduced moment of ∼4 μ{sub B} as determined by surface-sensitive x-ray magnetic circular dichroism. Their large atomic moment makes these films suitable for incorporation into heterostructures, where interface polarization effects can lead to the formation of magnetic order within the topological insulators.
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗
Forward volume and surface magnetostatic modes in an yttrium iron garnet film for out-of-plane magnetic fields: Theory and experiment
We present experimental and theoretical results on the propagation of magnetostatic spin waves in a film of yttrium iron garnet (YIG) for out-of-plane magnetic fields for which propagation in opposite directions is nonreciprocal in the presence of a metal layer. The plane studied is defined by the film normal n and n × k where k is the wave vector of the mode. Spin waves in this setting are classified as forward volume waves or surface waves and display non-reciprocity in the presence of an adjacent metal layer except for when H//n. The measurements are carried out in a transmission geometry, and a microwave mixer is used to measure the change of phase, and with it the evolution of wavevector, of the arriving spin wave with external magnetic field.
36 MATERIALS SCIENCE↗
Local order and the dependence of magnetization on Co content in V{sub 2}O{sub 5} layered films
Local order, electronic structure, and magnetic properties of Co-doped VO{sub x} films electrochemically grown onto Si are investigated. The films are studied by means of X-ray absorption spectroscopy (XAS) and magnetic measurements. Freshly made films have V{sub 2}O{sub 5}·n(H{sub 2}O) structure with vanadium valence close to +5. XAS data show that insertion of Co in the films does not affect the close environment around V, when compared to the undoped sample, even varying the concentration of Co by ten times. The site symmetry of Co dopant atoms in the films is consistent with an octahedral coordination where Co is surrounded by six oxygen atoms, as supported by X-ray absorption near-edge structure simulations. Furthermore, there is no evidence of the presence of metallic cobalt (Co{sup 0}) in the films. The incorporation of small amounts of Co turns ferromagnetic undoped samples into paramagnetic ones. The net magnetic moment per unit volume initially decreases with the incorporation of Co and enhances for higher concentrations. Such behavior is consistent with an O vacancy reduction process driven by the insertion of Co in the films.
37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗
Growth of L1{sub 0}-ordered crystal in FePt and FePd thin films on MgO(001) substrate
Formation of L1{sub 0}-oredered structure from disordered A1 phase has been investigated for FePt and FePd films on MgO(001) substrates employing a two-step method consisting of low temperature deposition at 200 °C followed by high-temperature annealing at 600 °C. L1{sub 0}-(001) variant crystal with the c-axis perpendicular to the substrate grows preferentially in FePd films whereas L1{sub 0}-(100), (010) variants tend to be mixed with the L1{sub 0}-(001) variant in FePt films. The structure analysis by X-ray diffraction indicates that a difference in A1 lattice strain is the influential factor that determines the resulting L1{sub 0}-variant structure in ordered thin films. Misfit dislocations and anti-phase boundaries are observed in high-resolution transmission electron micrographs of 10 nm-thick Fe(Pt, Pd) film consisting of L1{sub 0}-(001) variants which are formed through atomic diffusion at 600 °C in a laterally strained FePt/PeFd epitaxial thin film. Based on the experimental results, a nucleation and growth model for explaining L1{sub 0}-variant formation is proposed, which suggests a possibility in tailoring the L1{sub 0} variant structure in ordered magnetic thin films by controlling the alloy composition, the layer structure, and the substrate material.
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗
Exploring Structural Anisotropy in Amorphous Tb-Co via Changes in Medium-Range Ordering
Amorphous thin films grown by magnetron co-sputtering exhibit changes in atomic structure with varying growth and annealing temperatures. Structural variations influence the bulk properties of the films. Scanning nanodiffraction performed in a transmission electron microscope (TEM) is applied to amorphous Tb 17 Co 83 (a-Tb-Co) films deposited over a range of temperatures to measure relative changes in medium-range ordering (MRO). These measurements reveal an increase in MRO with higher growth temperatures and a decrease in MRO with higher annealing temperatures. The trend in MRO indicates a relationship between the growth conditions and local atomic ordering. By tilting select films, the TEM measures variations in the local atomic structure as a function of orientation within the films. The findings support claims that preferential ordering along the growth direction results from temperature-mediated adatom configurations during deposition, and that oriented MRO correlates with increased structural anisotropy, explaining the strong growth-induced perpendicular magnetic anisotropy found in rare earth–transition metal films. Beyond magnetic films, we propose the tilted FEM workflow as a method of extracting anisotropic structural information in a variety of amorphous materials with directionally dependent bulk properties, such as films with inherent bonding asymmetry grown by physical vapor deposition.
36 MATERIALS SCIENCE↗
Stacking Domain Wall Magnons in Twisted van der Waals Magnets
In this report using bilayer CrI 3 as an example, we demonstrate that stacking domain walls in van der Waals magnets can host one-dimensional (1D) magnon channels, which have lower energies than bulk magnons. Interestingly, some magnon channels are hidden in magnetically homogeneous background and can only be inferred with the knowledge of stacking domain walls. Compared to 1D magnons confined in magnetic domain walls, 1D magnons in stacking domain walls are more stable against external perturbations. We show that the relaxed moiré superlattices of small-angle twisted bilayer CrI 3 is a natural realization of stacking domain walls and host interconnected moiré magnon network. Our Letter reveals the importance of stacking domain walls in understanding magnetic properties of van der Waals magnets and extends the scope of stacking engineering to magnetic dynamics.
2-dimensional system↗
Epitaxial Fe-Ge thin films on Ge(111): Morphology, structure, and magnetic properties versus stoichiometry
We have studied the growth and magnetic properties of thin Fe-Ge films synthesized (codeposited at room temperature and postannealed at 250 deg. C) on Ge(111) wafers versus stoichiometry. Morphology and crystal structure have been investigated in situ by means of scanning tunneling microscopy, low-energy electron diffraction, and x-ray photoelectron diffraction and ex situ with x-ray diffraction. The magnetic properties were characterized ex situ by conventional polar and longitudinal magneto-optical Kerr effect and transverse biased initial inverse susceptibility and torque measurements. It is found that the growth is epitaxial for Ge content up to approx48 at. % (approxFe{sub 1.1}Ge composition). In particular, the film is homogeneous and flat and adopts a crystalline structure of hexagonal symmetry derived from the B8{sub 2} (Ni{sub 2}In) structure over a wide stoichiometry range extending from Fe{sub 2}Ge to Fe{sub 1.1}Ge. The epitaxial orientation between the Ge substrate and the germanide layer is (0001)Fe-Ge||(111)Ge with [1120]Fe-Ge||110]Ge. We found however that the surface periodicity and the out-of-plane lattice parameter c evolve within this stoichiometry range and two distinct stoichiometry regimes appear on both sides of a critical stoichiometry (approxFe{sub 1.5}Ge). Indeed, from Fe{sub 2}Ge to Fe{sub 1.5}Ge the surface periodicity is p(2x2) and c continuously decreases with Fe content, whereas from Fe{sub 1.5}Ge to Fe{sub 1.1}Ge the surface periodicity is (sq root(3)xsq root(3))R30 deg. and c remains constant. These features have been interpreted as a clear fingerprint of a minor transformation of the crystalline structure but without any change in symmetry. This structural order transformation is discussed in relation to previous results reported in the case of macroscopic single-crystal Fe-Ge ingots. On both sides of the wide [Fe{sub 2}Ge,Fe{sub 1.1}Ge] composition range the layer is no more homogeneous. More precisely, for higher Fe content the film contains both the above mentioned Ni{sub 2}In-derived phase and a Fe-richer phase (probably bcc Fe) whereas for higher Ge content the layer is amorphous. Magnetic characterization showed in particular that the homogeneous Ni{sub 2}In-derived epilayers are ferromagnetic with a Curie temperature that varies drastically with the stoichiometry, rising up to a high T{sub C} value of approx450 K for the Fe-rich Fe{sub 1.9}Ge composition. Finally, whatever the stoichiometry, the magnetic easy axis of the homogeneous phase lies in the film plane and a small uniaxial anisotropy is superimposed on a sixfold order one that results from the hexagonal symmetry of the crystallographic structure.
36 MATERIALS SCIENCE↗
Emergence of exchange bias and giant coercive field enhancement by internal magnetic frustration in La 0.67 Sr 0.33 MnO 3 thin films
We have studied the influence of controlled defects on the magnetic properties of La 0.67 Sr 0.33 MnO 3 (LSMO) thin films. We used 100 nm thick epitaxial LSMO films, which were grown on SrTiO 3 substrates and introduced stoichiometry changes and defects using oxygen ion irradiation through nanoporous alumina masks. Oxygen irradiation through the mask creates cascades of defects in spatially-modulated regions in the plane of the LSMO film. The magnetic properties of the samples were compared before and after the irradiation. We have found that irradiation reduces the ferromagnetic ordering temperature, decreases the total magnetization, enhances the coercivity, and induces exchange bias below 50 K. The coercivity enhancement is dramatically higher below 50 K and can be associated with exchange bias. These results can be explained by the formation of Mn-rich antiferromagnetic or ferrimagnetic phases within the bombarded regions that are exchange coupled to the non-irradiated - ferromagnetic host.
36 MATERIALS SCIENCE↗
Scaling of the anomalous Hall effect in lower conductivity regimes
In this paper, the scaling of the anomalous Hall effect (AHE) was investigated using amorphous and epitaxial Fe x Si 1-x (0.43 < x < 0.71) magnetic thin films by varying the longitudinal conductivity $(\sigma_{xx})$ using two different approaches: modifying the carrier mean free path $(l)$ with chemical or structural disorder while holding the carrier concentration $(n_{h})$ constant or varying n h and keeping l constant. The anomalous Hall conductivity $(\sigma_{xy})$ , when suitably normalized by magnetization and n h , is shown to be independent of $\sigma_{xx}$ for all samples. This observation suggests a primary dependence on an intrinsic mechanism, unsurprising for the epitaxial high conductivity films where the Berry phase curvature mechanism is expected, but remarkable for the amorphous samples. Finally, that the amorphous samples show this scaling indicates a local atomic level description of a Berry phase, resulting in an intrinsic AHE in a system that lacks lattice periodicity.
71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSIC↗
Magnetized, radiofrequency-driven hollow cathode chemical-vapor deposition of ultrathick hydrogenated amorphous carbon
Amorphous carbon is an attractive material for next-generation inertial confinement fusion (ICF) ablators due to its amorphous structure, tunable density, compatibility with dopants, chemical inertness, and mechanical robustness. Ablators are typically deposited as ultrathick (10–200 μm) coatings on removable spherical templates. The deposition of such thick amorphous carbon films is challenging due to high intrinsic compressive stress, which causes film buckling and delamination. Here, we study the deposition of amorphous carbon films by magnetized, radiofrequency-driven hollow cathode chemical vapor deposition with a custom-designed source in Ne plasmas. Emphasis is on the hollow-cathode source design and effects of the plasma discharge power and the precursor flow rate on film properties. We demonstrate deposition rates of >1 μm/h for films with hydrogen content of ∼40 at. %, densities of 1.1–1.7 g/cm 3 , and trace quantities of oxygen impurities. In conclusion, we also demonstrate the feasibility of depositing thick hydrogenated amorphous carbon films (∼30 μm) for ICF applications.
Carbon based materials↗
Surface and magnetic characteristics of Ni-Mn-Ga/Si (100) thin film
Polycrystalline Ni-Mn-Ga thin films have been deposited on Si (100) substrate with different film thickness. The influence of film thickness on the phase structure and magnetic domain of the films has been examined by scanning electron microscope, atomic force microscopy and magnetic force microscopy. Analysis of structural parameters indicates that the film at lower thickness exhibits the coexistence of both austenite and martensite phase, whereas at higher thickness L1{sub 2} cubic non magnetic phase is noticed. The grains size and the surface roughness increase along with the film thickness and attain the maximum of 45 nm and 34.96 nm, respectively. At lower film thickness, the magnetic stripe domain is found like maze pattern with dark and bright images, while at higher thickness the absence of stripe domains is observed. The magnetic results reveal that the films strongly depend on their phase structure and microstructure which influence by the film thickness.
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗
Magnetic resonance imaging features of pubic symphysis urinary fistula with pubic bone osteomyelitis in the treated prostate cancer patient
Introduction: Pubic bone osteomyelitis with pubic symphysis urinary fistula represents a debilitating complication of radiation and ablative treatments for prostate cancer. The definitive radiographic diagnosis of this clinical entity is not described. In this study, we characterize the plain film and magnetic resonance imaging findings of pubic osteomyelitis. Materials and Methods: We reviewed a database of prostate cancer survivors with diagnosed pubic osteomyelitis from 2011 to 2015. These patients underwent pelvic plain radiographs and magnetic resonance imaging with T1-weighted and fat-suppressed T2-weighted fast spin echo sequences. Intravenous gadolinium was utilized. The diagnosis was verified with extirpative surgery. 16 patients with diagnosed pubic osteomyelitis from 2011 to 2015 underwent imaging at our institution. Results: All patients demonstrated increased signal on T2- weighted sequences and decreased signal on T1-weighted sequences along the pubic symphysis and the marrow of the involved pubic rami. Inflammatory myositis with diastasis of the pubic symphysis and cortical bone erosion were identified in the majority of patients. Fluid collections were identified in 75% of patients. 63% of conventional radiographs demonstrated no radiographic evidence of pubic osteomyelitis. Conclusion: Magnetic resonance imaging of pubic symphysis osteomyelitis in the prostate cancer survivor is characterized by high signal on T2-weighted images and low signal on T1-weighted images of the involved pubic rami, with the majority of patients demonstrating regional myositis. Imaging data combined with clinical assessment should prompt diagnosis and management of pubic osteomyelitis. Conventional radiography is generally insensitive to these findings. We consider magnetic resonance imaging to be the definitive diagnostic modality for this clinical entity.
62 RADIOLOGY AND NUCLEAR MEDICINE↗
Structural, magnetic, and transport properties of sputtered hexagonal MnNiGa thin films
We report on a systematical study of the structure, magnetism, and magnetotransport behavior of the hexagonal MnNiGa films deposited on thermally oxidized Si (001) substrates by magnetron sputtering. X-ray diffractions reveal that all the films deposited at different temperatures crystallized in hexagonal Ni{sub 2}In-type structure (space group P6{sub 3}/mmc). Scanning electron microscopy observations show that the surface morphology of the films varies with deposition temperature, and energy dispersive spectroscopy analysis shows compositions of the films remain nearly unchanged, independent of the deposition temperature. Magnetic measurements indicate that all films are ferromagnetic and exhibit a magnetic anisotropy behavior. The magnetoresistance (MR) exhibits a negative temperature- and field-dependent behavior. The possible origin of the negative MR is discussed. Furthermore, we found that the Hall effect is dominated by an anomalous Hall effect (AHE) only due to skew scattering independent of the deposition temperature of films. Moreover, the anomalous Hall resistivity presents a non-monotonously temperature-dependent behavior.
36 MATERIALS SCIENCE↗
Vortex-antivortex coexistence in Nb-based superconductor/ferromagnet heterostructures
Low-temperature magnetic force microscopy was used to study the threshold of nucleation of spontaneous vortex-antivortex structures in superconductor/ferromagnet (S/F) hybrid systems. We investigated S/F heterostructures composed of Py as the magnetic material and Nb as the superconductor, with different thicknesses of Py and Nb. The condition for nucleation of spontaneous vortex-antivortex structures depends on fundamental parameters such as the superconducting penetration depth and the coherence length, as well as on the thickness of the superconducting film and the magnetic domain width. Here, we compare our experimental results with those of existing theoretical models and provide an estimate of the threshold of the local out-of-plane component of the magnetization for different Py film thicknesses.
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗
Large moments in bcc Fe x Co y Mn z ternary alloy thin films
The elemental magnetic moments and the average atomic moment of 10-20 nm thick single crystal bcc (bct) Fe x Co y Mn z films deposited on MgO(001) have been determined as a function of a broad range of compositions. Thin film epitaxy stabilized the bcc structure for 80% of the available ternary compositional space compared to only a 23% stability region for the bulk. The films that display ferromagnetism represent 60% of the available compositional possibilities compared to 25% for the bulk. A maximum average atomic moment of 3.25 ± 0.3 μ B /atom was observed for a bcc Fe 9 Co 62 Mn 29 film (well above the limit of the Slater-Pauling binary alloy curve of 2.45 μ B /atom). Furthermore, the Fe x Co y Mn z ternary alloys that exhibit high moments can only be synthesized as ultrathin films since the bcc structure is not stable in the bulk for those compositions.
36 MATERIALS SCIENCE↗
A Disruptive Approach to Electric Vehicle Power Electronics Final Report
This project developed and demonstrated a new power electronics technology for electric vehicle drivetrains, that achieved significant improvements in power density and efficiency over standard drive cycles, relative to the commercial state of the art. In particular, the prototype measured loss and efficiency curves demonstrated a reduction in total loss over the US EPA US06 drive cycle by a factor of four. Similar reductions are observed for urban (UDDS) and highway (HWFET) drive cycles. Further, the project demonstrated a significant reduction in the total film capacitor requirements, by over an order of magnitude; this was achieved through fundamental improvements in converter circuit topologies. These nonincremental technology advances can lead to significant improvements in temperature rise, reliability, cost, and cooling system size and weight. These results were achieved through a new proposed composite converter architecture, and were demonstrated in a boost-type system similar to that employed by Toyota, Ford, and Honda. A 30 kW silicon prototype achieved a US06 average efficiency of 97.5%, which represents a reduction in average loss by a factor of approximately four relative to the 92.5% average efficiency of the commercial state of the art. A silicon carbide prototype achieved similar efficiency, while also achieving power densities of 23 kW/L (volumetric) and 20 kW/kg (gravimetric) in a boost dc-dc system including magnetics and film capacitors. This was achieved with a SiC switching frequency of 240 kHz, which allowed employment of planar magnetics. These power densities are roughly four times better than the commercial state of the art, and significantly exceed the DOE APEEM 2020 goals. In addition to the composite boost system, a SiC inverter was demonstrated at the 800 V 30 kW level. This inverter was demonstrated driving a permanent magnet machine over the US 06 drive cycle. The replacement of 1200 V Si IGBTs with 1200 V SiC MOSFETs led to improvement of CAFE average efficiency from 98.7% to 99.5%, which corresponds to a reduction of average loss by a factor of approximately two. The modular nature of the composite converter architecture opens the possibility of reuse of one or more converter modules during charging operations, providing a path for onboard charging capability at significant power levels while significantly reducing the volume and weight of the added charger module. This project demonstrated an integrated Level II charger whose add-on specific weight was approximately four times better than the DOE PHEV charger 2022 targets.
33 ADVANCED PROPULSION SYSTEMS↗