Houbo Zhou's research while affiliated with Chinese Academy of Sciences and other places

What is this page?


This page lists the scientific contributions of an author, who either does not have a ResearchGate profile, or has not yet added these contributions to their profile.

It was automatically created by ResearchGate to create a record of this author's body of work. We create such pages to advance our goal of creating and maintaining the most comprehensive scientific repository possible. In doing so, we process publicly available (personal) data relating to the author as a member of the scientific community.

If you're a ResearchGate member, you can follow this page to keep up with this author's work.

If you are this author, and you don't want us to display this page anymore, please let us know.

Publications (20)


Figure 1. Schematic diagram of the working principle for three regeneration modes (A) PMR, (B) AMR, and (C) HMR.
Figure 2. Structure and working principle of the HMR refrigerator (A and B) The (A) compact and (B) split sketches of the refrigerator (Ns = 8 for example). (C and D) The working principle of the refrigerator is shown in (C) the top view (Ns = 8) and (D) temperature-entropy diagram (Brayton cycle). In simulations, the inner and outer radii of the investigated devices were 1 and 10 mm, respectively, while the CL thickness was set as 0.1 or 0.2 mm and the RL thickness ranged from 0.09 to 0.18 mm.
Figure 3. Impact of structural parameters and frequency on refrigeration performance of Gd-Cu (A) Temperature span (DT span ) and regeneration factor (R f ) versus utilization factor (U f ) at different working frequencies. (B) DT span and R f as a function of Ns for different working frequencies at an optimal U f of 1.0. (C) Evolution of the DT span and R f with working frequency for a U f of 1.0. (D) Frequency evolution of the thermal diffusion length of MCM-Gd, MCM-LFS, and HTCM-Cu elements, where the horizontal lines denote the element thickness of the investigated devices for Cu, Gd, and LFS. The purple and orange shaded areas in (C) and (D) denote the frequency areas where the heat transfer is sufficient and insufficient, respectively. (E and F) DT span (E) and exergy efficiency (h; F) versus specific cooling power (SCP) for different frequencies at a fixed U f = 1.0. The dashed lines in (F) are a guide for the eyes.
A full solid-state conceptual magnetocaloric refrigerator based on hybrid regeneration
  • Article
  • Full-text available

May 2024

·

3 Reads

The Innovation

Yuan Lin

·

·

Wei Dai

·

[...]

·

Baogen Shen

The environmental friendliness and high efficiency of magnetocaloric refrigeration make it a promising substitute for vapor compression refrigeration. However, the common use of heat transfer fluid in conventional passive magnetic regenerators (PMRs) and active magnetic regenerators (AMRs) makes only partial materials contribute to the regeneration process, which produces large regeneration loss and greatly limits the regeneration efficiency and refrigeration performance at high frequency. Herein, we propose a new conceptual hybrid magnetic regenerator (HMR) composed of multiple solid-state high thermal conductivity materials (HTCMs) and magnetocaloric materials (MCMs), in which both HTCM and MCM elements participate in the regeneration process. This novel working mode could greatly reduce regeneration losses caused by dead volume, pressure losses, and temperature nonuniformity in heat transfer substances to markedly improve regeneration efficiency at high working frequencies. Using the experimentally obtained adiabatic temperature change and magnetic work and with the help of finite element simulation, a maximum temperature of 26 K, a dramatically large cooling power of 8.3 kW/kg, and a maximum ideal exergy efficiency of 54.2% are achieved at the working frequency of 10 Hz for an ideal prototype device of a rotary HMR magnetocaloric refrigerator, which shows potential for achieving an integrative, advanced performance against current AMR/PMR systems.

Download
Share


(a) Lattice mismatch between the bulk perovskite LaCoO3 and various substrates. (b) The crystal structures of PV-LCO film and STO/LAO substrate. (c) XRD θ-2θ scans of the PV-LCO films on the STO substrate. (d) Reciprocal space mappings of (-103) peak reflections for the PV-LCO/STO films. (e) XRD θ-2θ scans of the PV-LCO films on LAO substrate. (f) Reciprocal space mappings of (-103) peak reflections for the PV-LCO/LAO films.
(a) Surface morphology of the PV-LCO films on STO and LAO substrates. (b) XRR measurements and corresponding data fitting of LaCoO3 films grown on STO and LAO substrates. (c) The chemical depth profiles from XRR fittings. (d) The rocking curves of the LCO (002) peak for the 50 nm films on STO and LAO substrates, respectively.
(a) Temperature dependence of magnetization M(T) for the PV-LCO/STO films under field cooling, measured by applying an in-plane magnetic field H = 500 Oe. (b) In-plane (IP) and out-of-plane (OOP) magnetic hysteresis loops for the PV-LCO/STO films measured at 10 K. (c) Resistivity of the PV-LCO/STO films as a function of temperature. (d) M–T curves of the PV-LCO/LAO films under field cooling. (e) M–H curves of the PV-LCO/LAO films at 10 K. (f) Resistivity of the PV-LCO/LAO films as a function of temperature.
Magnetic force microscopy investigations on 50-nm-thick PV-LCO film. (a)–(h) Representative MFM images measured at 2 K and taken with increasing field. All images were taken in the same area after zero-field cooling. For all images, the scanning area is 1 × 1 μm². The color bar is ±8° for phase shift.
(a)–(d) The plots of χ⁻¹ vs T for PV-LCO films on STO and LAO substrates, respectively. The red line corresponds to fitting by the Curie–Weiss law, and the green line is fitting using the Griffith phase model.
The significant magnetic attenuation with submicrometer scale magnetic phase separation in tensile-strained LaCoO3 films

September 2023

·

51 Reads

APL Materials

APL Materials

It is well known that the epitaxial strain plays a vital role in tuning the magnetic states in transition metal oxide LaCoO3 films. Here, we reported a robust long-range ferromagnetic (FM) ground state in a tensile-strained perovskite LaCoO3 film on a SrTiO3 (STO) substrate, which has a very significant attenuation when the thickness ranges from 10 to 50 nm. It is speculated that such attenuation may be caused by the appearance of the cross-hatched grain boundary, which relaxes the tensile strain around the crosshatch, resulting in the local non-FM phases. Magnetic force microscope observation reveals non-FM patterns correlated with the structural crosshatches in the strain-relaxed film even down to a temperature of 2 K and up to a magnetic field of 7 T, suggesting the phase separation origin of magnetization attenuation. Furthermore, the investigations of the temperature-dependent inverse magnetic susceptibility show a deviation from the Curie–Weiss law above the transition temperature in a 50-nm-thick LaCoO3/STO film but not in the LaCoO3/LaAlO3 film, which is ascribed to the Griffiths phase due to the crosshatch-line grain boundaries. These results demonstrated that the local strain effect due to structural defects is important to affect the ferromagnetism in strain-engineered LaCoO3 films, which may have potential implications for future oxide-based spintronics.


Three-dimensional weak localization and negative magnetoresistance in high-quality PtP2 crystals

March 2023

·

29 Reads

·

1 Citation

Science China Materials

Pentagonal-ring-structured PtP2 bulk crystals and the two-dimensional (2D) PtP2 with rich theoretical physical and chemical properties have attracted considerable attention for the applications in high-performance electronic and optoelectronic devices. Here, high-quality PtP2 single crystals have been successfully prepared by using a tin flux method with the optimal molar ratios of Pt and P. 3D weak localization effect and negative magnetoresistance (NMR) are observed in the high-quality PtP2 single crystals for the first time. Crystalline structure, magnetization, and optical spectral characterizations have demonstrated that the defects in PtP2 crystals can suppress the NMR effect and magnetic ordered states. These findings open up a way to synthesize the bulk and low-dimensional noble-metal-based phosphides of high quality and provide new platforms for studying the different correlated electronic states.


Colossal barocaloric effect achieved by exploiting the amorphous high entropy of solidified polyethylene glycol

December 2022

·

213 Reads

·

3 Citations

NPG Asia Materials

The barocaloric effect (BCE) has emerged as an intense research topic in regard to efficient and clean solid-state refrigeration. Materials with solid-liquid phase transitions (SL-PTs) usually show huge melting entropies but cannot work in full solid-state refrigeration. Here, we report a colossal barocaloric effect realized by exploiting high entropy inherited from huge disorder of liquid phase in amorphous polyethylene glycol (PEG), which is solidified by introducing 5 wt.% polyethylene terephthalate (PET). Transmission electron microscopy (TEM) combined with X-ray diffraction (XRD) demonstrates the amorphous nature of the high-temperature phase after fixation by PET. Although PEG loses its –OH end mobility in amorphous solid, high entropy still retains owing to the retained high degrees of freedom of its molecular chains. The remaining entropy of amorphous PEG is up to 83% of that of liquid PEG in PEG10000/PET15000, and the barocaloric entropy change reaches ΔSp ∼ 416 J·kg⁻¹·K⁻¹ under a low pressure of 0.1 GPa, which exceeds the performance of most other BCE materials. Infrared spectra combined with density function theory (DFT) calculations disclose conformational change from the liquid to amorphous state, which explains the origin of the large entropy retained and hence the colossal BCE of the solidified PEG. This research opens a new avenue for exploring full solid-state barocaloric materials by utilizing genetic high entropy from huge disordering of liquid phases in various materials with SL-PTs.


Sensitive electric field control of first-order phase transition in epitaxial multiferroic heterostructures

September 2022

·

172 Reads

·

1 Citation

Acta Materialia

Strongly correlated electron materials that exhibit rich phase transition and multiple phase separation have shown many fascinating properties. Using these properties in the electronic device will require the ability to control their phase transition and phase separation behaviours. In this work, we report a sensitive electric field control of firstorder phase transition in epitaxial (011)-Nd 0.5 Sr 0.5 MnO 3 /0.71Pb(Mg 1/3 Nb2/3 )O 3 -0.29PbTiO 3 (PMN-PT) heterostructure. The pristine film shows phase separation character with the penetration of the ferromagnetic metallic phase into the charge and orbital ordered antiferromagnetic insulating phase in the pristine film, and this was revealed by the XMCD and XLD investigation. The (011)-oriented PMN-PT piezoelectric single crystal adopted can exert anisotropic in-plane tensile strains on the epitaxial Nd 0.5 Sr 0.5 MnO 3 film when applying the electric field. The coaction of the electric field-induced strain and polarization effects of the PMN-PT piezoelectrics enable the efficient manipulation of orbital ordering and the coupled electronic and magnetic phase transitions. Accordingly, a small +1.6 kV cm -1 electric field can recover the first-order metal-insulator transition which was inhibited in the pristine heterostructure, increase the transition temperature by 56 K and the maximum resistance change reaches 7033%. Furthermore, the electric field demonstrated nonvolatile control of magnetization, and the magnetoelectric coefficient reaches 1.89*10-7 sm -1 at 200 K. This work indicates that choosing the piezoelectric substrate with appropriate electric-field-induced strain opens a route to designing functional electronic devices where the tunable macroscopic properties derive from strongly interacting degrees of freedom present in the manganite


Compressive-Strain-Facilitated Fast Oxygen Migration with Reversible Topotactic Transformation in La 0.5 Sr 0.5 CoO x via All-Solid-State Electrolyte Gating

September 2022

·

116 Reads

·

10 Citations

ACS Nano

Modifying the crystal structure and corresponding functional properties of complex oxides by regulating their oxygen content has promising applications in energy conversion and chemical looping, where controlling oxygen migration plays an important role. Therefore, finding an efficacious and feasible method to facilitate oxygen migration has become a critical requirement for practical applications. Here, we report a compressive-strain-facilitated oxygen migration with reversible topotactic phase transformation (RTPT) in La0.5Sr0.5CoOx films based on all-solid-state electrolyte gating modulation. With the lattice strain changing from tensile to compressive strain, significant reductions in modulation duration (∼72%) and threshold voltage (∼70%) for the RTPT were observed, indicating great promotion of RTPT by compressive strain. Density functional theory calculations verify that such compressive-strain-facilitated efficient RTPT comes from significant reduction of the oxygen migration barrier in compressive-strained films. Further, ac-STEM, EELS, and sXAS investigations reveal that varying strain from tensile to compressive enhances the Co 3d band filling, thereby suppressing the Co-O hybrid bond in oxygen vacancy channels, elucidating the micro-origin of such compressive-strain-facilitated oxygen migration. Our work suggests that controlling electronic orbital occupation of Co ions in oxygen vacancy channels may help facilitate oxygen migration, providing valuable insights and practical guidance for achieving highly efficient oxygen-migration-related chemical looping and energy conversion with complex oxides.


Figure 2
Figure 3
Figure 4
Figure 5
Colossal barocaloric effect exploiting amorphous high entropy in solidified polyethylene glycol

July 2022

·

99 Reads

Barocaloric effect (BCE) has emerged as one of intense topics aiming at solid-state refrigeration featuring efficiency and cleanness. Materials with solid-liquid phase transition (SL-PT) usually show huge melting entropy but cannot work in full solid-state refrigeration. Here we report colossal barocaloric effect realized by exploiting high entropy inherited from huge disorder of liquid phase in amorphous polyethylene glycol (PEG), which is solidified through introducing 5wt.% polyethylene terephthalate (PET). TEM combined XRD demonstrate the amorphous nature of high-temperature phase after fixed by PET. Although the PEG loses the -OH end mobility in amorphous solid, high entropy still retains owing to retained high freedom of molecule chains. The remained entropy in amorphous PEG is up to 83% of liquid PEG in PEG10000/PET15000, and the barocaloric entropy change reaches ΔS p ∼ 416 J·kg − 1 ·K − 1 under a low pressure 0.1 GPa, which exceeds the performance of most other BCE materials. Infrared spectra combined with density function theory (DFT) calculations disclose conformational change from liquid to amorphous state, which explains the origin of huge entropy retained and hence colossal BCE in the solidified PEG. This research opens a new avenue for exploring full solid-state barocaloric materials by utilizing genetic high entropy from huge disordering of liquid phase in various materials with SL-PT.


The comparison of the barocaloric entropy change under hydrostatic pressure change of 0 → 1 kbar and the thermal conductivity between the present composites and the reported barocaloric materials.
(a) The schematic of the fabrication process of the NPG-GPNs composites. (b) Thermal conductivity evolution with the content of GPNs fillers of the composites, the inset in (b) denotes the fabrication stress influence on the thermal conductivity values of the composites with GPNs fillers content of 41.1 wt%. (c, d, e) SEM images of the cross-section morphology of NPG-GPNs composites plates with GPNs filler content of 9.1, 28.5, and 50 wt%.
The XRD patterns of pure (a) NPG and NPG-GPNs composites with (b) GPNs content of 28.5 wt%, and (c) GPNs content of 50 wt%, measured at various temperatures. The subscripts ‘m' and ‘c' refer to the monoclinic and cubic structures of NPG.
The dQ/dT curves of the (a1) pure NPG, NPG-GPNs composites with the NPG content of (a2) 28.5 wt%, and (a3) 50 wt%, measured under hydrostatic pressure of 0, 0.25, 0.5, 0.75, and 1.0 kbar. (b1-b3) The corresponding isobaric entropy curves S’(T, p) at different pressures for the three samples. (c1-c3) The barocaloric entropy change for hydrostatic pressure changes of 0 → 0.25 kbar, 0 → 0.5 kbar, 0 → 0.75 kbar, and 0 → 1 kbar for the compression and decompression process.
Giant barocaloric effect in neopentylglycol-graphene nanosheets composites with large thermal conductivity

June 2022

·

116 Reads

·

7 Citations

We report the enhancement of the thermal conductivity of neopentylglycol (NPG) by compositing it with graphene nanosheets (GPNs). Adding 50 wt% GPNs enhanced the thermal conductivity from 0.42 to 18.4 Wm⁻¹K⁻¹, and the barocaloric entropy change can still reach 122 Jkg⁻¹K⁻¹ under pressure loading of 0 → 1.0 kbar. The obtained composites demonstrated reduced thermal hysteresis, which will facilitate the large reversible entropy change. The present work thus provides a simple and feasible way to enhance the thermal conductivity of plastic crystals with a giant barocaloric effect, and promisingly accelerate the application of these materials in the solid-state refrigeration technique.


Reversible colossal barocaloric effect dominated by disordering of organic chains in (CH3–(CH2)n−1–NH3)2MnCl4 single crystals

April 2022

·

163 Reads

·

8 Citations

NPG Asia Materials

Solid-state refrigeration based on the caloric effect is viewed as a promising efficient and clean refrigeration technology. Barocaloric materials were developed rapidly but have since encountered a general obstacle: the prominent caloric effect cannot be utilized reversibly under moderate pressure. Here, we report a mechanism of an emergent large, reversible barocaloric effect (BCE) under low pressure in the hybrid organic–inorganic layered perovskite (CH 3 –(CH 2 ) n −1 –NH 3 ) 2 MnCl 4 ( n = 9,10), which show the reversible barocaloric entropy change as high as Δ S r ∼ 218, 230 J kg ⁻¹ K ⁻¹ at 0.08 GPa around the transition temperature ( T s ∼ 294, 311.5 K). To reveal the mechanism, single-crystal (CH 3 –(CH 2 ) n −1 –NH 3 ) 2 MnCl 4 ( n = 10) was successfully synthesized, and high-resolution single-crystal X-ray diffraction (SC-XRD) was carried out. Then, the underlying mechanism was determined by combining infrared (IR) spectroscopy and density function theory (DFT) calculations. The colossal reversible BCE and the very small hysteresis of 2.6 K (0.1 K/min) and 4.0 K (1 K/min) are closely related to the specific hybrid organic–inorganic structure and single-crystal nature. The drastic transformation of organic chains confined to the metallic frame from ordered rigidity to disordered flexibility is responsible for the large phase-transition entropy comparable to the melting entropy of organic chains. This study provides new insights into the design of novel barocaloric materials by utilizing the advantages of specific organic–inorganic hybrid characteristics.


Citations (10)


... h P e =CB m 2 f 2 d 2 /ρ, (4) H, B, B m , d, ρ, f and C represent magnetic field, induction, magnetic flux density, particle diameter, electrical resistivity, frequency and a constant, respectively. At certain B m and f, the core loss is mainly determined by particle size, electrical resistivity and H c [42][43][44]. The following part will illustrate the influence of BM on P cv from these aspects. ...

Reference:

Ultrahigh saturation magnetization in FeCoB powders with controllable amorphous-nanocrystalline structure via the synergism of deformation and energy injection变形和能量注入协同作用制备可控非晶纳米晶结构超高饱和磁化强度FeCoB粉末
Three-dimensional weak localization and negative magnetoresistance in high-quality PtP2 crystals
  • Citing Article
  • March 2023

Science China Materials

... With the growing greenhouse gas emission and energy crisis that limit the use of traditional liquid refrigerants, there is an increasing demand for solid-state refrigeration materials and technologies. [1][2][3][4][5] Among them, thermoelectric cooling [6][7][8] enabled by the Peltier effect [9][10][11][12][13][14][15][16][17] and magnetic cooling led by the magnetocaloric effect [18][19][20][21][22][23][24][25][26][27][28] are the most promising, since they have the advantages of high reliability, no moving parts, compact size, and quiet operation. However, their conversion efficiency is still much lower than conventional mechanical-compression refrigeration, making their commercial use impractical. ...

Compressive-Strain-Facilitated Fast Oxygen Migration with Reversible Topotactic Transformation in La 0.5 Sr 0.5 CoO x via All-Solid-State Electrolyte Gating
  • Citing Article
  • September 2022

ACS Nano

... At present, the means to improve the thermal conductivity of BCE materials is mainly by combining with high thermal conductivity materials (such as graphene nanosheets and expanded graphite) to make composite materials, but this will reduce the performance of refrigerants, so it is urgent to further find high thermal conductivity BCE materials and improve thermal conductivity means. 46 In this work, we investigated the BCE properties of {Fe (pz) 2 (BH 3 CN) 2 } with first-order SCO near room temperature. The DS SCO associated with the SCO process of per mole compound {Fe(pz) 2 (BH 3 CN) 2 } is $60 J mol À1 K À1 , indicating that the introduction of a third source of entropy change DS reo has a limited effect on lifting DS SCO . ...

Giant barocaloric effect in neopentylglycol-graphene nanosheets composites with large thermal conductivity
Materials Research Letters

Materials Research Letters

... The barocaloric cooling system superiorly features the accessible mechanical field, instead of costly magnetic field, and general barocaloric materials not requesting rigorous mechanical properties, which however is necessary for electrocaloric, magnetocaloric and elastocaloric materials 10,11 . Escaping from the restriction of mechanical property requirement and specific ferroicity such as ferromagnetism, ferroelectricity or ferroelasticity, barocaloric materials include a mass of structural phase change materials; developing from the incipient metallic compounds [12][13][14][15][16][17][18][19] , some emergent barocaloric materials can exhibit colossal caloric effect [20][21][22][23][24][25][26][27][28][29] with entropy change larger than 100 J kg −1 K −1 , the phase transitions of which relate to the coupling between the remarkable structural change and large orderdisorder transition of order parameters such as molecular orientation order 20,21,23,25 , conformational order of organic chain [27][28][29] and spin crossover 26 . ...

Reversible colossal barocaloric effect dominated by disordering of organic chains in (CH3–(CH2)n−1–NH3)2MnCl4 single crystals

NPG Asia Materials

... To achieve reversible magnetostrain through a magneticfield-induced phase transition, our attention is focused on MnCoSi-based alloys with a TiNiSi-type orthorhombic structure [12][13][14][15][16][17][18][19]. The stoichiometric MnCoSi alloy exhibits a nonlinear antiferromagnetic state below its Néel temperature (∼381 K) but undergoes a transition into a ferromagnetic state when the external magnetic field reaches a critical value (µ 0 H cri ) [13][14][15][16][17]19]. ...

Strengthened caloric effect in MnCoSi under combined applications of magnetic field and hydrostatic pressure

Journal of Materials Science

... From the discovery of Gd 5 (Si,Ge) 4 [1], the magnetocaloric effect (MCE) of first-order phase transition materials has gained a lot of attention as a prospective candidate material for magnetic refrigeration. As the research further develops, various problems such as the narrow cooling temperature span [13][14][15] and large hysteresis loss [16,17] in these materials gradually emerge, limiting their application. Great efforts have been made to solve these problems by doping [18,19] or introducing multi-field stimuli [20][21][22]. ...

Electric field control of the reversible magnetocaloric effect in strain-mediated Ni37.5Co12.5Mn35Ti15/PMN-PT composite
  • Citing Article
  • November 2021

Scripta Materialia

... In addition, the transition is accompanied by a piezomagnetic effect where piezomagnetic coefficient d 12 under the 3.2% strain was theoretically derived to be 1.29 eμ/g/kbar. This value is comparable to those of other piezomagnetic materials, such as 1.92 eμ/g/kbar of Mn 3 Ga 0.95 N 0.94 [38] and 4.27 eμ/g/kbar for Mn 0.87 Fe 0.13 NiGe [39]. An alternative way to tune the interlayer AFM-FM transition of CrSBr is to apply magnetic fields, which induce the nucleation and subsequent propagation of an AFM-FM phase wall [40] and anisotropic optical reflectivity [41]. ...

A Distinct Spin Structure and Giant Baromagnetic Effect in MnNiGe Compounds with Fe-Doping

Journal of the American Chemical Society

... [1][2][3][4] Therefore, solidstate cooling technology has mushroomed, as exemplified by magnetocaloric and electrocaloric effects (ECE), and so forth. [5][6][7] Ferroelectric cooling based on ECE features easier integration and miniaturization and is thus suitable for active cooling in microelectronic devices. ECE is defined as an entropy change in polar dielectrics by external electric field (E) stimuli in adiabatic conditions. ...

Regulation of phase transition and magnetocaloric effect by ferroelectric domains in FeRh/PMN-PT heterojunctions
  • Citing Article
  • April 2020

Acta Materialia

... From a crystallographic viewpoint, Fe and Co atoms would reside at three distinct crystallographic sites: Fe I (8b), Fe II (96i), and Fe (2a). Si atoms share the Fe II (96i) and Fe (2a) with Fe and Co atoms 30,31 . This occupation type results in deteriorating thermal expansion upon introduction of the α phase (Fig. 1d). ...

Large enhancement of magnetocaloric and barocaloric effect by hydrostatic pressure in La(Fe 0.92 Co 0.08 ) 11.9 Si 1.1 with NaZn 13 -type structure
  • Citing Article
  • January 2020

Chemistry of Materials

... In amorphous structures, it is furthermore possible to significantly alter the microscopic magnetic properties through sample design and growth conditions, e.g., introducing imprinted uniaxial anisotropy, or a certain amount of intermixing at the interfaces. 9,[12][13][14] In the present study, we examine the magnetic properties of a model system of rigid-exchange-coupled amorphous heterostructures, both bilayers and multilayers, with Sm 11 Co 82 Ti 7 (denoted SmCoTi) as the hard phase and Co 85 (Al 70 Zr 30 ) 15 (denoted CoAlZr) as the soft phase. 14,15 A uniaxial in-plane anisotropy has been imprinted in the samples by applying an external magnetic field during growth. ...

Tunable In-Plane Anisotropy in Amorphous Sm–Co Films Grown on (011)-Oriented Single-Crystal Substrates

Engineering