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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Boulet, Pascal
Institut Jean Lamour
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (54/54 displayed)
- 2024<i>In situ</i> tracking the phase change in metastable copper oxide thin film via thermal oxidation
- 2024In situ tracking the phase change in metastable copper oxide thin film via thermal oxidation
- 2024Hot melt extruded amorphous solid dispersions containing lumefantrine and Solupluscitations
- 2024High quality ZnMgAlO thin films by ultrasonic spray pyrolysis: tuning of optoelectronic properties for use as TCO, window layer, and buffer layer in all-oxide solar cellscitations
- 2024Integration of epitaxial LiNbO3 thin films with silicon technologycitations
- 2024ZnMgO Thin Films by Ultrasonic Spray Pyrolysis: Modulation of Optical and Electrical Properties by Post‐annealing and Magnesium Compositioncitations
- 2023Crystal structure and ferromagnetism of the CeFe$_9$Si$_4$ intermetallic compoundcitations
- 2023Investigation of PbSnTeSe High-Entropy Thermoelectric Alloy: A DFT Approachcitations
- 2023Crystal Structure and Ferromagnetism of the CeFe₉Si₄ Intermetallic Compoundcitations
- 2023Development of a two-step process based on ultrasonic spray pyrolysis to optimize optical and electrical properties of ZnMgAlO
- 2022Crystal structure, microstructure and electronic properties of a newly discovered ternary phase in the Al-Cr-Sc systemcitations
- 2022Investigation of PbSnTeSe High-Entropy Thermoelectric Alloy: A DFT Approachcitations
- 2022Effect of Pre-Oxidation on a Ti PVD Coated Ferritic Steel Substrate during High-Temperature Agingcitations
- 2022Theoretical and experimental approaches for the determination of functional properties of MgSnN 2 thin filmscitations
- 2022Theoretical and experimental approaches for the determination of functional properties of MgSnN2 thin filmscitations
- 2022Al 4 Ir: An Al–Ir Binary-Phase Superstructure of the Ni 2 Al 3 Typecitations
- 2021Structure–Property Relationships in Transition Metal Dichalcogenide Bilayers under Biaxial Strainscitations
- 2021Continuous manufacture of hydroxychloroquine sulfate drug products via hot melt extrusion technology to meet increased demand during a global pandemic: From bench to pilot scalecitations
- 2021Continuous manufacture of hydroxychloroquine sulfate drug products via hot melt extrusion technology to meet increased demand during a global pandemic: From bench to pilot scalecitations
- 2021Investigation of the (1 0 0) and (0 0 1) surfaces of the Al5Fe2 intermetallic compoundcitations
- 2021Structural model and spin-glass magnetism of the Ce 3 Au 13 Ge 4 quasicrystalline approximantcitations
- 2021Crystal Structure, Microstructure and Electronic Properties of a Newly Discovered Ternary Phase in the Al-Cr-Sc Systemcitations
- 2021Effect of the precursor concentration on structural properties of ZnO thin films by ultrasonic spray pyrolysis
- 2021Elaboration of high-transparency ZnO thin films by ultrasonic spray pyrolysis with fast growth ratecitations
- 2020Effect of Thermal Stresses Formed during Air Annealing of Amorphous Lanthanum Cuprate Thin Films Deposited on Silicon Substratecitations
- 2020Epitaxial Growth of Sc0.09Al0.91N and Sc0.18Al0.82N Thin Films on Sapphire Substrates by Magnetron Sputtering for Surface Acoustic Waves Applicationscitations
- 2020Paramagnetism and martensite stabilization of tensile strained NiTi shape memory alloycitations
- 2020Single crystal growth, crystal structure and surface characterisation of the binary phase Al45Cr7.citations
- 2019Probing the growth window of LaVO 3 perovskites thin films elaborated using magnetron co-sputteringcitations
- 2019Probing the growth window of LaVO3 perovskites thin films elaborated using magnetron co-sputteringcitations
- 2019Study of ignition and extinction of spruce glulam exposed to a radiative flux
- 2019Overview of the U3TGe5 family with T=Ti, V, Cr, Mn, Zr, Nb, Mo, Hf, Ta and W Nine new members, phase formation, stability, structural and physical properties and electronic structurescitations
- 2019A new ternary compound with the BGa8Ir4 structure type in the Al-Au-Ir systemcitations
- 2018Chemical environment and functional properties of highly crystalline ZnSnN2 thin films deposited by reactive sputtering at room temperaturecitations
- 2018Towards stoichiometric LiNbO3 epitaxial thin films grown by DLI-MOCVD
- 2018A voltammetric study on the atomic layer deposition of selenium and antimony on platinum electrode
- 2017Surface temperature of carbon composite samples during thermal degradationcitations
- 2017LaFeOxNy perovskite thin films: Nitrogen location and its effect on morphological, optical and structural propertiescitations
- 2017Comparison between Ir, Ir 0.85 Rh 0.15 and Ir 0.7 Rh 0.3 thin films as electrodes for surface acoustic waves applications above 800°C in air atmospherecitations
- 2016Properties of rare-earth orthoferrites perovskite driven by steric hindrancecitations
- 2016Influence of plasma treatments and SnO2 alloying on the conductive properties of epitaxial Ga2O3 films deposited on C-sapphire by chemical vapor deposition
- 2016Epitaxy, optical and acoustical properties of X-, Y-, and Z-axis oriented LiNbO3 thin films on sapphire substrates
- 2016Residual stresses in X-, Y-, and Z-axis oriented LiNbO3 thin films on sapphire substrates
- 2015Thermoelectric Properties of Sn-Containing Mg 2 Si Nanostructurescitations
- 2015On the Influence of the Sample Absorptivity when Studying the Thermal Degradation of Materialscitations
- 2015AlN films deposited by dc magnetron sputtering and high power impulse magnetron sputtering for SAW applicationscitations
- 2015Tuning the structure and preferred orientation in reactively sputtered copper oxide thin filmscitations
- 2014Controlling the preferred orientation in sputter-deposited Cu2O thin films: Influence of the initial growth stage and homoepitaxial growth mechanismcitations
- 2014Testing epitaxial Co1.5Fe1.5Ge(001) electrodes in MgO-based magnetic tunnel junctionscitations
- 2013Isothermal α″ formation in β metastable titanium alloyscitations
- 2013Magnetic and electronic properties of NpCo2: Evidence for long-range magnetic ordercitations
- 2013Cation size effect on the thermochromic properties of rare earth cobaltites RECoO3 (RE: La, Nd, Sm)citations
- 2013Combined Temperature and Deformation Measurement During Glass Forming in a Real Scale Setupcitations
- 2011Experimental Investigation of Radiation Emitted by Optically Thin to Optically Thick Wildland Flamescitations
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article
Paramagnetism and martensite stabilization of tensile strained NiTi shape memory alloy
Abstract
We present an experimental and theoretical study of Pauli paramagnetism and martensite stabilization in a near equiatomic NiTi shape memory alloy. We demonstrate a direct correlation between strain-induced shear of the B19' NiTi lattice and its electronic and thermodynamical features. An increase of the monoclinic angle β from 97.4 to 98 degrees induces a 7 % decrease of the magnetic susceptibility because of a shift and deepening of a dip in B19' density of state at the Fermi level. It also produces a decrease of the B19' enthalpy, which translates into an increase of the martensite-to-austenite transition temperature by 60 K. Near equiatomic NiTi alloys carry remarkable properties such as shape memory effect and pseudoelasticity. Both effects are born of first-order reversible phase transformation between low-symmetry monoclinic B19' martensite phase and high-symmetry cubic B2 austenite phase. Tuning the transition temperatures and martensite transformation hysteresis has been a constant objective. It has yet been achieved by adjusting NixTi1-x concentration [1] or by substituting element in ternary NiTiX alloys (with X=Hf, Pd, Cu,…)[2,3]. Geometrical compatibility of B19' and B2 phases [4], change of valence electron number [5] and thermodynamics [1,6] have been investigated to explain the influence of theses chemical changes on NiTi-based alloys characteristics. Interestingly, no direct correlation between electronic features, transition temperatures and NiTi lattice distortion for a fixed concentration has yet been demonstrated, whereas the complex microstructure of NiTi under strain has been heavily studied [7-9]. Moreover, magnetism, which is known as a good probe of the electronic properties, has been rarely studied in NiTi alloys [10-13], although its impact on the magnetic resonance imaging of NiTi-based stents and biomedical implants has often been highlighted [14,15]. Here, we perform systematic X-ray diffraction (XRD) and magnetization measurements in order to characterize the influence of the tensile strain on both the martensite-to-austenite transition temperature and magnetic susceptibility of a NiTi sheet. Ab-initio calculations correlate the measured strain-induced shear of the martensite lattice to particular features of the B19' energy and density of states at the Fermi level. Figure 1. Magnetic susceptibility χ of NiTi versus temperature for as grown sample (black curve), 5% strained sample (red curve), 16.5% strained sample (blue curve). We use NiTi (50.6 at% Ti; 49.4 at% Ni ± 0.5%) free-standing polycrystalline 20µm thick sheets, grown by DC magnetron sputtering as described in details in Ref. [16]. Fig.1 shows the DC Magnetic susceptibility χ measured by SQUID magnetometer as a function of temperature under a constant magnetic field of 2T. Magnetic field is applied in the plane of the NiTi sheet. Note that χ does not depend on the measurement direction in the film plane because of the polycrystalline nature of the NiTi sheet. As-grown NiTi sample overcomes a hysteretic transition between a value M= 23 mJ.T-2 .kg-1 in the martensite phase and A=32.5 mJ.T-2 .kg-1 in the austenite phase, in agreement with [10]. A magnetic transition temperature of around 360 K (330K) matches the martensite-to-austenite (respectively austenite-to-martensite) transition in XRD curves, in agreement with [8,17] for similar concentrations. Tensile tests are performed using a Deformation Device System