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               <dc:title>Microstructure, martensitic transformation kinetics, and magnetic properties of (Ni50Mn40In10)100−xCox melt-spun ribbons</dc:title>
               <dc:creator>Bekhouche, Ahlem</dc:creator>
               <dc:creator>Alleg, Safia</dc:creator>
               <dc:creator>Dadda, Karima</dc:creator>
               <dc:creator>Daoudi, Ibrahim Mourad</dc:creator>
               <dc:creator>Saurina Canals, Joan</dc:creator>
               <dc:creator>Suñol Martínez, Joan Josep</dc:creator>
               <dc:subject>Transformacions martensítiques</dc:subject>
               <dc:subject>Martensitic transformations</dc:subject>
               <dc:subject>Microestructura</dc:subject>
               <dc:subject>Microstructure</dc:subject>
               <dc:subject>Aliatges</dc:subject>
               <dc:subject>Alloys</dc:subject>
               <dc:description>The effect of Co-doping on the structure, microstructure, martensitic phase transformation kinetics, and magnetic properties of the melt-spun (Ni50Mn40In10)1−xCox (x = 1, 2, and 3) Heusler ribbons, named hereafter Co1 (x = 1), Co2 (x = 2), and Co3 (x = 3), was assessed using X-ray diffraction, scanning electron microscope, energy-dispersive spectroscopy, X-ray fluorescence, differential scanning calorimetry, and vibrating sample magnetometer. The XRD results reveal the formation of a 14M martensite structure alongside the face-centered-cubic (fcc) γ phase. The crystallite size ranges between 50 and 98 nm for the 14M martensite and from 9 to 16 nm for the γ phase. The mass fraction of the γ phase lies between 36.4 and 44.2%. Co-doping affects the lattice parameters and the characteristic temperatures (martensite start, martensite finish, austenite start, and austenite finish). The calculated activation energy values for the non-isothermal martensitic transformation kinetics are 257 kJ mol−1 and 135.6 kJ mol−1 for the Co1 and Co2, respectively. The produced ribbons show a paramagnetic behavior. The variation in the coercivity can be related to the crystallite size and mass fraction of the γ phase. The produced ribbons exhibit an exchange bias at room temperature that decreases with increasing the Co content</dc:description>
               <dc:description>Open Access funding provided thanks to the CRUE-CSIC agreement with Springer Nature</dc:description>
               <dc:date>2024-10-29T20:42:12Z</dc:date>
               <dc:date>2024-10-29T20:42:12Z</dc:date>
               <dc:date>2024-06-06</dc:date>
               <dc:type>info:eu-repo/semantics/article</dc:type>
               <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
               <dc:type>peer-reviewed</dc:type>
               <dc:identifier>http://hdl.handle.net/10256/25079</dc:identifier>
               <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1007/s10973-024-13277-3</dc:relation>
               <dc:relation>info:eu-repo/semantics/altIdentifier/issn/1388-6150</dc:relation>
               <dc:relation>info:eu-repo/semantics/altIdentifier/eissn/1588-2926</dc:relation>
               <dc:rights>Attribution 4.0 International</dc:rights>
               <dc:rights>http://creativecommons.org/licenses/by/4.0/</dc:rights>
               <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
               <dc:publisher>Springer Nature</dc:publisher>
               <dc:source>Journal of Thermal Analysis and Calorimetry, 2024, vol. undef, núm. undef</dc:source>
               <dc:source>Articles publicats (D-F)</dc:source>
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