Authors: Lorena González, J. García, M. Nazmunnahar, W.O. Rosa, L. Escoda, Joan Josep Suñol, V.M. Prida, V.V. Koledov, V.G. Shavrov, B. Hernando
Abstract: We report the effect of shorttime vacuum annealing, during 10 minutes at 923 K, 973 K, 1023 K and 1073 K, on magnetostructural properties of as-quenched ribbons of Ni45.5Mn43In11.5 Heusler alloy. The martensitic transformation is strongly sensitive to annealing treatments. The martensitic phase starting temperature is significantly shifted from 239 K towards higher temperatures around 370 K. It suffers a break down in two peaks when a field equal or higher than 500 Oe is applied to the as-quenched sample. This effect is not detected in the transformation of annealed ribbons but its signature can be observed at low temperature. Moreover, under high magnetic field up to 30 kOe temperatures associated with both martensitic and reverse transitions do not change for annealed samples, meanwhile the magnetization difference between austenite and martensite increases with the field. Nevertheless, it almost remains unchanged in the as-quenched ribbon.
307
Authors: T. Sánchez, José Luis Sánchez Llamazares, B. Hernando, J.D. Santos, M.L. Sánchez, M.J. Perez, Joan Josep Suñol, Reiko Sato Turtelli, Roland Grössinger
Abstract: We report the effect of a short-time vacuum annealing (1073 K during 10 minutes) on structural phase transition temperatures and magneto-structural properties of as-quenched ribbons of the Heusler alloy Ni50.6Mn34.5In14.9. This alloy crystallizes in a single phase cubic B2-type austenite with a Curie point of TCA=284 K that with the lowering in temperature transforms into a martensite with TCM185 K. The direct and reverse martensitic phase transition temperatures were MS=257 K, Mf = 221 K, AS = 239 K, and Af = 266 K. After annealing austenite shows the highly ordered L21-type structure while the average chemical composition as well as the structural and magnetic transition temperatures were shifted to Ni50.2Mn34.3In15.5 and MS = 253 K, Mf = 238 K, AS = 257 K, Af = 265 K, ΔT = 13 K, TCA = 299 K and TCM207 K. In the annealed samples the magnetization changes associated to the magnetic and structural transitions are more abrupt and magnetization isotherms in both the austenitic and martensitic existence region show higher initial magnetic susceptibility and faster approach to saturation. Field-cooled hysteresis loops at 10 K were shifted along the negative H-axis for both samples, but a significant anomaly was evident on the left side of the hysteresis loop for as-quenched ribbons.
81
Authors: Joan Josep Suñol, L. Escoda, C. García, V.M. Prida, Victor Vega, M.L. Sánchez, José Luis Sánchez Llamazares, B. Hernando
Abstract: Glass-coated Cu-Mn-Ga microwires were fabricated by Taylor-Ulitovsky technique. By means of energy dispersive spectroscopy microanalysis, an average alloy composition of Cu56Ga28Mn16 was determined. The temperature dependence of magnetization measured at a low magnetic field showed the coexistence of two ferromagnetic phases. The Curie temperature of one phase is 125 K and above room temperature for the other one. X-ray diffraction at room temperature and at 100 K reflects the presence of the same three crystalline phases corresponding to the cubic B2 Cu-Mn-Ga structure as a main phase and the minor phases of fcc Cu rich solid solution with Mn and Ga and the monoclinic CuO.
79
Authors: Joan Josep Suñol, J. Saurina, Rastislav Varga, B. Hernando, José Luis Sánchez Llamazares, J.D. Santos, V.M. Prida
Abstract: The most extensively studied Heusler alloys are those based on the Ni-Mn-Ga system. However, to overcome the high cost of Gallium and the usually low martensitic transformation temperature, the search for Ga-free alloys has been recently attempted, particularly, by introducing In, Sn or Sb. In this work, Mn50Ni40In10, Mn50Ni34In16, Ni50Mn36-xIn14+x (x = 0, 0.5, 1, 1.5) and Ni50Mn37Sn13 ribbons has been obtained by melt spinning. We outline their structural and thermomagnetic behavior. Columnar grains and preferential orientation has been obtained. The martensitic, Tm, and the Curie, TC, temperatures of the ribbons are lower than those of the bulk samples with similar compositions. This effect is probably due to the ribbons small and constrained grains. For it, a large under-cooling is necessary for the martensitic transformation. The decrease of TC in the ribbons could be associated with the increased degree of quenched-in short-range disorder around defects.
143
Authors: P. Mendoza Zélis, C.E. Rodríguez Torres, A.F. Cabrera, M.B. Fernández Van Raap, G.A. Pasquevich, Francisco H. Sánchez, A. González, Joan Josep Suñol
571
Authors: Joan Josep Suñol, A. González
4325
Authors: Joan Josep Suñol, A. González, P. Bruna, Trinitat Pradell, Narcis Clavaguera, M.T. Mora
1927
Authors: Joan Josep Suñol, Trinitat Pradell, Narcis Clavaguera, Maria T. Clavaguera-Mora
525
Authors: Maria T. Clavaguera-Mora, Joan Josep Suñol, Narcis Clavaguera
459
Authors: Joan Josep Suñol, Trinitat Pradell, Narcis Clavaguera, Maria T. Clavaguera-Mora
525