2007
DOI: 10.1016/j.jallcom.2006.09.105
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Magnetic entropy changes of NiMnGa alloys both on the heating and cooling processes

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Cited by 15 publications
(10 citation statements)
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“…12 If the martensitic transformation is tuned to be coupled with the magnetic transition, i.e., the magnetostructural transformation, the MCE becomes giant. 3,12 Currently, large MCE has been observed in single crystals, 3 polycrystalline bulk alloys, [12][13][14][15][16][17][18][19][20] and melt-spun ribbons 21,22 with magneto-unistructural transformation. The highest DS M of À86 J kg À1 K À1 was achieved in singlecrystalline Ni 55 Mn 20 Ga 25 alloy at a magnetic field change of about 5 T. 3 However, the high cost and complexity associated with the fabrication of single crystals becomes an unavoidable hindrance for practical applications.…”
mentioning
confidence: 99%
“…12 If the martensitic transformation is tuned to be coupled with the magnetic transition, i.e., the magnetostructural transformation, the MCE becomes giant. 3,12 Currently, large MCE has been observed in single crystals, 3 polycrystalline bulk alloys, [12][13][14][15][16][17][18][19][20] and melt-spun ribbons 21,22 with magneto-unistructural transformation. The highest DS M of À86 J kg À1 K À1 was achieved in singlecrystalline Ni 55 Mn 20 Ga 25 alloy at a magnetic field change of about 5 T. 3 However, the high cost and complexity associated with the fabrication of single crystals becomes an unavoidable hindrance for practical applications.…”
mentioning
confidence: 99%
“…The preparation and subsequent heat treatment of the polycrystalline ingots are the same as those in Refs. [15] and [16]. The x-ray powder diffraction measurements were investigated with Cu Kα radiation to prove the present samples crystallised in the non-modulated tetragonal martensitic structure at room temperature without secondary phase.…”
Section: Methodsmentioning
confidence: 92%
“…The x-ray powder diffraction measurements were investigated with Cu Kα radiation to prove the present samples crystallised in the non-modulated tetragonal martensitic structure at room temperature without secondary phase. [15,16] Magnetisation data were measured in fields from 0 to 2 T by vibrating sample magnetometer (VSM). The measurements of heating and cooling isothermal magnetisation curves were carried out by the following steps: at first, the sample was cooled to temperatures far below the Curie temperature T C and then heated to temperature near T C , after that the measurement of the isothermal magnetisation (M -H) curve began.…”
Section: Methodsmentioning
confidence: 99%
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“…The aforementioned record-breaking values of magnetostrain, the high values of estimated magnetocaloric effect [56][57][58], and the effect of twinning-strain-induced rotation of the magnetization vector [59][60][61] are the phenomena in the focus of current research and development.…”
Section: Introductionmentioning
confidence: 99%