Results 241 to 250 of about 28,460 (303)
Topological thermal Hall effect and nondissipative transport of the nanometric skyrmion lattice in Gd<sub>2</sub>PdSi<sub>3</sub>. [PDF]
Yamaguchi D +6 more
europepmc +1 more source
Fabrication of Janus Supraparticles by Induced Phase Separation by Gravity. [PDF]
Ramachandran S +4 more
europepmc +1 more source
Theoretical Considerations for Patient-Specific Modeling Based on Observable State Variables. [PDF]
Ateshian GA, Deiters S, Weiss JA.
europepmc +1 more source
Some of the next articles are maybe not open access.
Related searches:
Related searches:
Magnetic entropy change in Ni51.5Mn22.7Ga25.8 alloy
Applied Physics Letters, 2000A considerable magnetic entropy change has been observed in Ni51.5Mn22.7Ga25.8 alloys under a field of 0.9 T. This change originates from a sharp magnetization jump which is associated with a martensitic to austenitic structure transition. The large low field entropy change and the adjustable martensic–austensic transition temperature indicate a great ...
Fengxia Hu, Ji-Rong Sun, Shen Bao-Gen
exaly +2 more sources
Broadening of the magnetic entropy change in La0.75Ca0.15Sr0.10MnO3
Abstract A broad table-like entropy change (ΔS) at room temperature has been observed in the ferromagnetic compound La0.75Ca0.15Sr0.10MnO3, which is analyzed in the concept of Landau theory and with critical exponent analysis obtained from the magnetization measurements.
R. Venkatesh +4 more
openaire +2 more sources
Large magnetic entropy change in La0.75Ca0.25MnO3
Applied Physics Letters, 1997Magnetic entropy change of La0.75Ca0.25MnO3 with different particle size has been investigated. Magnetic entropy change ∼4.7 J/kg K larger than that of Gd has been observed at 224 K under a magnetic field of 1.5 T in comparatively big particles. This phenomenon of large magnetic entropy change indicates that the perovskite-type manganese oxides have ...
J R Zhang, Du Y W
exaly +2 more sources
The magnetic phase transition and magnetic entropy change (−ΔSM) in the La0.40Nd0.30Sr0.30Mn0.70Cr0.30O3 perovskite were investigated by measuring the magnetization as a function of temperature. The ferromagnetic transition temperature TC and the critical exponents β and γ, determined by analyzing the Arrott plots, are found to be TC = 191 K, β = 0.433,
Kallel, Sami +3 more
openaire +3 more sources
Magnetic entropy change and magnetoresistance in the LaFe11.375Al1.625 compound
Large magnetic entropy change |ΔS| with a nearly temperature-independent magnitude over a wide temperature range (about 70 K span from ∼140 K to 210 K) was observed in an Fe-based NaZn13-type compound LaFe11.375Al1.625. Such a behavior of magnetic entropy change is ascribed to two closely spaced magnetic transitions. One at 181 K (TN) with second-order
Hu, FX +9 more
openaire +3 more sources

