Low temperature magnetization measurements on heavy-electron Ce compounds

1995 ◽  
Vol 206-207 ◽  
pp. 249-251 ◽  
Author(s):  
T. Sakakibara ◽  
T. Tayama ◽  
H. Mitamura ◽  
K. Matsuhira ◽  
H. Amitsuka ◽  
...  
Cryogenics ◽  
1979 ◽  
Vol 19 (9) ◽  
pp. 543-546 ◽  
Author(s):  
A. Berton ◽  
J. Chaussy ◽  
B. Cornut ◽  
J. Odin ◽  
J. Paureau ◽  
...  

1995 ◽  
Vol 206-207 ◽  
pp. 304-306 ◽  
Author(s):  
A. Meyer ◽  
M.J. Besnus ◽  
P. Haen ◽  
J.P. Kappler ◽  
G. Mathis

2001 ◽  
Vol 86 (9) ◽  
pp. 957-964 ◽  
Author(s):  
Sigrid G. Eeckhout ◽  
Eddy de Grave ◽  
André Lougear ◽  
Michael Gerdan ◽  
Catherine A. McCammon ◽  
...  

2000 ◽  
Vol 15 (7) ◽  
pp. 1635-1641 ◽  
Author(s):  
K. E. Kuehn ◽  
D. Sriram ◽  
S. S. Bayya ◽  
J. J. Simmins ◽  
R. L. Snyder

The ferrite with composition Cu0.5Fe2.5O4 was heat treated in air and in reducing atmospheres to different temperatures within the solid solution region confirmed by dynamic high-temperautre x-ray characterization. The samples were quenched in oil and air, and lattice parameter, Curie temperature, and saturation magnetization measurements were completed. The magnetization measurements for these samples showed a maximum 4πMs of 0.7729 and 0.5426 T at 10 and 300 K, respectively. The cationic distribution based on the low-temperature 4πMs measurements is (Cu+0.24Fe3+0.76)A[Cu+0.26Fe3+1.74]BO4 → 4.9 µ B. X-ray-pure Cu0.5Fe2.5O4 samples were also synthesized by slow cooling from the formation temperature to 900 °C in a reducing atmosphere. A temperature–PO2 diagram for the stability of Cu0.5Fe2.5O4 under the conditions of the experiment was determined. Low-temperature 4πMs measurements did not indicate an increase in the Cu+ A site occupancy for the samples cooled to 900 °C in a reducing environment above those samples that were quenched from high temperature. Curie temperatures for all Cu0.5Fe2.5O4 samples ranged from 348 to 369 °C. Lithium additions (0.1 mol/unit formula) to copper ferrite Li0.1Cu0.4Fe2.5O4 decreased the room-temperature 4πMs values to 0.5234 T with a corresponding decrease in the 10 K measurements to 0.7047 T. From the low-temperature magnetization measurements, the distribution was (Cu+0.15Fe3+0.85)A[Cu+0.25Li+0.1Fe3+1.65]BO4 → 4.48 µ B.


1993 ◽  
Vol 07 (01n03) ◽  
pp. 14-17
Author(s):  
H. P. VAN DER MEULEN ◽  
J. J. M. FRANSE ◽  
A. DE VISSER

Specific-heat measurements on single-crystalline samples of U ( Pt 1− x Pd x )3 ( x = 0.00, 0.05 and 0.10) reveal anomalously large values for c/T at low temperatures. The data for UPt 3 have previously been analyzed by making use of the enhanced value of the low-temperature Grüneisen parameter. By this analysis, the heavy-electron contribution to the specific heat has been separated from the normal part that is largely due to the phonon term. Taking this latter term to be the same for all three compounds, the heavy-electron contribution has been evaluated for temperatures below 20 K. This contribution is compared with a spin-1/2 Kondo-type of specific heat. The resulting curves for the x = 0.00 and x = 0.10 alloys are very similar and mainly differ in the temperature at which the maximum is found. The effect of an applied magnetic field within the hexagonal plane, however, shifts the maximum to lower temperatures for x = 0.00 whereas for x = 0.10 a shift towards higher temperatures is found.


2004 ◽  
Vol 13 (12) ◽  
pp. 2130-2135 ◽  
Author(s):  
Jiang Li-Xia ◽  
Meng Ji-Bao ◽  
Xia Zhao-Yang ◽  
Chen Zhao-Jia ◽  
Luo Jian-Lin ◽  
...  

1975 ◽  
Vol 53 (2) ◽  
pp. 145-150 ◽  
Author(s):  
R. W. Cochrane ◽  
F. T. Hedgcock ◽  
J. P. Tidman ◽  
M. J. Zuckermann

Low temperature magnetization measurements in magnetic fields up to 55 kOe are reported for a series of PdRhNi alloys containing 1 to 7 at.% Rh and up to 1 at.% Ni. These data indicate a critical Ni concentration for ferromagnetism close to 2 at.%. Comparison of the field and concentration dependence of the susceptibility to the magnetoresistance data of Purwins et al. reveals that the coefficient of the T2 local spin fluctuation resistivity scales directly with the nickel susceptibility. Experimentally, the scaling parameter varies only slightly with Rh concentration, a result which extends to the binary PdNi alloys.


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