Magnetic ordering in two ferromagnetic sublattices of two mixed-valence iron(II)-iron(III) metal formate frameworks

2019 ◽  
Vol 119 ◽  
pp. 110572 ◽  
Author(s):  
H. Yurtseven ◽  
E. Kilit Dogan
1978 ◽  
Vol 49 (3) ◽  
pp. 2101-2106 ◽  
Author(s):  
S. M. Shapiro ◽  
H. B. Mo/ller ◽  
J. D. Axe ◽  
R. J. Birgeneau ◽  
E. Bucher

1984 ◽  
Vol 55 (6) ◽  
pp. 1978-1980 ◽  
Author(s):  
J. Teter ◽  
J. E. Crow ◽  
T. Mihalisin

1999 ◽  
Vol 259-261 ◽  
pp. 349-350 ◽  
Author(s):  
H Aoki ◽  
A Ochiai ◽  
T Suzuki

2001 ◽  
Vol 64 (17) ◽  
Author(s):  
A. N. Vasil’ev ◽  
V. I. Marchenko ◽  
A. I. Smirnov ◽  
S. S. Sosin ◽  
H. Yamada ◽  
...  

2016 ◽  
Vol 4 (6) ◽  
pp. 1186-1193 ◽  
Author(s):  
Mirosław Mączka ◽  
Aneta Ciupa ◽  
Anna Gągor ◽  
Adam Sieradzki ◽  
Adam Pikul ◽  
...  

Mixed-valence iron(ii)–iron(iii) formate framework templated by diethylammonium cations exhibit structural and magnetic phase transitions near 240 and 39 K, respectively.


2002 ◽  
Vol 17 (12) ◽  
pp. 3090-3097
Author(s):  
Ranjan Kumar Sahu ◽  
Manju Lata Rao ◽  
Solomon Sundar Manoharan ◽  
Dieter Elefant ◽  
Peter Verges ◽  
...  

A novel magnetic pair-making interaction between Mn and Ru shows a strong correlation between the magnetic ordering and electronic transport, which was well exemplified in the investigation of bulk polycrystalline samples of La0.7Pb0.3Mn1⊟xRuxO3 and La0.6Pb0.4Mn1⊟xRuxO3, where 0.0 ≤ x ≤ 0.4. The metal-insulator transition (Tρ) complementing the Curie temperature (Tc) was observed up to 30% of Ru in La0.7Pb0.3Mn1⊟xRuxO3, and extended up to 40% of Ru in La0.6Pb0.4Mn1⊟xRuxO3, showing a unique double-exchange ferromagnetic exchange interaction between Mn and Ru ions. An upturn in resistance due to charge carrier localization at low temperatures (T<0.5 Tc) for more than 20% Ru doping was due to a dominant hole carrier density contribution rather than to grain boundary effects as inferred from the scanning electron microscopy and energy dispersive x-ray studies of the samples sintered at 1200 and 1400 °C. The charge localization effect of the eg electrons was removed by tuning the hole carrier density as demonstrated in the La0.6Pb0.4Mn1⊟xRuxO3 samples. Long range correlations between magnetism and transport in this series was attributed to the presence of mixed valence Ru(IV/V) and Mn(III)/(IV) pair, which shows a unique double exchange mediated interaction.


1983 ◽  
Vol 51 (1) ◽  
pp. 37-40 ◽  
Author(s):  
G. v. Eynatten ◽  
C. F. Wang ◽  
N. S. Dixon ◽  
L. S. Fritz ◽  
S. S. Hanna

2007 ◽  
Vol 62 (1) ◽  
pp. 5-14 ◽  
Author(s):  
Petra Jakubcová ◽  
Dirk Johrendt ◽  
Peter Sebastian ◽  
Sudhindra Rayaprol ◽  
Rainer Pöttgen

Eu5Sn3S12 and Eu4LuSn3S12 were synthesized and their structures refined from single crystal data (Pmc21, Eu5Sn3S12: a = 3.908(1), b = 20.115(4), c = 11.451(2) Å ; wR2 = 0.0519 for 3048 F2 and 122 parameters; Eu4LuSn3S12: a = 3.920(1), b = 20.132(4), c = 11.459(2) Å ; wR2 = 0.0737 for 3298 F2 and 122 parameters). The structures contain one-dimensional chains of edge-sharing SnS2S4/2 octahedra and corner-sharing SnS3S2/2 trigonal bipyramids, running parallel to [100]. Five europium sites are seven- or eightfold coordinated by sulfur atoms. Lutetium atoms in Eu4LuSn3S12 show a strong site preference for one of the two Eu3+ positions of Eu5Sn3S12 and no structural disorder was observed. Both compounds show static mixed valence according to Eu2+3 Eu3+2 Sn4+3 S2−12 and Eu2+3 Eu3+Lu3+Sn4+3 S2−12 , which was confirmed by temperature dependent magnetic susceptibility measurements. The experimental magnetic moments of 14.6(1) (Eu5Sn3S12) and 14.1(1) (Eu4LuSn3S12) μB/f.u. indicate that each of the two sulfides contains three divalent europium atoms per formula unit. Magnetic ordering for Eu5Sn3S12 and Eu4LuSn3S12 sets in below 5 and 3 K, respectively. Both sulfides show metamagnetic or spin-flip transitions in the magnetization curves at 3 K (2 K) with full saturation of the europium magnetic moments at 3 K (2 K) and 80 kOe. 151Eu Mössbauer spectra fully confirm the Eu2+ and Eu3+ site occupancies. At 4.2 K an increase in line width indicates small hyperfine fields at the europium nuclei.


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