Disorder-induced short-range ferromagnetism and cluster spin-glass state in sol-gel derivedLa0.7Ca0.3Mn1−xCdxO3(0⩽x⩽0.2)

2006 ◽  
Vol 74 (10) ◽  
Author(s):  
Shilpi Karmakar ◽  
S. Taran ◽  
B. K. Chaudhuri ◽  
H. Sakata ◽  
C. P. Sun ◽  
...  
2019 ◽  
Vol 492 ◽  
pp. 165671 ◽  
Author(s):  
Shivani Sharma ◽  
Poonam Yadav ◽  
Tusita Sau ◽  
Premakumar Yanda ◽  
Peter J. Baker ◽  
...  

2017 ◽  
Vol 29 (40) ◽  
pp. 405806 ◽  
Author(s):  
W P Cai ◽  
Z R Yan ◽  
R M Liu ◽  
M H Qin ◽  
M Zeng ◽  
...  

2018 ◽  
Vol 749 ◽  
pp. 134-139 ◽  
Author(s):  
Y.J. Zhang ◽  
Q.Q. Zeng ◽  
Z.Y. Wei ◽  
Z.P. Hou ◽  
Z.H. Liu ◽  
...  

2009 ◽  
Vol 105 (7) ◽  
pp. 07A326 ◽  
Author(s):  
C. L. Lu ◽  
S. Dong ◽  
K. F. Wang ◽  
J.-M. Liu ◽  
Q. Wang ◽  
...  

2016 ◽  
Vol 418 ◽  
pp. 158-162 ◽  
Author(s):  
Sk. Mohammad Yasin ◽  
Ritwik Saha ◽  
V. Srinivas ◽  
S. Kasiviswanathan ◽  
A.K. Nigam

1983 ◽  
Vol 61 (12) ◽  
pp. 1599-1608 ◽  
Author(s):  
M. Crişan ◽  
Zs. Gulácsi ◽  
M. Gulácsi

The magnetic susceptibility of the spin-glass state that may appear in an itinerant-electron antiferromagnet containing magnetic impurities has been calculated as a function of the temperature. The spin–spin interaction mediated by the condensed electrons has been calculated and a short-range interaction of the form (cos 2k0r/r2)e−r/ξ0 has been obtained. A percolation mechanism has been used in order to explain the occurrence of the spin-glass state.


1984 ◽  
Vol 40 (3) ◽  
pp. 247-258 ◽  
Author(s):  
Zs. Gulácsi ◽  
M. Gulácsi ◽  
M. Crisan

2004 ◽  
Vol 443-444 ◽  
pp. 391-396 ◽  
Author(s):  
I.M. Siouris ◽  
I.P. Semitelou ◽  
J.K. Yakinthos ◽  
Wolfgang Schäfer

Evidence of the coexistence of an ordered antiferromagnetic and a spin glass state is given by studying a polycrystalline Tb2CuIn3 sample with neutron diffraction in a non-magnetic and a magnetic environment. Tb2CuIn3 is an antiferromagnet with competing exchange interactions (J1> 0 for nearest neighbours and J2 < 0 for next nearest neighbours) and an ordering temperature TN =33 ± 1 K. Powder diffraction measurements reveal a broad diffuse peak - due to short-range magnetic order - underneath the (100) long-range order magnetic Bragg reflection. The exposure of the sample in magnetic fields up to 7.5 T, under both zero field and field-cooled conditions, show that neither the long-range magnetic order nor the short-range order are destroyed by the outer magnetic fields. The almost field independent behaviour of the magnetic intensities is explained by the existence of a spin glass state. Support on the simultaneous presence of antiferromagnetic and spin glass states is given by recent ac-dc magnetic measurements. The infinite range model for spin glasses with strong uniaxial anisotropy has predicted this kind of magnetic behaviour.


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