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024 7 _ |a 1089-7550
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024 7 _ |a 10.1063/1.3686137
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024 7 _ |a 2128/4973
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024 7 _ |a :/content/aip/journal/jap/111/5/10.1063/1.3686137
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037 _ _ |a FZJ-2013-00944
041 _ _ |a English
082 _ _ |a 530
100 1 _ |a Pradheesh, R.
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245 _ _ |a Observation of spin glass state in weakly ferromagnetic Sr2FeCoO6 double perovskite
260 _ _ |a Melville, NY
|c 2012
|b American Institute of Physics
336 7 _ |a Journal Article
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500 _ _ |a The authors acknowledge the Department of Science and Technology (DST), India for financial support for providing the facilities used in this study (Grant Nos. SR/FST/PSII-002/2007 and SR/NM/NAT-02/2005). P. R wishes to thank M. Angst and K. Balamurugan for fruitful discussions.
520 _ _ |a A spin glass state is observed in the double perovskite oxide Sr2FeCoO6 prepared through sol-gel technique. Initial structural studies using x rays reveal that the compound crystallizes in tetragonal I4/m structure with lattice parameters, a = 5.4609(2) angstrom and c = 7.7113(7) angstrom. The temperature dependent powder x ray diffraction data reveal no structural phase transition in the temperature range 10-300 K. However, the unit cell volume shows an anomaly coinciding with the magnetic transition temperature thereby suggesting a close connection between lattice and magnetism. Neutron diffraction studies and subsequent bond valence sums analysis show that in Sr2FeCoO6, the B site is randomly occupied by Fe and Co in the mixed valence states of Fe3+ /Fe4+ and Co3+/Co4+. The random occupancy and mixed valence sets the stage for inhomogeneous magnetic exchange interactions and in turn, for the spin glass state in this double perovskite, which is observed as an irreversibility in temperature dependent dc magnetization at T-f similar to 75 K. Dynamical scaling analysis of chi'(T) yields a critical temperature T-ct = 75.14(8) K and an exponent zv = 6.2(2) typical for spin glasses. The signature of presence of mixed magnetic interactions is obtained from the thermal hysteresis in magnetization of Sr2FeCoO6. Combining the neutron and magnetization results of Sr2FeCoO6, we deduce that Fe is in low spin state while Co is in both low spin and intermediate spin states. (C) 2012 American Institute of Physics. [doi:10.1063/1.3686137]
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700 1 _ |a Nair, Harikrishna
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700 1 _ |a Kumar, Naveen
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700 1 _ |a Sethupathi, K.
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773 _ _ |a 10.1063/1.3686137
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