2017
DOI: 10.1016/j.jallcom.2017.03.331
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Magnetic properties, resistivity and magnetoresistance effects of double perovskite La2Co1−xFexMnO6

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Cited by 29 publications
(9 citation statements)
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“…With an increasing magnetic field, the bifurcation in the M(T) data is significantly reduced and shifts to lower temperature (figures 4(b) and (c)). ZFC magnetization, M ZFC (T) curves reveal a cusp at a temperature below T b , which is indicative of a magnetically frustrated spin-glass-like ground state in LFMO [16,27]. The cusp in M ZFC (T) gradually shifts from T p ∼ 90 K to 20 K as the field is increased from 100 Oe to 500 Oe.…”
Section: Resultsmentioning
confidence: 92%
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“…With an increasing magnetic field, the bifurcation in the M(T) data is significantly reduced and shifts to lower temperature (figures 4(b) and (c)). ZFC magnetization, M ZFC (T) curves reveal a cusp at a temperature below T b , which is indicative of a magnetically frustrated spin-glass-like ground state in LFMO [16,27]. The cusp in M ZFC (T) gradually shifts from T p ∼ 90 K to 20 K as the field is increased from 100 Oe to 500 Oe.…”
Section: Resultsmentioning
confidence: 92%
“…Two spin freezing processes were realized at ∼20 and 255 K [18], and ∼55 and 280 K [24] in LFMO without any long-range order. Although a downward deviation in the inverse susceptibility has been found in LFMO below the Curie-Weiss line [15,18,27], it was absent in many reports [10,16,17]. While Zhang et al indicated that behavior of reciprocal susceptibility is similar to that expected for Griffiths-like phase [15], Bhame et al suggested the mixture of ferromagnetic and superparamagnetic phases in the intermediate state [10].…”
Section: Introductionmentioning
confidence: 98%
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“…The positive values of the Weiss constants θ Weiss , obtained from the x ‐intercepts of the linear fits, indicate that the magnetic interactions in our samples are primarily ferromagnetic in nature. The effective paramagnetic moment, µ eff is related to C as μeff=3kBCNAμB2=2.827C where k B is the Boltzmann constant, µ B is Bohr magneton, and N A is the Avogadro's number.…”
Section: Resultsmentioning
confidence: 99%
“…In the temperature range from 10 to 40 K, the conductive mechanism is well fitted with the adiabatic small polaron hopping (SPH) model, which can be explained by the expression: ρ = ρ 0 T exp(E A /k B T). 49 When the temperature is above 40 K, the conductive mechanism is more consistent with the thermal activation (TA) model, which can be expressed by the formula: ρ = ρ 0 exp(E A /k B T), 50 where E A refers to the energy difference between the intermediate and initial states, and the E A values of SPH and TA models are 4.23 and 8.28 meV, respectively. k B is the Boltzmann constant, and ρ 0 is the pre-exponential factor.…”
Section: ■ Results and Discussionmentioning
confidence: 88%