2005
DOI: 10.1103/physrevb.71.224409
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Pressure effects on the magnetic and transport properties ofPr1xSrxMnO3crystals nea

Abstract: Effects of hydrostatic pressure up to 11 kbar on the magnetic and transport properties of Pr 1−x Sr x MnO 3 ͑PSMO͒ were investigated in single crystals with various doping level: x = 0.22, 0.24, 0.26, in a wide range of temperature. In similarity with other low doped manganites, PSMO exhibits a metal to insulator transition and magnetoresistance maxima at the same temperature T = T MI . It was found that the magnetic ordering temperature T C of the Mn spin sublattice and T MI increase linearly upon applying th… Show more

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Cited by 37 publications
(14 citation statements)
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“…Double exchange is more sensitive to the pressure than SE and therefore the pressure coefficients are significantly different: dT C / dP Ϸ 0.2-0.3 K / kbar and dT C / dP Ϸ 2 K/ kbar for x Ͻ x C and x Ͼ x C , respectively. 55 Since the pressure coefficient dT C / dP Ϸ 1.8-1.9 K / kbar is very close for our NPs ensembles to that of metallic La 1−x Ca x MnO 3 ͑x Ͼ x C ͒ bulk manganites it seems reasonable to assume that a dominant magnetic interaction in the NPs cores is the ferromagnetic DE. For all fine-particle systems, different interparticle interactions exist and play a decisive role in formation of collective states and determine magnetic behavior of NP ensembles.…”
Section: Discussionmentioning
confidence: 59%
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“…Double exchange is more sensitive to the pressure than SE and therefore the pressure coefficients are significantly different: dT C / dP Ϸ 0.2-0.3 K / kbar and dT C / dP Ϸ 2 K/ kbar for x Ͻ x C and x Ͼ x C , respectively. 55 Since the pressure coefficient dT C / dP Ϸ 1.8-1.9 K / kbar is very close for our NPs ensembles to that of metallic La 1−x Ca x MnO 3 ͑x Ͼ x C ͒ bulk manganites it seems reasonable to assume that a dominant magnetic interaction in the NPs cores is the ferromagnetic DE. For all fine-particle systems, different interparticle interactions exist and play a decisive role in formation of collective states and determine magnetic behavior of NP ensembles.…”
Section: Discussionmentioning
confidence: 59%
“…55 In the case of x Ͼ x C , FM double exchange ͑DE͒ interactions control the magnetic and transport properties, whereas at x Ͻ x C DE is partly replaced by superexchange ͑SE͒ FM interactions. Double exchange is more sensitive to the pressure than SE and therefore the pressure coefficients are significantly different: dT C / dP Ϸ 0.2-0.3 K / kbar and dT C / dP Ϸ 2 K/ kbar for x Ͻ x C and x Ͼ x C , respectively.…”
Section: Discussionmentioning
confidence: 99%
“…The parameter A = (1 − f c )/f c , with f c being the percolation threshold. The GEM theory has been demonstrated to describe well the transport properties of phase-separated manganites [88][89][90], Although the generally accepted three-dimensional value of f c is 0.16, Kim et al found that f c = 0.17 presents a better fit for La 5/8−x Pr x Ca 3/8 MnO 3 (LPCMO) single crystals, whereas even higher values in the range of 0.22-0.24 were found for manganite thin films [88,89,91]. This discrepancy was attributed to both the quasi-two-dimensional nature of the films and the difference of the assumed values of σ M and σ I from the actual ones [88].…”
Section: Electric Field Effect On the Phase Separationmentioning
confidence: 99%
“…It has been known for decades that measurements of the initial susceptibility yield important information on magnetic domain processes [18,19]. Accordingly, ACsusceptibility has been used as a probe to study magnetic inhomogeneities due to phase separation in manganite single crystals [20][21][22][23] and the influence of preparation conditions on the magnetic properties in manganite ceramics [24]. Moreover, it has been established that ACsusceptibility can be a powerful tool to study magnetic inhomogeneities in manganites films [25].…”
Section: Introductionmentioning
confidence: 99%