2011
DOI: 10.1007/s00339-011-6284-5
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Anomalous phase separation in La0.225Pr0.4Ca0.375MnO3: consequence of temperature and magnetic-field cycles

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Cited by 8 publications
(9 citation statements)
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“…As shown in Figures (a) and (b), in the as‐grown samples, the conducting FMM domains with different sizes distribute randomly within the COI matrix without any preferred orientation. The simulation shows that the electric potential and current density vary inhomogeneous in the sample, and the current follow the paths with the least COI phase, which is in line with the percolation transport in phase‐separated manganites . As expected, the current has no preferred orientation, or in other words, the transport is isotropic.…”
Section: Resultssupporting
confidence: 78%
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“…As shown in Figures (a) and (b), in the as‐grown samples, the conducting FMM domains with different sizes distribute randomly within the COI matrix without any preferred orientation. The simulation shows that the electric potential and current density vary inhomogeneous in the sample, and the current follow the paths with the least COI phase, which is in line with the percolation transport in phase‐separated manganites . As expected, the current has no preferred orientation, or in other words, the transport is isotropic.…”
Section: Resultssupporting
confidence: 78%
“…Both ferromagnetic metallic (FMM) and charge‐ordered insulator (COI) phases with vastly different resistive and magnetic characters exist and compete with each other in some mixed‐valence manganites, which is believed to be the key ingredient in the well‐known colossal magnetoresistance (CMR) effect, one of the most fascinating phenomena in condensed matter physics . Because of the energetic degeneracy of ground states, the electronic phase separation (EPS) in manganite can be modulated to a large degree by factors like temperature, magnetic field, substrate strain, and so on, leading to rich phenomena . For example, an earlier report of La 0.7 Ca 0.15 Sr 0.15 MnO 3 thin films grown on ferroelectric single‐crystal substrates demonstrated that an in‐plane tensile strain induced by the ferroelectric poling leads to a weakening of the electron‐lattice coupling and thus a decrease (increase) in resistance (ferromagnetism) .…”
Section: Introductionmentioning
confidence: 99%
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“…Depending upon the thermal and magnetic history, LCMO exhibits a competition between FM and antiferromagnetic (AFM) states [6,10] in both tetragonal as well as orthorhombic structures [11,12] with growth of nano phase regions below T C [1]. LCMO is reported to exhibit change in crystal symmetry (T C = 225 K) along with a transition from paramagnetic (PM) to ferromagnetic metal (FMM) and then further to a charge exchange type antiferromagnetic insulating (CE-AFI) phase below T N = 155 K [6,12].…”
Section: Introductionmentioning
confidence: 99%
“…The magnetic and electronic properties vary greatly with different thermal or magnetic field cycling. 38 To directly examine the evolution of various EPS states with the magnetic field, magnetoresistance (MR), (H), has been measured at several temperatures for S2 and S3 along the two in-plane directions. Fig.…”
Section: B Static Anisotropic Transport: Magnetic Field Dependencementioning
confidence: 99%