2004
DOI: 10.1016/j.physb.2004.04.034
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Crystallographic phases in La2/3Ba1/3MnO3: temperature transformations and relation to magnetism

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Cited by 6 publications
(10 citation statements)
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“…The susceptibility hysteresis loop is asymmetric: its high temperature extent ($140 K) is much greater than the low temperature one ($20 K). This is in accordance with the neutron diffraction data [5,6] and is attributed to the high temperature of the reverse martensitic transformation that finishes at $370 K when heating (strictly speaking the A f temperature for the present samples can be slightly different from 370 K because of certain difference between their oxygen content and that of the samples have been studied in [5,6]; see next section). 3.…”
Section: Thermal Hysteresissupporting
confidence: 90%
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“…The susceptibility hysteresis loop is asymmetric: its high temperature extent ($140 K) is much greater than the low temperature one ($20 K). This is in accordance with the neutron diffraction data [5,6] and is attributed to the high temperature of the reverse martensitic transformation that finishes at $370 K when heating (strictly speaking the A f temperature for the present samples can be slightly different from 370 K because of certain difference between their oxygen content and that of the samples have been studied in [5,6]; see next section). 3.…”
Section: Thermal Hysteresissupporting
confidence: 90%
“…[5,6] below the room temperature crystal structure of La 2/3 Ba 1/3 MnO 3 manganite represents a mixture of the high temperature rhombohedral R3c phase (austenite) and the low temperature orthorhombic phase Imma (martensite) as a result of martensitic phase transformation. It occurs over a wide range of temperatures [5,6] that is typical for transformations of such type [7,30]. Note, that on cooling, a martensitic transformation starts at the martensite start temperature M s , and finishes at the martensite finish temperature M f .…”
Section: Thermal Hysteresismentioning
confidence: 99%
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“…The first-order structural transformations in manganites which are not associated with charge-ordering are still not enough understood, although experiments on La 1 À x Sr x MnO 3 [19][20][21][22] and La 1 À x Ba x MnO 3 (x¼0.2, 0.33) [16,[23][24][25][26] many interesting peculiarities of their behavior associated with the MT, such as the dependence of the transformation temperature T s on magnetic field and hydrostatic pressure, a wide temperature range of the phases coexistence and nonequilibrium thermodynamics.…”
Section: Introductionmentioning
confidence: 99%