2012
DOI: 10.1088/0953-8984/24/19/195901
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Collective phase-like mode and the role of lattice distortions atTNTCin RMn2O5(R= Pr, Sm, Gd, Tb, Bi)

Abstract: We report on electronic collective excitations in RMn 2 O 5 (R= Pr, Sm, Gd, Tb) showing condensation starting at and below ~T N~TC~4 0-50 K. Its origin is understood as partial delocalized e g electron orbitals in the Jahn-Teller distortion of the pyramids dimmer with strong hybridized Mn 3+ -O bonds. Our local probes, Raman, infrared, and X-ray absorption, back the conclusion by which there is no structural phase transition at T N~TC . Ferroelectricity is magnetically assisted by electron localization trig… Show more

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Cited by 3 publications
(4 citation statements)
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(139 reference statements)
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“…They may hint JT lattice distortion enhancements contributing to local structural modifications due to the magnetoelastic volume contraction at ~78 K. At this respect is worth noticing that in the context of orbital physics Saitoh et al [20] pointed that similar shoulder behavior, but from Mn-O stretching bond in LaMnO 3 , were bound to appear as due to a zone boundary phonon folded back to k≈0 in the orbital ordered state. This kind of mode, that was observed by us in RMn 2 O 5 [21] and reported anomalous in TbMn 2 O 5 [22], does not seem to have a direct counterpart in NdMnO 3 .…”
Section: I) Phonon Activitymentioning
confidence: 68%
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“…They may hint JT lattice distortion enhancements contributing to local structural modifications due to the magnetoelastic volume contraction at ~78 K. At this respect is worth noticing that in the context of orbital physics Saitoh et al [20] pointed that similar shoulder behavior, but from Mn-O stretching bond in LaMnO 3 , were bound to appear as due to a zone boundary phonon folded back to k≈0 in the orbital ordered state. This kind of mode, that was observed by us in RMn 2 O 5 [21] and reported anomalous in TbMn 2 O 5 [22], does not seem to have a direct counterpart in NdMnO 3 .…”
Section: I) Phonon Activitymentioning
confidence: 68%
“…A transmission (absorption) spectrum peaking at a transverse optical (TO) mode will yield, at higher frequencies than the TO, a featureless background missing most of the information on longitudinal (and collective) excitations [52] as we have found for temperatures above T N in NdMnO 3 (Fig. 6 a; also [21]). This is also supported by our preliminary results on hexagonal TmMnO 3 , which show the low frequency collective excitation and magnetoelectric couplings playing a main role.…”
Section: Ii) Thz Collective Mode and Soft Bandsmentioning
confidence: 83%
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“…The mode intensity increases with decreasing temperature in the low-temperature magnetic phase, where it can be suppressed by an external z-axis polarised magnetic field of an order of several Tesla [49]. In multiferroics of more complex mixed-valence manganites of RMn 2 O 5 (R=Pr,Sm,Gd,Tb) a strong featureless band around these frequencies in the infrared reflectivity spectra was associated with collective electronic excitations of partially delocalised e g electronic orbitals, participating in dynamical multiferroic coupling in the Jahn-Teller distortion of the pyramid dimer [50]. The transmission measurements detected this mode in TbMn 2 O 5 and YMn 2 O 5 at 9.6 cm −1 and 7.2 cm −1 , respectively [51].…”
Section: Discussionmentioning
confidence: 99%