“…The COO phase in Pr 0.6 Ca 0.4 MnO 3 is evidenced by a sudden decrease in the magnetic susceptibility, an increase in the resistivity at T COO > T N [23,24] and by the appearance of superstructure Bragg reflections which indicate a doubling of the unit cell. These reflections also disappear when the magnetic field drives the compound into the metallic state [14].…”
Section: Materials and Experimental Methodsmentioning
We report a resonant x-ray diffraction study of the magnetoresistant perovskite Pr0.6Ca0.4MnO3. We discuss the spectra measured above and below the semiconductor-insulator transition temperature with aid of a detailed formal analysis of the energy and polarization dependences of the structure factors and ab initio calculations of the spectra. In the low temperature insulating phase, we find that inequivalent Mn atoms order in a CE-type pattern and that the crystallographic structure of La0.5Ca0.5MnO3, (Radaelli et al., Phys. Rev. B 55, 3015 (1997)) can also describe this system in fine details. Instead, the alternative structure proposed for the so-called Zener polaron model (Daoud-Aladine et al., Phys. Rev. Lett. 89, 097205 (2002)) is ruled out by crystallographic and spectroscopic evidences. Our analysis supports a model involving orbital ordering. However, we confirm that there is no direct evidence of charge disproportionation in the Mn K-edge resonant spectra. Therefore, we consider a CE-type model in which there are two Mn sublattices, each with partial eg occupancy. One sublattice consists of Mn atoms with the 3x 2 − r 2 or 3y 2 − r 2 orbitals partially occupied in a alternating pattern, the other sublattice with the x 2 − y 2 orbital partially occupied.
“…The COO phase in Pr 0.6 Ca 0.4 MnO 3 is evidenced by a sudden decrease in the magnetic susceptibility, an increase in the resistivity at T COO > T N [23,24] and by the appearance of superstructure Bragg reflections which indicate a doubling of the unit cell. These reflections also disappear when the magnetic field drives the compound into the metallic state [14].…”
Section: Materials and Experimental Methodsmentioning
We report a resonant x-ray diffraction study of the magnetoresistant perovskite Pr0.6Ca0.4MnO3. We discuss the spectra measured above and below the semiconductor-insulator transition temperature with aid of a detailed formal analysis of the energy and polarization dependences of the structure factors and ab initio calculations of the spectra. In the low temperature insulating phase, we find that inequivalent Mn atoms order in a CE-type pattern and that the crystallographic structure of La0.5Ca0.5MnO3, (Radaelli et al., Phys. Rev. B 55, 3015 (1997)) can also describe this system in fine details. Instead, the alternative structure proposed for the so-called Zener polaron model (Daoud-Aladine et al., Phys. Rev. Lett. 89, 097205 (2002)) is ruled out by crystallographic and spectroscopic evidences. Our analysis supports a model involving orbital ordering. However, we confirm that there is no direct evidence of charge disproportionation in the Mn K-edge resonant spectra. Therefore, we consider a CE-type model in which there are two Mn sublattices, each with partial eg occupancy. One sublattice consists of Mn atoms with the 3x 2 − r 2 or 3y 2 − r 2 orbitals partially occupied in a alternating pattern, the other sublattice with the x 2 − y 2 orbital partially occupied.
“…[2][3][15][16][17][18] In the pump-probe spectroscopy studies, Pr 0. to the formation of a pseudo plasma edge in the metallic state. 12 Our observation of the ultrafast formation of a metallic-like reflectivity spectrum following 17 m pump excitation provides the first evidence that the metallic state is formed promptly (within the 300 fs experimental resolution) via direct vibrational excitation, 20 and that this state persists for 100's of picoseconds. Magneto-optic Kerr effect measurements following mid-infrared excitation will be important in the future to establish whether this insulator-to-metal transition is synonymous with an antiferromagnetic-to-ferromagnetic phase transformation, as would be expected for a magnetoresistive manganite where metallicity is associated with ferromagnetism through a double-exchange mechanism.…”
mentioning
confidence: 94%
“…Figure 1(b) shows the low-temperature optical conductivity spectrum of Pr 0.7 Ca 0.3 MnO 3 with three dominant phonon modes (23,42, and 71 meV) 12 corresponding to the three (F 2u ) infrared active vibrational modes of a cubic perovskite. 13 The two highest frequency vibrations are assigned to the Mn-O-Mn bending mode and the Mn-O stretching mode respectively.…”
“…Such a behavior is very sensitive to stoichiometry. In P r 0.6 Ca 0.4 MnO 3 [9], [11], as well as in Nd 0.6 Ca 0.4 MnO 3 [12], the anomaly at T CO persists while the signature of T N is quite visible. What is the exact nature of the phase when T N < T < T CO ?…”
In the manganite N d 0.5 Ca 0.5 M nO 3 , charge ordering occurs at much higher temperature than the antiferromagnetic order (T CO = 250K, T N = 160K).the magnetic behavior of the phase T N < T < T CO is puzzling: its magnetization and susceptibility are typical of an antiferromagnet while no magnetic order is detected by neutron diffraction.We have undertaken an extensive study
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