1
98 JAHN-TELLER PHONON ANOMALY AND PHASE INHOMOGENEITIES IN La 0.7 Ca 0.3 MnO 3 1 J. Zhang, 2 P. Dai, 3 J. A. Fernandez-Baca, E. W. Plummer, 4 Y. Tomioka, 5 and Y. Tokura 5,6 It is known that the richness of the novel prop- erties of colossal magnetoresistance (CMR) manga- nites originates from the strong interplay between the charge, lattice, orbital, and spin degrees of free- dom found in these systems. Although several mechanisms [involving double-exchange (DE), elec- tron-phonon interactions, and electron-electron cor- relations] have been proposed to explain the ob- served CMR effect in this class of materials, a clear understanding of its microscopic origin is still lack- ing. In particular, if dynamic Jahn-Teller (JT) dis- tortions of the MnO 6 octahedra are crucial to the metal-to-insulator transition (MIT) and the CMR effect, the lattice vibrations associated with such distortions (i.e., the so-called JT phonons) would be expected to exhibit unusual behavior across the MIT/magnetic transition temperature (T c ). The T- dependence of the optical phonons in La 1-x Ca x MnO 3 and in La 1 x Sr x MnO 3 has been studied with infrared reflectivity and optical conductivity, and the ob- served energy shifts across T c were attributed to a strong electron-phonon interaction. In this work, inelastic neutron scattering is used to demonstrate that the JT phonons in La 0.7 Ca 0.3 MnO 3 do indeed exhibit an abnormal behavior across the MIT/ T c . As in the other CMR manganites, the optimally doped La 0.7 Ca 0.3 MnO 3 exhibits a ferromagnetic (FM) to paramagnetic (PM) transition and a simultaneous MIT at T c 240 K. While its structure maintains the slightly distorted cubic perovskite (orthorhombic- pnma) symmetry, there are small incoherent dy- namic distortions across T c . In general, the electron- phonon coupling across T c should renormalize the phonon energies without drastically changing their intensities. This should be especially true for the high-energy optical phonons because the change in their population factors is negligible across T c . Sur- prisingly, it has been discovered that one of Mn-O stretching JT phonon modes shows anomalous damping with increasing temperature in the FM phase and vanishes around T c , in concurrence with FM ordering and metallicity of the system (Fig. 1). Such drastic T-dependent damping cannot be ex- plained with simple arguments based on the dy- namic JT distortions at individual J-T sites. It is ar- gued that this behavior may be directly related to decoherence effects because of the growing dynamic phase fluctuations of the short-range polaron or charge/orbital ordering associated with JT-distor- tion in the FM metallic phase matrix as T T c . Fig. 1. (a) Relative integrated intensities of the JT breathing phonon mode as a function of tempera- ture at the middle of the zone (Q = {3.7, 1, 1}) and the zone boundary (Q = {3.5, 1, 1}) along the [1,0,0] direction. (b) Schematic illustration of the evolu- tion of dynamic phase segregation with increasing temperature. ___________________ 1. Summary of paper: Phys. Rev. Lett. 86, 3823 (2001). 2. ORNL/UT joint faculty participant. 3. UT/ORNL Distinguished Scientist Pro- gram. 4. Joint Research Center for Atomic Technol- ogy (JRCAT), Tsukuba, Japan. 5. University of Tokyo, Tokyo, Japan. Relative Intensity Temperature (K) 0 0.4 0.8 0.6 1.0 0.2 q = 0.3 T C FMM PMI q = 0.5 0 50 100 150 200 250 300 350

JAHN-TELLER PHONON ANOMALY AND PHASE ...98 JAHN-TELLER PHONON ANOMALY AND PHASE INHOMOGENEITIES IN La 0.7 Ca 0.3 MnO 3 1 J. Zhang,2 P. Dai, 3 J. A. Fernandez-Baca, E. W. Plummer,4

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Page 1: JAHN-TELLER PHONON ANOMALY AND PHASE ...98 JAHN-TELLER PHONON ANOMALY AND PHASE INHOMOGENEITIES IN La 0.7 Ca 0.3 MnO 3 1 J. Zhang,2 P. Dai, 3 J. A. Fernandez-Baca, E. W. Plummer,4

98

JAHN-TELLER PHONON ANOMALY AND PHASEINHOMOGENEITIES IN La0.7Ca0.3MnO3

1

J. Zhang,2 P. Dai, 3 J. A. Fernandez-Baca, E. W. Plummer,4 Y. Tomioka,5 and Y. Tokura5,6

It is known that the richness of the novel prop-erties of colossal magnetoresistance (CMR) manga-nites originates from the strong interplay betweenthe charge, lattice, orbital, and spin degrees of free-dom found in these systems. Although severalmechanisms [involving double-exchange (DE), elec-tron-phonon interactions, and electron-electron cor-relations] have been proposed to explain the ob-served CMR effect in this class of materials, a clearunderstanding of its microscopic origin is still lack-ing. In particular, if dynamic Jahn-Teller (JT) dis-tortions of the MnO6 octahedra are crucial to themetal-to-insulator transition (MIT) and the CMReffect, the lattice vibrations associated with suchdistortions (i.e., the so-called JT phonons) would beexpected to exhibit unusual behavior across theMIT/magnetic transition temperature (Tc). The T-dependence of the optical phonons in La1-xCaxMnO3

and in La1 xSrxMnO3 has been studied with infraredreflectivity and optical conductivity, and the ob-served energy shifts across Tc were attributed to astrong electron-phonon interaction. In this work,inelastic neutron scattering is used to demonstratethat the JT phonons in La0.7Ca0.3MnO3 do indeedexhibit an abnormal behavior across the MIT/Tc. As in the other CMR manganites, the optimallydoped La0.7Ca0.3MnO3 exhibits a ferromagnetic (FM)to paramagnetic (PM) transition and a simultaneousMIT at Tc ≅ 240 K. While its structure maintains theslightly distorted cubic perovskite (orthorhombic-pnma) symmetry, there are small incoherent dy-namic distortions across Tc. In general, the electron-phonon coupling across Tc should renormalize thephonon energies without drastically changing theirintensities. This should be especially true for thehigh-energy optical phonons because the change intheir population factors is negligible across Tc. Sur-

prisingly, it has been discovered that one of Mn-Ostretching JT phonon modes shows anomalousdamping with increasing temperature in the FMphase and vanishes around Tc, in concurrence withFM ordering and metallicity of the system (Fig. 1).Such drastic T-dependent damping cannot be ex-plained with simple arguments based on the dy-namic JT distortions at individual J-T sites. It is ar-gued that this behavior may be directly related todecoherence effects because of the growing dynamic

phase fluctuations of the short-range polaron orcharge/orbital ordering associated with JT-distor-tion in the FM metallic phase matrix as T → Tc.

Fig. 1. (a) Relative integrated intensities of theJT breathing phonon mode as a function of tempera-ture at the middle of the zone (Q = {3.7, 1, 1}) andthe zone boundary (Q = {3.5, 1, 1}) along the [1,0,0]direction. (b) Schematic illustration of the evolu-tion of dynamic phase segregation with increasingtemperature.

___________________

1. Summary of paper: Phys. Rev. Lett. 86,3823 (2001).

2. ORNL/UT joint faculty participant.3. UT/ORNL Distinguished Scientist Pro-

gram.4. Joint Research Center for Atomic Technol-

ogy (JRCAT), Tsukuba, Japan.5. University of Tokyo, Tokyo, Japan.

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