22–27 Jul 2012
Embassy Suites Napa Valley
US/Pacific timezone

Orbital fluctuations and orbital order below the Jahn-Teller transition in Sr3Cr2O8

23 Jul 2012, 20:00
2h
Fountain Court (Embassy Suites Napa Valley)

Fountain Court

Embassy Suites Napa Valley

1075 California Boulevard, Napa, California, United States 94559
Board: 33
Student Poster Competition Spin Phenomena Poster Session 1

Speaker

Zhe Wang (EP 5, EKM, Institute for Physics, Augsburg University, Augsburg, Germany)

Description

Zhe Wang, Joachim Deisenhofer, Michael Schmidt, Franz Mayr, Hans-Abrecht Krug von Nidda, and Alois Loidl Experimental Physics V, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86135 Augsburg, Germany Yuan Wan Department of Physics and Astronomy, Johns Hopkins University, Baltimore, Maryland 21218, USA Diana Lucia Quintero-Castro, A. T. M. Nazmul Islam, and Bella Lake Helmholtz-Zentrum Berlin für Materialien und Energie, D-14109 Berlin, Germany We report on the magnetic-, phononic-, and crystal-field-excitation spectrum of a spin-gapped system Sr3Cr2O8 determined by Terahertz and infrared (IR) spectroscopy across the Jahn-Teller (JT) transition at T_JT = 285 K. We identify the spin singlet-triplet excitations in the dimerized ground state and reveal the corresponding selection rules, which rely on an inter-dimer Dzyaloschinskii-Moriya (DM) interaction with DM vector parallel with crystalline a-axis. The temperature-dependent feature of magnetic and phononic excitations supports the existence of strong orbital fluctuation in an extended temperature regime T* < T < T_JT with T* ~120K, in agreement with the results from Raman spectroscopy and electron spin resonance (ESR) measurements.[1,2] The strong fluctuation regime results from the competition between spin-orbital interaction and JT interaction, since, in contrary to the effect of JT distortion, spin-orbital interaction stabilizes the chromium orbital of d_{x^2-y^2} with respect to d_{z^2}. The excitation corresponding to the split of the orbitals due to spin-orbital interaction is observed from T>T_JT down to T*, whose energy is around 3 meV consistent with the estimation based on the results of ESR and crystal-field-excitation spectrum. Below T*, JT interaction is dominant that the ordering of lower-lying d_{z^2} orbital is achieved. [1] Zhe Wang et al., Phys. Rev. B 83 201102 (2011) [2] D. Wulferding et al., Phys. Rev. B 84, 064419 (2011)

Primary author

Zhe Wang (EP 5, EKM, Institute for Physics, Augsburg University, Augsburg, Germany)

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