Commensurate and incommensurate charge order in Fe$_2$OBO$_3$

ORAL

Abstract

Charge order CO in the form of a Wigner crystal had been proposed by Attfield {\em et al}. [Nature {\bf 396}, 655 (1998)] based on measurements, particularly M\"{o}ssbauer spectroscopy, on polycrystalline Fe$_2$OBO$_3$, but no superstructure due to the CO had been detected. We have grown the first single crystals of pure Fe$_2$OBO$_3$, and resistivity and thermal analysis indicate not one, but two transitions associated with CO. To elucidate the nature of these two transitions a synchrotron study was performed. At low $T$ a superstructure corresponding to a doubling of the $a$ axis was observed for the first time. The phase between the two phase transitions, in contrast, exhibits an incommensurate modulation with propagation vector ($\frac{1}{2}$,$0$,$\tau$), $\tau$ increasing with $T$ towards $\frac{1}{2}$. Resonances in the energy-dependence of the scattered intensity around the Fe $K$ edge suggest that the modulations in both phases are indeed associated with CO.

Authors

  • Manuel Angst

    Oak Ridge National Laboratory, Oak Ridge TN 37831, Oak Ridge National Laboratory

  • Raphael Hermann

    FZ Juelich, 52425 Juelich, Germany

  • J.-W. Kim

    Ames Laboratory, Ames IA 50011, Ames Laboratory, Dept. of Physics, Iowa State University, IA 50011

  • Peter Khalifah

    U Massachusetts, Amherst MA 01003

  • Brian Sales

    Oak Ridge National Laboratory, Oak Ridge TN 37831, Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee, Oak Ridge National Laboratory, Oak Ridge National Laboratory, Oak Ridge, TN 37831

  • David Mandrus

    Oak Ridge National Laboratory, Oak Ridge TN 37831, Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee, Oak Ridge National Laboratory, Oak Ridge National Lab., Materials Science and Technology Division, Oak Ridge, TN, Oak Ridge National Laboratory, Oak Ridge, TN 37831