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

α-(BEDT-TTF)2I3: Complex electrodynamic response of the charge-ordered phase

23 Jul 2012, 14:45
12m
Chardonnay Ballroom (Embassy Suites Napa Valley)

Chardonnay Ballroom

Embassy Suites Napa Valley

1075 California Boulevard, Napa, California, United States 94559
Rapid Correlated Physics Correlated Physics

Speaker

Tomislav Ivek (Institut za fiziku)

Description

Tomislav Ivek [1], Ivan Kovačević [1], Marko Pinterić [1,2], Bojana Korin-Hamzić [1], Silvia Tomić [1], Conrad Clauss [3], Martin Dressel [3], Dieter Schweitzer [4] [1] Institut za fiziku, P.O.Box 304, HR-10001 Zagreb, Croatia [2] Faculty of Civil Engineering, Smetanova 17, 2000 Maribor, Slovenia [3] 1. Physikalisches Institut, Universität Stuttgart, Pfaffenwaldring 57, D-70550 Stuttgart, Germany [4] 3. Physikalisches Institut, Universität Stuttgart, Pfaffenwaldring 57, D-70550 Stuttgart, Germany Much experimental and theoretical attention has been attracted by organic systems with reduced dimensionality and strong Coulomb interactions, and deservedly so due to their novel broken-symmetry phases and corresponding excitations. Here we take a detailed look at the electrodynamics of one of the most prominent charge-ordered systems, the quasi-2D conductor α-(BEDT-TTF)2I3. A semimetal at high temperatures, at 136 K this particular system transitions into an insulating, diamagnetic ground state. Within the insulating phase a long-range commensurate ordering appears in the BEDT-TTF molecular planes, the so-called "horizontal stripe" charge order. [1,2,3] We characterize the charge response of the low-temperature phase using dc resistivity, dielectric and optical spectroscopy in different crystallographic directions within the BEDT-TTF layer. [4,5] Interestingly, two dielectric relaxation modes appear in the kHz-MHz range. The large mode features an anisotropic phason-like behavior, while the small mode presents a soliton-like characteristic. The observed type of excitations agrees with the most relevant physical picture of this charge order as a cooperative bond-charge density wave with ferroelectric-like features. [6] On the other hand, puzzling phenomena including negative differential resistance and voltage oscillations have been reported under application of high electric fields. [7] Our carefully designed electric-field-dependent measurements of conductivity anisotropy within the molecular plane qualitatively confirm these findings; additionally, they reveal novel intriguing behaviors. [8]. [1] Y. Takano et al., J. Phys. Chem. Solids 62, 393 (2001). [2] Organic Conductors, Special Topics Section, J. Phys. Soc. Jpn. 75, No. 5, (2006). [3] T. Kakiuchi et al., J. Phys. Soc. Jpn. 76, 113702 (2007). [4] T. Ivek et al., Phys. Rev. Lett. 104, 206406 (2010) [5] T. Ivek et al., Phys. Rev. B 83, 165128, (2011). [6] R. T. Clay et al., J. Phys. Soc. Jpn. 71, 1816 (2002). [7] K.Tamura et al., J. Appl.Phys.107, 103716(1-5), (2010). [8] T. Ivek et al., to be submitted (2012).

Primary author

Tomislav Ivek (Institut za fiziku)

Presentation materials

There are no materials yet.