Mott-Hubbard transition in V2O3 revisited

Karsten Held

Technische Universität Wien, Festkörperphysik, Wien, Austria

V2O3 is the prototype system for the Mott transition, one of the most fundamental phenomena of electronic correlation. Here, temperature, doping or pressure induce a metal to insulator transition (MIT) between a paramagnetic metal and a paramagnetic insulator. This or related MITs have a high technological potential, among others for intelligent windows and field effect transistors. As this MIT was well studied experimentally [1] and theoretically even by realistic local density approximation plus dynamical mean field theory calculations [2] before, it was a big surprise that our new experimental and theoretical results [3-5] put a new twist to the V2O3 story. First, a microscopic photoemission view revealed that the metallic state of slightly doped V2O3 is actually a percolation of metallic and insulating islands, where upon increasing temperature the metallic islands turn insulating at the MIT [3]. Second, the long-hold paradigm of the equivalence of doping and pressure for the MIT does not bear a closer experimental and theoretical inspection. While doping increases the crystal field splitting between a1g and egpi states, decreasing pressure reduces the bandwidth. That is, exactly the two opposite parameters which control the multi- orbital MIT are affected. Third, infrared conductivity showed the disappearance of quasiparticle excitations and the opening of a pseudogap with increasing temperature [5].

[1] D. B. McWhan et al., Phys. Rev. B 7, 1920 (1973).
[2] K. Held et al., Phys. Rev. Lett. 86 5345 (2001).
[3] S. Lupi et al., Nature Communications 1, 105 (2010).
[4] F. Rodolakis et al., Phys. Rev. Lett. 104, 047401 (2010).
[5] L. Baldassarre et al., Phys. Rev. B 77, 113107 (2008).

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