96 research outputs found
Origin of the high Neel temperature in SrTcO3
We investigate the origin of the high Neel temperature recently found in Tc
perovskites. The electronic structure in the magnetic state of SrTcO3 and its
3d analogue SrMnO3 is calculated within a framework combining band-structure
and many-body methods. In agreement with experiment, the Neel temperature of
SrTcO3 is found to be four times larger than that of SrMnO3. We show that this
is because the Tc-compound lies on the verge of the itinerant-to-localized
transition, and also has a larger bandwidth, while the Mn-compound lies deeper
into the localized side. For SrTcO3 we predict that the Neel temperature
depends weakly on applied pressure, in clear violation of Bloch's rule,
signaling the complete breakdown of the localized picture.Comment: 4+ pages, 3 figures, published versio
Non-local self energies in pyrochlore iridates from ab-initio TRILEX calculations, and their relevance for the Weyl semimetal phase
Motivated by recent experiments and computational results on pyrochlore
iridates, we compare single-particle properties of Y2Ir2O7 obtained from
single-site dynamical mean-field calculations with results within the TRILEX
approximation, where the latter takes non-local correlations into account. Our
calculations are all based on ab-initio calculations within density-functional
theory, and take spin-orbit coupling into account. In order to make the
treatment within TRILEX feasible, we first define a single-band jeff = 1/2
model, by comparing its spectral features within DMFT to a three-band model
that includes both jeff = 1/2 and jeff = 3/2 orbitals. Our calculations show
consistently a paramagnetic metallic phase at small interaction values, and an
insulating antiferromagnetic phase at larger interaction values. The critical
interactions, however, differ between single-site and TRILEX calculations. The
antiferromagnetic phase shows the already predicted all-in/all-out magnetic
ordering. Different to the single-site results, the TRILEX calculation gives
also evidence for the Weyl-semimetal regime in the vicinity of the
metal-insulator transition
Topological insulator on honeycomb lattices and ribbons without inversion symmetry
We study the Kane-Mele-Hubbard model with an additional
inversion-symmetry-breaking term. Using the topological Hamiltonian approach,
we calculate the invariant of the system as function of
spin-orbit coupling, Hubbard interaction , and inversion-symmetry-breaking
on-site potential. The phase diagram calculated in that way shows that, on the
one hand, a large term of the latter kind destroys the topological non-trivial
state. On the other hand, however, this inversion-symmetry-breaking field can
enhance the topological state, since for moderate values the transition from
the non-trivial topological to the trivial Mott insulator is pushed to larger
values of interaction . This feature of an enhanced topological state is
also found on honeycomb ribbons. With inversion symmetry, the edge of the
zigzag ribbon is magnetic for any value of . This magnetic moment destroys
the gapless edge mode. Lifting inversion symmetry allows for a finite region in
interaction strength below which gapless edge modes exist.Comment: 9 pages, 9 figure
Quantum Fluctuations, Temperature and Detuning Effects in Solid-Light Systems
The superfluid to Mott insulator transition in cavity polariton arrays is
analyzed using the variational cluster approach, taking into account quantum
fluctuations exactly on finite length scales. Phase diagrams in one and two
dimensions exhibit important non-mean-field features. Single-particle
excitation spectra in the Mott phase are dominated by particle and hole bands
separated by a Mott gap. In contrast to Bose-Hubbard models, detuning allows
for changing the nature of the bosonic particles from quasi-localized excitons
to polaritons to weakly interacting photons. The Mott state with density one
exists up to temperatures , implying experimentally accessible
temperatures for realistic cavity couplings .Comment: 4 pages, 4 figures, to appear in Phys. Rev. Letter
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