50 research outputs found
Electrical Control of Structural and Physical Properties via Strong Spin-Orbit Interactions in Sr\u3csub\u3e2\u3c/sub\u3eIrO\u3csub\u3e4\u3c/sub\u3e
Electrical control of structural and physical properties is a long-sought, but elusive goal of contemporary science and technology. We demonstrate that a combination of strong spin-orbit interactions (SOI) and a canted antiferromagnetic Mott state is sufficient to attain that goal. The antiferromagnetic insulator Sr2IrO4 provides a model system in which strong SOI lock canted Ir magnetic moments to IrO6 octahedra, causing them to rigidly rotate together. A novel coupling between an applied electrical current and the canting angle reduces the Néel temperature and drives a large, nonlinear lattice expansion that closely tracks the magnetization, increases the electron mobility, and precipitates a unique resistive switching effect. Our observations open new avenues for understanding fundamental physics driven by strong SOI in condensed matter, and provide a new paradigm for functional materials and devices
Electrical Control of Structural and Physical Properties via Strong Spin-Orbit Interactions in Sr2IrO4
Electrical control of structural and physical properties is a long-sought,
but elusive goal of contemporary science and technology. We demonstrate that a
combination of strong spin-orbit interactions (SOI) and a canted
antiferromagnetic (AFM) Mott state is sufficient to attain that goal. The AFM
insulator Sr2IrO4 provides a model system in which strong SOI lock canted Ir
magnetic moments to IrO6-octahedra, causing them to rigidly rotate together. A
novel coupling between an applied electrical current and the canting angle
reduces the N\'eel temperature and drives a large, non-linear lattice expansion
that closely tracks the magnetization, increases the electron mobility, and
precipitates a unique resistive switching effect. Our observations open new
avenues for understanding fundamental physics driven by strong SOI in condensed
matter, and provide a new paradigm for functional materials and devices.Comment: 5 figures; to be published in Physical Review Letter
Thermoelectric Figure of Merit of Strongly Correlated Superlattice Semiconductors
We solved the Anderson Lattice Hamiltonian to get the energy bands of a
strongly correlated semiconductor by using slave boson mean field theory. The
transport properties were calculated in the relaxation-time approximation,and
the thermoelectric figure of merit was obtained for the strongly correlated
semiconductor and its superlattice structures. We found that at room
temperature can reach nearly 2 for the quantum wire lattice structure.We
believe that it is possible to find high values of thermoelectric figure of
merit from strongly correlated semiconductor superlattice systems.Comment: 4 pages, 3 figure
X-boson cumulant approach to the periodic Anderson model
The Periodic Anderson Model (PAM) can be studied in the infinite U limit by
employing the Hubbard X operators to project out the unwanted states. We have
already studied this problem employing the cumulant expansion with the
hybridization as perturbation, but the probability conservation of the local
states (completeness) is not usually satisfied when partial expansions like the
Chain Approximation (CHA) are employed. Here we treat the problem by a
technique inspired in the mean field approximation of Coleman's slave-bosons
method, and we obtain a description that avoids the unwanted phase transition
that appears in the mean-field slave-boson method both when the chemical
potential is greater than the localized level Ef at low temperatures (T) and
for all parameters at intermediate T.Comment: Submited to Physical Review B 14 pages, 17 eps figures inserted in
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Floquet-Markov description of the parametrically driven, dissipative harmonic quantum oscillator
Using the parametrically driven harmonic oscillator as a working example, we
study two different Markovian approaches to the quantum dynamics of a
periodically driven system with dissipation. In the simpler approach, the
driving enters the master equation for the reduced density operator only in the
Hamiltonian term. An improved master equation is achieved by treating the
entire driven system within the Floquet formalism and coupling it to the
reservoir as a whole. The different ensuing evolution equations are compared in
various representations, particularly as Fokker-Planck equations for the Wigner
function. On all levels of approximation, these evolution equations retain the
periodicity of the driving, so that their solutions have Floquet form and
represent eigenfunctions of a non-unitary propagator over a single period of
the driving. We discuss asymptotic states in the long-time limit as well as the
conservative and the high-temperature limits. Numerical results obtained within
the different Markov approximations are compared with the exact path-integral
solution. The application of the improved Floquet-Markov scheme becomes
increasingly important when considering stronger driving and lower
temperatures.Comment: 29 pages, 7 figure
Fermi surface topology and hot spot distribution in the Kondo lattice system CeB
We present high-resolution angle-resolved photoemission spectroscopy studies
of trivalent CeB6 and divalent BaB6 rare-earth hexaborides. We find that the
Fermi surface electronic structure of CeB6 consists of large oval-shape pockets
around the X points of the Brillouin zone, while the states around the zone
centre 'Gamma' point are strongly renormalized. Our first-principles
calculations agree with data around the X points, but not at the 'Gamma'
points, indicating areas of strong renormalization located around 'Gamma'. The
Ce quasi-particle states participate in formation of hotspots at the Fermi
surface, while the incoherent f states hybridize and lead to the emergence of
dispersive features absent in non-f counterpart BaB6. These experimental and
theoretical results provide a new understanding of rare-earth hexaboride
materials.Comment: 21 pages, 9 figure