3,116 research outputs found
Nonequilibrium electron spectroscopy of Luttinger liquids
Understanding the effects of nonequilibrium on strongly interacting quantum
systems is a challenging problem in condensed matter physics. In dimensions
greater than one, interacting electrons can often be understood within
Fermi-liquid theory where low-energy excitations are weakly interacting
quasiparticles. On the contrary, electrons in one dimension are known to form a
strongly-correlated phase of matter called a Luttinger liquid (LL), whose
low-energy excitations are collective density waves, or plasmons, of the
electron gas. Here we show that spectroscopy of locally injected high-energy
electrons can be used to probe energy relaxation in the presence of such strong
correlations. For detection energies near the injection energy, the electron
distribution is described by a power law whose exponent depends in a continuous
way on the Luttinger parameter, and energy relaxation can be attributed to
plasmon emission. For a chiral LL as realized at the edge of a fractional
quantum Hall state, the distribution function grows linearly with the distance
to the injection energy, independent of filling fraction.Comment: 4+ pages, 3 figure
X-ray Development of the Classical Nova V2672 Ophiuchi with Suzaku
We report the Suzaku detection of a rapid flare-like X-ray flux amplification
early in the development of the classical nova V2672 Ophiuchi. Two
target-of-opportunity ~25 ks X-ray observations were made 12 and 22 days after
the outburst. The flux amplification was found in the latter half of day 12.
Time-sliced spectra are characterized by a growing supersoft excess with
edge-like structures and a relatively stable optically-thin thermal component
with Ka emission lines from highly ionized Si. The observed spectral evolution
is consistent with a model that has a time development of circumstellar
absorption, for which we obtain the decline rate of ~10-40 % in a time scale of
0.2 d on day 12. Such a rapid drop of absorption and short-term flux
variability on day 12 suggest inhomogeneous ejecta with dense blobs/holes in
the line of sight. Then on day 22 the fluxes of both supersoft and thin-thermal
plasma components become significantly fainter. Based on the serendipitous
results we discuss the nature of this source in the context of both short- and
long-term X-ray behavior.Comment: To appear in PASJ; 9 pages, 5 figures, 2 table
Magmatic focusing to mid-ocean ridges: the role of grain size variability and non-Newtonian viscosity
Melting beneath mid-ocean ridges occurs over a region that is much broader
than the zone of magmatic emplacement to form the oceanic crust. Magma is
focused into this zone by lateral transport. This focusing has typically been
explained by dynamic pressure gradients associated with corner flow, or by a
sub-lithospheric channel sloping upward toward the ridge axis. Here we discuss
a novel mechanism for magmatic focusing: lateral transport driven by gradients
in compaction pressure within the asthenosphere. These gradients arise from the
co-variation of melting rate and compaction viscosity. The compaction
viscosity, in previous models, was given as a function of melt fraction and
temperature. In contrast, we show that the viscosity variations relevant to
melt focusing arise from grain-size variability and non-Newtonian creep. The
asthenospheric distribution of melt fraction predicted by our models provides
an improved ex- planation of the electrical resistivity structure beneath one
location on the East Pacific Rise. More generally, although grain size and
non-Newtonian viscosity are properties of the solid phase, we find that in the
context of mid-ocean ridges, their effect on melt transport is more profound
than their effect on the mantle corner-flow.Comment: 20 pages, 4 figures, 1 tabl
Time domain Einstein-Podolsky-Rosen correlation
We experimentally demonstrate creation and characterization of
Einstein-Podolsky-Rosen (EPR) correlation between optical beams in the time
domain. The correlated beams are created with two independent continuous-wave
optical parametric oscillators and a half beam splitter. We define temporal
modes using a square temporal filter with duration and make time-resolved
measurement on the generated state. We observe the correlations between the
relevant conjugate variables in time domain which correspond to the EPR
correlation. Our scheme is extendable to continuous variable quantum
teleportation of a non-Gaussian state defined in the time domain such as a
Schr\"odinger cat-like state.Comment: 4 pages, 4 figure
Virtual turning points and bifurcation of Stokes curves for higher order ordinary differential equations
For a higher order linear ordinary differential operator P, its Stokes curve
bifurcates in general when it hits another turning point of P. This phenomenon
is most neatly understandable by taking into account Stokes curves emanating
from virtual turning points, together with those from ordinary turning points.
This understanding of the bifurcation of a Stokes curve plays an important role
in resolving a paradox recently found in the Noumi-Yamada system, a system of
linear differential equations associated with the fourth Painleve equation.Comment: 7 pages, 4 figure
Evolution of the single-hole spectral function across a quantum phase transition in the anisotropic-triangular-lattice antiferromagnet
We study the evolution of the single-hole spectral function when the ground
state of the anisotropic-triangular-lattice antiferromagnet changes from the
incommensurate magnetically-ordered phase to the spin-liquid state. In order to
describe both of the ground states on equal footing, we use the large-N
approach where the transition between these two phases can be obtained by
controlling the quantum fluctuations via an 'effective' spin magnitude. Adding
a hole into these ground states is described by a t-J type model in the
slave-fermion representation. Implications of our results to possible future
ARPES experiments on insulating frustrated magnets, especially CsCuCl,
are discussed.Comment: 8 pages, 7 figure
Nonequilibrium quantum criticality in bilayer itinerant ferromagnets
We present a theory of nonequilibrium quantum criticality in a coupled
bilayer system of itinerant electron magnets. The model studied consists of the
first layer subjected to an inplane current and open to an external substrate.
The second layer is closed and subject to no direct external drive, but couples
to the first layer via short-ranged spin exchange interaction. No particle
exchange is assumed between the layers. Starting from a microscopic fermionic
model, we derive an effective action in terms of two coupled bosonic fields
which are related to the magnetization fluctuations of the two layers. When
there is no interlayer coupling, the two bosonic modes possess different
dynamical critical exponents z with z=2 (z=3) for the first (second) layer.
This results in multi-scale quantum criticality in the coupled system. It is
shown that the linear coupling between the two fields leads to a low energy
fixed point characterized by the larger dynamical critical exponent z=3. The
perturbative renormalization group is used to compute the correlation length in
the quantum disordered and quantum critical regimes. We also derive the
stochastic dynamics obeyed by the critical fluctuations in the quantum critical
regime. Comparing the nonequilibrium situation to the thermal equilibrium
scenario, where the whole system is at a temperature T, we find that the
nonequilibrium drive does not always play the role of temperature.Comment: 20+ pages, 3 figures; Revised version as accepted by PRB, added
figure of mean field phase diagra
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