320 research outputs found
NMR relaxation in the spin-1 Heisenberg chain
We consider the isotropic Heisenberg chain with a finite Haldane gap
and use state-of-the-art numerical techniques to investigate its
dynamical properties at finite temperature, focusing on the nuclear
spin-lattice relaxation rate measured in nuclear magnetic resonance
(NMR) experiments for instance. In particular, we analyze the contributions
from modes with momenta close to and as a function
of temperature. At high-temperature, we observe spin diffusion with a
non-trivial exponent. At low-temperature, we argue that a simple activated
behavior can only be observed at temperatures
much smaller than the gap .Comment: published versio
Microwave-stimulated Raman adiabatic passage in a Bose-Einstein condensate on an atom chip
We report the achievement of stimulated Raman adiabatic passage (STIRAP) in
the microwave frequency range between internal states of a Bose-Einstein
condensate (BEC) magnetically trapped in the vicinity of an atom chip. The
STIRAP protocol used in this experiment is robust to external perturbations as
it is an adiabatic transfer, and power-efficient as it involves only resonant
(or quasi-resonant) processes. Taking into account the effect of losses and
collisions in a non-linear Bloch equations model, we show that the maximum
transfer efficiency is obtained for non-zero values of the one- and two-photon
detunings, which is confirmed quantitatively by our experimental measurements
Disorder-Induced Revival of the Bose-Einstein Condensation in Ni(Cl_{1-x}Br_{x})_{2}-4SC(NH_{2})_{2} at High Magnetic Fields.
Building on recent NMR experiments [A. Orlova et al., Phys. Rev. Lett. 118, 067203 (2017).PRLTAO0031-900710.1103/PhysRevLett.118.067203], we theoretically investigate the high magnetic field regime of the disordered quasi-one-dimensional S=1 antiferromagnetic material Ni(Cl_{1-x}Br_{x})_{2}-4SC(NH_{2})_{2}. The interplay between disorder, chemically controlled by Br-doping, interactions, and the external magnetic field, leads to a very rich phase diagram. Beyond the well-known antiferromagnetically ordered regime, an analog of a Bose condensate of magnons, which disappears when Hâ„12.3ââT, we unveil a resurgence of phase coherence at a higher field HâŒ13.6ââT, induced by the doping. Interchain couplings stabilize the finite temperature long-range order whose extension in the field-temperature space is governed by the concentration of impurities x. Such a "minicondensation" contrasts with previously reported Bose-glass physics in the same regime and should be accessible to experiments
Dynamical properties of the random Heisenberg chain
We use numerical techniques to study dynamical properties at finite
temperature () of the Heisenberg spin chain with random exchange couplings,
which realizes the random singlet (RS) fixed point in the low-energy limit.
Specifically, we study the dynamic spin structure factor , which
can be probed directly by inelastic neutron scattering experiments and, in the
limit of small , in nuclear magnetic resonance (NMR) experiments
through the spin-lattice relaxation rate . Our work combines three
complementary methods: exact diagonalization, matrix-product-state algorithms,
and stochastic analytic continuation of quantum Monte Carlo results in
imaginary time. Unlike the uniform system, whose low-energy excitations at low
are restricted to close to and , our study reveals a
continuous narrow band of low-energy excitations in , extending
throughout the Brillouin zone. Close to , the scaling properties of
these excitations are well captured by the RS theory, but we also see
disagreements with some aspects of the predicted -dependence further away
from . Furthermore we find spin diffusion effects close to that
are not contained within the RS theory but give non-negligible contributions to
the mean . To compare with NMR experiments, we consider the distribution
of the local values, which is broad, approximately described by a
stretched exponential. The mean value first decreases with , but starts to
increase and diverge below a crossover temperature. Although a similar
divergent behavior has been found for the static uniform susceptibility, this
divergent behavior of has never been seen in experiments. Our results
show that the divergence of the mean is due to rare events in the
disordered chains and is concealed in experiments, where the typical
value is accessed.Comment: 19 pages, 14 figure
Fast Pyrolysis of Biomass Under Gasification Conditions: Influence of Particle Size, Reactor Temperature and Gas Phase Reactions
N/
Experimental study of the role of trap symmetry in an atom-chip interferometer above the Bose-Einstein condensation threshold
We report the experimental study of an atom-chip interferometer using
ultracold rubidium 87 atoms above the Bose-Einstein condensation threshold. The
observed dependence of the contrast decay time with temperature and with the
degree of symmetry of the traps during the interferometer sequence is in good
agreement with theoretical predictions published in [Dupont-Nivet et al., NJP
18, 113012 (2016)]. These results pave the way for precision measurements with
trapped thermal atoms.Comment: 11 pages, 4 figure
Near-Optimal Parameterization of the Intersection of Quadrics: III. Parameterizing Singular Intersections
In Part II [3] of this paper, we have shown, using a classification of pencils of quadrics over the reals, how to determine quickly and efficiently the real type of the intersection of two given quadrics. For each real type of intersection, we design, in this third part, an algorithm for computing a near-optimal parameterization. We also give here examples covering all the possible situations, in terms of both the real type of intersection and the number and depth of square roots appearing in the coefficients
Near-Optimal Parameterization of the Intersection of Quadrics: Theory and Implementation
Colloque avec actes et comité de lecture. internationale.International audienceWe present an algorithm that computes an exact parametric form of the intersection of two real quadrics in projective three-space given by implicit equations with rational coefficients. This algorithm represents the first complete and robust solution to what is perhaps the most basic problem of solid modeling by implicit curved surfaces
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