95 research outputs found
The Efimovian three-body potential from broad to narrow Feshbach resonances
We analyse the change in the hyperradial Efimovian three-body potential as the two-body interaction is tuned from the broad to narrow Feshbach resonance regime. Here, it is known from both theory and experiment that the three-body dissociation scattering length a− shifts away from the universal value of −9.7 rvdW, with rvdW=12(mC6/ℏ2)1/4 the two-body van der Waals range. We model the three-body system using a separable two-body interaction that takes into account the full zero-energy behaviour of the multichannel wave function. We find that the short-range repulsive barrier in the three-body potential characteristic for single-channel models remains universal for narrow resonances, whilst the change in the three-body parameter originates from a strong decrease in the potential depth. From an analysis of the underlying spin structure we further attribute this behavior to the dominance of the two-body interaction in the resonant channel compared to other background interactions
Resonance triplet dynamics in the quenched unitary Bose gas
The quenched unitary Bose gas is a paradigmatic example of a strongly interacting out-of-equilibrium quantum system, whose dynamics become difficult to describe theoretically due to the growth of non-Gaussian quantum correlations. We develop a conserving many-body theory capable of capturing these effects, allowing us to model the postquench dynamics in the previously inaccessible time regime where the gas departs from the universal prethermal stage. Our results show that this departure is driven by the growth of strong lossless three-body correlations, rather than atomic losses, thus framing the heating of the gas in this regime as a fully coherent phenomenon. We uncover the specific few-body scattering processes that affect this heating and show that the expected connection between the two-body and three-body contacts and the tail of the momentum distribution is obscured following the prethermal stage, explaining the absence of this connection in experiments. Our general framework, which reframes the dynamics of unitary quantum systems in terms of explicit connections to microscopic physics, can be broadly applied to any quantum system containing strong few-body correlations.</p
Efimovian three-body potential from broad to narrow Feshbach resonances
We analyse the change in the hyperradial Efimovian three-body potential as
the two-body interaction is tuned from the broad to narrow Feshbach resonance
regime. Here, it is known from both theory and experiment that the three-body
dissociation scattering length shifts away from the universal value of
, with the two-body van der Waals range. We model the
three-body system using a separable two-body interaction that takes into
account the full zero-energy behaviour of the multichannel wave function. We
find that the short-range repulsive barrier in the three-body potential
characteristic for single-channel models remains universal for narrow
resonances, whilst the change in the three-body parameter originates from a
strong decrease in the potential depth. From an analysis of the underlying spin
structure we further attribute this behavior to the dominance of the two-body
interaction in the resonant channel compared to other background interactions.Comment: 12 pages, 11 figure
Resonance triplet dynamics in the quenched unitary Bose gas
The quenched unitary Bose gas is a paradigmatic example of a strongly
interacting out-of-equilibrium quantum system, whose dynamics become difficult
to describe theoretically due to the growth of non-Gaussian quantum
correlations. We develop a conserving many-body theory capable of capturing
these effects, allowing us to model the post-quench dynamics in previously
inaccessible time regimes. By comparing our results directly to experiment, we
answer long-standing fundamental questions regarding the heating and population
dynamics in the gas, specifically highlighting the dominance of strong lossless
correlations rather than incoherent atomic losses. Our general framework, which
reframes the dynamics of unitary quantum systems in terms of explicit
connections to microscopic physics, can be broadly applied to any quantum
system containing strong few-body correlations.Comment: 7 pages, 4 figure
Emergent inflation of the Efimov spectrum under three-body spin-exchange interactions
One of the most fascinating predictions of few-body quantum physics is the
Efimov effect, a universal accumulation of an infinite geometric series of
three-body bound states at a two-body scattering resonance. Ever since the
first experimental observation of such an Efimov state, the precise
characterization of their physical properties has continued to challenge
few-body theory. This is demonstrated most strongly by the lithium few-body
puzzle, a remarkable theoretical discrepancy with the observed Efimov spectrum
in . Here, we resolve this long-standing puzzle, demonstrating
that the discrepancy arises out of the presence of strong non-universal
three-body spin-exchange interactions. This conclusion is obtained from a
thorough numerical solution of the quantum mechanical three-body problem,
including precise interatomic interactions and all spin degrees of freedom for
three alkali-metal atoms. Our results show excellent agreement with the
experimental data regarding both the Efimov spectrum and the absolute rate
constants of three-body recombination, and in addition reveal a general product
propensity for such triatomic reactions in the Paschen-Back regime, stemming
from Wigner's spin conservation rule.Comment: 7+5 pages, 3+2 figure
Cumulant theory of the unitary Bose gas: Prethermal and Efimovian dynamics
We study the quench of a degenerate ultracold Bose gas to the unitary regime,
where interactions are as strong as allowed by quantum mechanics. We lay the
foundations of a cumulant theory able to capture simultaneously the three-body
Efimov effect and ergodic evolution. After an initial period of rapid quantum
depletion, a universal prethermal stage is established characterized by a
kinetic temperature and an emergent Bogoliubov dispersion law while the
microscopic degrees of freedom remain far-from-equilibrium. Integrability is
then broken by higher-order interaction terms in the many-body Hamiltonian,
leading to a momentum-dependent departure from power law to decaying
exponential behavior of the occupation numbers at large momentum. We find also
signatures of the Efimov effect in the many-body dynamics and make a precise
identification between the observed beating phenomenon and the binding energy
of an Efimov trimer. Throughout the work, our predictions for a uniform gas are
quantitatively compared with experimental results for quenched unitary Bose
gases in uniform potentials.Comment: 34 pages, 12 figure
Articulated Model Registration of MRI/X-Ray Spine Data
Collection : Lecture Notes in Computer Science ; vol. 6112This paper presents a method based on articulated models for the registration of spine data extracted from multimodal medical images of patients with scoliosis. With the ultimate aim being the development of a complete geometrical model of the torso of a scoliotic patient, this work presents a method for the registration of vertebral column data using 3D magnetic resonance images (MRI) acquired in prone position and X-ray data acquired in standing position for five patients with scoliosis. The 3D shape of the vertebrae is estimated from both image modalities for each patient, and an articulated model is used in order to calculate intervertebral transformations required in order to align the vertebrae between both postures. Euclidean distances between anatomical landmarks are calculated in order to assess multimodal registration error. Results show a decrease in the Euclidean distance using the proposed method compared to rigid registration and more physically realistic vertebrae deformations compared to thin-plate-spline (TPS) registration thus improving alignment.IRS
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