116 research outputs found
Groundstates of SU(2)-Symmetric Confined Bose Gas: Trap for a Schr\"odinger Cat
Conservation of the total isotopic spin S of a two-component Bose gas-like
Rb-has a dramatic impact on the structure of the ground state. In the
case when S is much smaller than the total number of particles N, the
condensation of each of the two components occurs into two single-particle
modes. The quantum wavefunction of such a groundstate is a Schr\"odinger Cat-a
superposition of the phase separated classical condensates, the most "probable"
state in the superposition corresponding to the classical groundstate in the
sector of given N and S. After measurement of the spatial distribution of the
densities of the two components, the Cat collapses into one of the classical
condensate states.Comment: 5 RevTex pages, no figures; replaced with revised version, where the
discussion on stability against temporal white noise and losses is adde
Diagrammatic Monte Carlo for Correlated Fermions
We show that Monte Carlo sampling of the Feynman diagrammatic series (DiagMC)
can be used for tackling hard fermionic quantum many-body problems in the
thermodynamic limit by presenting accurate results for the repulsive Hubbard
model in the correlated Fermi liquid regime. Sampling Feynman's diagrammatic
series for the single-particle self-energy we can study moderate values of the
on-site repulsion () and temperatures down to . We
compare our results with high temperature series expansion and with single-site
and cluster dynamical mean-field theory.Comment: 4 pages, 5 figures, stylistic change
Fluctuating and dissipative dynamics of dark solitons in quasi-condensates
The fluctuating and dissipative dynamics of matter-wave dark solitons within
harmonically trapped, partially condensed Bose gases is studied both
numerically and analytically. A study of the stochastic Gross-Pitaevskii
equation, which correctly accounts for density and phase fluctuations at finite
temperatures, reveals dark soliton decay times to be lognormally distributed at
each temperature, thereby characterizing the previously predicted long lived
soliton trajectories within each ensemble of numerical realizations (S.P.
Cockburn {\it et al.}, Phys. Rev. Lett. 104, 174101 (2010)). Expectation values
for the average soliton lifetimes extracted from these distributions are found
to agree well with both numerical and analytic predictions based upon the
dissipative Gross-Pitaevskii model (with the same {\it ab initio} damping).
Probing the regime for which , we find average
soliton lifetimes to scale with temperature as , in agreement
with predictions previously made for the low-temperature regime .
The model is also shown to capture the experimentally-relevant decrease in the
visibility of an oscillating soliton due to the presence of background
fluctuations.Comment: 17 pages, 14 figure
The effect of light assisted collisions on matter wave coherence in superradiant Bose-Einstein condensates
We investigate experimentally the effects of light assisted collisions on the
coherence between momentum states in Bose-Einstein condensates. The onset of
superradiant Rayleigh scattering serves as a sensitive monitor for matter wave
coherence. A subtle interplay of binary and collective effects leads to a
profound asymmetry between the two sides of the atomic resonance and provides
far bigger coherence loss rates for a condensate bathed in blue detuned light
than previously estimated. We present a simplified quantitative model
containing the essential physics to explain our experimental data and point at
a new experimental route to study strongly coupled light matter systems.Comment: 10 pages, 4 figure
Observation of vortex dipoles in an oblate Bose-Einstein condensate
We report experimental observations and numerical simulations of the
formation, dynamics, and lifetimes of single and multiply charged quantized
vortex dipoles in highly oblate dilute-gas Bose-Einstein condensates (BECs). We
nucleate pairs of vortices of opposite charge (vortex dipoles) by forcing
superfluid flow around a repulsive gaussian obstacle within the BEC. By
controlling the flow velocity we determine the critical velocity for the
nucleation of a single vortex dipole, with excellent agreement between
experimental and numerical results. We present measurements of vortex dipole
dynamics, finding that the vortex cores of opposite charge can exist for many
seconds and that annihilation is inhibited in our highly oblate trap geometry.
For sufficiently rapid flow velocities we find that clusters of like-charge
vortices aggregate into long-lived dipolar flow structures.Comment: 4 pages, 4 figures, 1 EPAPS fil
ΠΠ΅Π»ΡΠ½ΠΎΠΊΠ°ΠΌΠ΅Π½Π½Π°Ρ Π±ΠΎΠ»Π΅Π·Π½Ρ ΡΡΠ΅Π΄ΠΈ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΎΠ³ΠΎ ΠΏΠ΅ΡΡΠΎΠ½Π°Π»Π° ΠΏΠΎΠ»ΠΈΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ: ΡΠ°ΠΊΡΠΎΡΡ ΡΠΈΡΠΊΠ° Π΅Π΅ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π² ΡΠ°Π·Π½ΡΡ ΠΏΡΠΎΡΠ΅ΡΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π³ΡΡΠΏΠΏΠ°Ρ
The aim. Identification of risk factors for gallstone disease (GDS) development between different professional groups of polyclinic medical staff. Material and methods. 75 medical staff members were divided into two groups (1st group: 30 doctors; 2nd group: 45 nurses). All of them were interviewed fo r information about profession, gender, age, waist circumference (WC), body mass index (BMI), smoking, arterial hypertension (AH), diabetes mellitus (DM) and hypercholesterolemia. In addition, women were interviewed about the number of pregnancies, ostmenopause and taking oral contraceptive pills (OCPs). To assess physical activity, a short international questionnaire on physical activity (IPAQ) was used. To identify the presence of professional burnout (PB) syndrome we applied the Maslach Burnout Inventory (MBI) questionnaire, adapted by N.Π. Vodopianova for medical staff. At the final stage, the data of abdominal organs ultrasound examination were analyzed based on the materials of medical staff outpatient records. Results. The GSD prevalence among doctors was 33.3%, and 24.4% among nurses. In both groups age, AH, weight, WC and BMI contribute to GSD formation. In the first group of individuals with GSD, the level of total cholesterol (TC) was significantly higher. In the same group extremely high PB, postmenopause (p <0.05) and hypodynamia (p <0.1) were much more common. In the second group, there were more DM cases and pregnancies (p <0.05). Conclusion. The medical staff of the clinic has a high GSD incidence, whose frequency depends not only on classical risk factors prevalence, but is also determined by profession peculiarities, characterized by high psychological stress and lower physical activity of physicians, compared to nurses.Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. ΠΡΡΠ²ΠΈΡΡ ΡΠ°ΠΊΡΠΎΡΡ ΡΠΈΡΠΊΠ° ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΆΠ΅Π»ΡΠ½ΠΎΠΊΠ°ΠΌΠ΅Π½Π½ΠΎΠΉ Π±ΠΎΠ»Π΅Π·Π½ΠΈ (ΠΠΠ) ΡΡΠ΅Π΄ΠΈ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΎΠ³ΠΎ ΠΏΠ΅ΡΡΠΎΠ½Π°Π»Π° ΠΏΠΎΠ»ΠΈΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ Π² ΡΠ°Π·Π½ΡΡ
ΠΏΡΠΎΡΠ΅ΡΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
Π³ΡΡΠΏΠΏΠ°Ρ
. ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π ΠΏΠΎΠ»ΠΈΠΊΠ»ΠΈΠ½ΠΈΠΊΠ΅ Π±ΡΠ»ΠΎ ΠΎΡΠΌΠΎΡΡΠ΅Π½ΠΎ ΠΈ Π°Π½ΠΊΠ΅ΡΠΈΡΠΎΠ²Π°Π½ΠΎ 75 ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
ΡΠΎΡΡΡΠ΄Π½ΠΈΠΊΠΎΠ² ΠΏΠΎΠ»ΠΈΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ, ΠΊΠΎΡΠΎΡΡΠ΅ Π±ΡΠ»ΠΈ ΡΠ°Π·Π΄Π΅Π»Π΅Π½Ρ Π½Π° Π΄Π²Π΅ Π³ΡΡΠΏΠΏΡ. Π 1-Ρ Π±ΡΠ»ΠΈ Π²ΠΊΠ»ΡΡΠ΅Π½Ρ 30 Π²ΡΠ°ΡΠ΅ΠΉ; Π²ΠΎ 2-Ρ - 45 ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
ΡΠ΅ΡΡΠ΅Ρ. ΠΠ½Π°Π»ΠΈΠ·Ρ ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π°Π»ΠΈΡΡ ΡΠ°ΠΊΠΈΠ΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΠΈ, ΠΊΠ°ΠΊ ΠΏΡΠΎΡΠ΅ΡΡΠΈΡ, ΠΏΠΎΠ», Π²ΠΎΠ·ΡΠ°ΡΡ, ΠΎΠ±ΡΠ΅ΠΌ ΡΠ°Π»ΠΈΠΈ (ΠΠ’), ΠΈΠ½Π΄Π΅ΠΊΡ ΠΌΠ°ΡΡΡ ΡΠ΅Π»Π° (ΠΠΠ’), ΠΊΡΡΠ΅Π½ΠΈΠ΅, Π½Π°Π»ΠΈΡΠΈΠ΅ Π°ΡΡΠ΅ΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π³ΠΈΠΏΠ΅ΡΡΠ΅Π½Π·ΠΈΠΈ (ΠΠ), ΡΠ°Ρ
Π°ΡΠ½ΠΎΠ³ΠΎ Π΄ΠΈΠ°Π±Π΅ΡΠ° (Π‘Π), Π³ΠΈΠΏΠ΅ΡΡ
ΠΎΠ»Π΅ΡΡΠ΅ΡΠΈΠ½Π΅ΠΌΠΈΠΈ, ΠΏΠΎΡΡΠΌΠ΅Π½ΠΎΠΏΠ°ΡΠ·Ρ; Ρ ΠΆΠ΅Π½ΡΠΈΠ½ β ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ Π±Π΅ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΡΡΠ΅ΠΉ ΠΈ ΠΏΡΠΈΠ΅ΠΌ ΠΎΡΠ°Π»ΡΠ½ΡΡ
ΠΊΠΎΠ½ΡΡΠ°ΡΠ΅ΠΏΡΠΈΠ²ΠΎΠ² (ΠΠ). ΠΠ»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½ΡΠ»ΠΈ ΠΊΡΠ°ΡΠΊΠΈΠΉ ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΡΠΉ ΠΎΠΏΡΠΎΡΠ½ΠΈΠΊ ΠΏΠΎ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ (IPAQ). ΠΠ»Ρ Π²ΡΡΠ²Π»Π΅Π½ΠΈΡ ΡΠΈΠΌΠΏΡΠΎΠΌΠΎΠ² ΠΏΡΠΎΡΠ΅ΡΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ Π²ΡΠ³ΠΎΡΠ°Π½ΠΈΡ (ΠΠ) ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΈ ΠΎΠΏΡΠΎΡΠ½ΠΈΠΊ Maslach Burnout Inventory (MBI), Π°Π΄Π°ΠΏΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠΉ Π.Π. ΠΠΎΠ΄ΠΎΠΏΡΡΠ½ΠΎΠ²ΠΎΠΉ Π΄Π»Ρ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
ΡΠΎΡΡΡΠ΄Π½ΠΈΠΊΠΎΠ². ΠΠ° ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠΌ ΡΡΠ°ΠΏΠ΅ Π°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π»ΠΈΡΡ Π΄Π°Π½Π½ΡΠ΅ ΡΠ»ΡΡΡΠ°Π·Π²ΡΠΊΠΎΠ²ΠΎΠ³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΎΡΠ³Π°Π½ΠΎΠ² Π±ΡΡΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΠΎΡΡΠΈ ΠΏΠΎ Π°ΠΌΠ±ΡΠ»Π°ΡΠΎΡΠ½ΡΠΌ ΠΊΠ°ΡΡΠ°ΠΌ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
ΡΠ°Π±ΠΎΡΠ½ΠΈΠΊΠΎΠ². Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Π Π°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΠΎΡΡΡ ΠΠΠ ΡΡΠ΅Π΄ΠΈ Π²ΡΠ°ΡΠ΅ΠΉ ΡΠΎΡΡΠ°Π²ΠΈΠ»Π° 33,3%, ΠΈ 24,4% ΡΡΠ΅Π΄ΠΈ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
ΡΠ΅ΡΡΠ΅Ρ. Π ΠΎΠ±Π΅ΠΈΡ
Π³ΡΡΠΏΠΏΠ°Ρ
Π½Π° ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΠΠ Π²Π»ΠΈΡΡΡ Π²ΠΎΠ·ΡΠ°ΡΡ, Π½Π°Π»ΠΈΡΠΈΠ΅ ΠΠ, Π²Π΅Ρ, ΠΠ’, ΠΠΠ’. Π ΠΏΠ΅ΡΠ²ΠΎΠΉ Π³ΡΡΠΏΠΏΠ΅ Π»ΠΈΡ Ρ ΠΠΠ ΡΡΠΎΠ²Π΅Π½Ρ ΠΎΠ±ΡΠ΅Π³ΠΎ Ρ
ΠΎΠ»Π΅ΡΡΠ΅ΡΠΈΠ½Π° Π±ΡΠ» Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎ Π²ΡΡΠ΅ (ΠΠ₯). Π ΡΡΠΎΠΉ ΠΆΠ΅ Π³ΡΡΠΏΠΏΠ΅ ΠΠ ΠΊΡΠ°ΠΉΠ½Π΅ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ, ΠΏΠΎΡΡΠΌΠ΅Π½ΠΎΠΏΠ°ΡΠ·Π° (p<0,05) ΠΈ Π³ΠΈΠΏΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡ (p<0,1) Π²ΡΡΡΠ΅ΡΠ°Π»ΠΈΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΠ°ΡΠ΅. Π Π³ΡΡΠΏΠΏΠ΅ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
ΡΠ΅ΡΡΠ΅Ρ Ρ ΠΠΠ ΠΎΡΠΌΠ΅ΡΠ°Π»ΠΎΡΡ ΠΏΡΠ΅ΠΎΠ±Π»Π°Π΄Π°Π½ΠΈΠ΅ Π»ΠΈΡ Ρ Π‘Π ΠΈ Π±ΠΎΠ»ΡΡΠ΅Π΅ ΡΠΈΡΠ»ΠΎ Π±Π΅ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΡΡΠ΅ΠΉ (p<0,05). ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. Π£ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΎΠ³ΠΎ ΠΏΠ΅ΡΡΠΎΠ½Π°Π»Π° ΠΏΠΎΠ»ΠΈΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ ΠΈΠΌΠ΅Π΅Ρ ΠΌΠ΅ΡΡΠΎ Π²ΡΡΠΎΠΊΠ°Ρ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΠΎΡΡΡ ΠΠΠ, ΡΠ°ΡΡΠΎΡΠ° ΠΊΠΎΡΠΎΡΠΎΠΉ Π·Π°Π²ΠΈΡΠΈΡ Π½Π΅ ΡΠΎΠ»ΡΠΊΠΎ ΠΎΡ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΠΎΡΡΠΈ ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΡΠΈΡΠΊΠ°, Π½ΠΎ ΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΡΠΌΠΈ ΠΏΡΠΎΡΠ΅ΡΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ Π΄Π΅ΡΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ, Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΡΡΠ΅ΠΉΡΡ Π²ΡΡΠΎΠΊΠΎΠΉ ΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π½Π°Π³ΡΡΠ·ΠΊΠΎΠΉ ΠΈ Π±ΠΎΠ»Π΅Π΅ Π½ΠΈΠ·ΠΊΠΎΠΉ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ Π²ΡΠ°ΡΠ΅Π±Π½ΠΎΠ³ΠΎ ΠΏΠ΅ΡΡΠΎΠ½Π°Π»Π°, ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΠΌΠΈ ΡΠ΅ΡΡΡΠ°ΠΌΠΈ
Exact Quantum Monte Carlo Process for the Statistics of Discrete Systems
We introduce an exact Monte Carlo approach to the statistics of discrete
quantum systems which does not rely on the standard fragmentation of the
imaginary time, or any small parameter. The method deals with discrete objects,
kinks, representing virtual transitions at different moments of time. The
global statistics of kinks is reproduced by explicit local procedures, the key
one being based on the exact solution for the biased two-level system.Comment: 4 pages, latex, no figures, English translation of the paper
Dissipative dynamics of superfluid vortices at non-zero temperatures
We consider the evolution and dissipation of vortex rings in a condensate at
non-zero temperature, in the context of the classical field approximation,
based on the defocusing nonlinear Schr\"odinger equation. The temperature in
such a system is fully determined by the total number density and the number
density of the condensate. A vortex ring is introduced into a condensate in a
state of thermal equilibrium, and interacts with non-condensed particles. These
interactions lead to a gradual decrease in the vortex line density, until the
vortex ring completely disappears. We show that the square of the vortex line
length changes linearly with time, and obtain the corresponding universal decay
law. We relate this to mutual friction coefficients in the fundamental equation
of vortex motion in superfluids.Comment: 4 pages, 3 figure
Decay of quantised vorticity by sound emission
It is thought that in a quantum fluid sound generation is the ultimate sink
of turbulent kinetic energy in the absence of any other dissipation mechanism
near absolute zero. We show that a suitably trapped Bose-Einstein condensate
provides a model system to study the sound emitted by accelerating vortices in
a controlled way.Comment: 6 pages, 3 figure
Ultracold Dipolar Gases in Optical Lattices
This tutorial is a theoretical work, in which we study the physics of
ultra-cold dipolar bosonic gases in optical lattices. Such gases consist of
bosonic atoms or molecules that interact via dipolar forces, and that are
cooled below the quantum degeneracy temperature, typically in the nK range.
When such a degenerate quantum gas is loaded into an optical lattice produced
by standing waves of laser light, new kinds of physical phenomena occur. These
systems realize then extended Hubbard-type models, and can be brought to a
strongly correlated regime. The physical properties of such gases, dominated by
the long-range, anisotropic dipole-dipole interactions, are discussed using the
mean-field approximations, and exact Quantum Monte Carlo techniques (the Worm
algorithm).Comment: 56 pages, 26 figure
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