2,468 research outputs found
Many-body localization beyond eigenstates in all dimensions
Isolated quantum systems with quenched randomness exhibit many-body
localization (MBL), wherein they do not reach local thermal equilibrium even
when highly excited above their ground states. It is widely believed that
individual eigenstates capture this breakdown of thermalization at finite size.
We show that this belief is false in general and that a MBL system can exhibit
the eigenstate properties of a thermalizing system. We propose that localized
approximately conserved operators (l-bits) underlie localization in such
systems. In dimensions , we further argue that the existing MBL
phenomenology is unstable to boundary effects and gives way to l-bits.
Physical consequences of l-bits include the possibility of an eigenstate
phase transition within the MBL phase unrelated to the dynamical transition in
and thermal eigenstates at all parameters in . Near-term experiments
in ultra-cold atomic systems and numerics can probe the dynamics generated by
boundary layers and emergence of l-bits.Comment: 12 pages, 5 figure
Thermal inclusions: how one spin can destroy a many-body localized phase
Many-body localized (MBL) systems lie outside the framework of statistical
mechanics, as they fail to equilibrate under their own quantum dynamics. Even
basic features of MBL systems such as their stability to thermal inclusions and
the nature of the dynamical transition to thermalizing behavior remain poorly
understood. We study a simple model to address these questions: a two level
system interacting with strength with localized bits subject to
random fields. On increasing , the system transitions from a MBL to a
delocalized phase on the \emph{vanishing} scale , up to
logarithmic corrections. In the transition region, the single-site eigenstate
entanglement entropies exhibit bi-modal distributions, so that localized bits
are either "on" (strongly entangled) or "off" (weakly entangled) in
eigenstates. The clusters of "on" bits vary significantly between eigenstates
of the \emph{same} sample, which provides evidence for a heterogenous
discontinuous transition out of the localized phase in single-site observables.
We obtain these results by perturbative mapping to bond percolation on the
hypercube at small and by numerical exact diagonalization of the full
many-body system. Our results imply the MBL phase is unstable in systems with
short-range interactions and quenched randomness in dimensions that are
high but finite.Comment: 17 pages, 12 figure
Stratospheric sudden warming effects on winds and temperature in the middle atmosphere at middle and low latitudes: a study using WACCM
A stratospheric sudden warming (SSW) is a dynamical phenomenon of the
wintertime stratosphere caused by the interaction between planetary Rossby
waves propagating from the troposphere and the stratospheric zonal-mean flow.
While the effects of SSW events are seen predominantly in high latitudes,
they can also produce significant changes in middle and low latitude
temperature and winds. In this study we quantify the middle and low latitude
effects of SSW events on temperature and zonal-mean winds using a composite
of SSW events between 1988 and 2010 simulated with the specified dynamics
version of the Whole Atmosphere Community Climate Model (WACCM). The
temperature and wind responses seen in the tropics also extend into the low
latitudes in the other hemisphere. There is variability in observed zonal-mean winds and temperature depending on the observing location within the
displaced or split polar vortex and propagation direction of the planetary
waves. The propagation of planetary waves show that they originate in
midβhigh latitudes and propagate upward and equatorward into the mid-latitude
middle atmosphere where they produce westward forcing reaching peak values of
~ 60β70 m s<sup>β1</sup> day<sup>β1</sup>. These propagation paths in the
lower latitude stratosphere appear to depend on the phase of the quasi-biennial oscillation (QBO). During
the easterly phase of the QBO, waves originating at high latitudes propagate
across the equator, while in the westerly phase of the QBO, the planetary
waves break at ~ 20β25Β° N and there is no propagation across
the equator. The propagation of planetary waves across the equator during the
easterly phase of the QBO reduces the tropical upwelling and poleward flow in
the upper stratosphere
Emergent Coulombic criticality and Kibble-Zurek scaling in a topological magnet
When a classical system is driven through a continuous phase transition, its
nonequilibrium response is universal and exhibits Kibble-Zurek scaling. We
explore this dynamical scaling in the novel context of a three-dimensional
topological magnet with fractionalized excitations, namely the liquid-gas
transition of the emergent mobile magnetic monopoles in dipolar spin ice. Using
field-mixing and finite-size scaling techniques, we place the critical point of
the liquid-gas line in the three-dimensional Ising universality class. We then
demonstrate Kibble-Zurek scaling for sweeps of the magnetic field through the
critical point. Unusually slow microscopic time scales in spin ice offer a
unique opportunity to detect this universal nonequilibrium physics in current
experimental setups.This work was supported in part by Engineering and Physical Sciences Research Council (EPSRC) Grant No. EP/G049394/1 (C.C.), the Helmholtz Virtual Institute βNew States of Matter and Their Excitations,β and the EPSRC NetworkPlus on βEmergence and Physics far from Equilibrium.β Research at Perimeter Institute is supported by the Government of Canada through Industry Canada and by the Province of Ontario through the Ministry of Economic Development and Innovation. The calculations were performed using the Darwin Supercomputer of the University of Cambridge High Performance Computing Service (http://www.hpc.cam.ac.uk/) and the ARCHER UK National Supercomputing Service (http://www.archer.ac.uk/, for which access was provided by the ARCHER Driving Test scheme). The authors are grateful to A. Sandvik for useful discussions and to S. L. Sondhi for advice and collaboration on several pieces of related work. J.O.H. is grateful to the EPSRC for funding, and to Michael Rutter for computing support.This is the author accepted manuscript. The final version is available from the American Physical Society via http://dx.doi.org/10.1103/PhysRevB.92.07514
Nanosecond pulsed 620 nm source by frequency-doubling a phosphosilicate Raman fiber amplifier
We demonstrate a nanosecond pulsed source at 620 nm with watt-level average power by frequency-doubling a 1240 nm phosphosilicate Raman fiber amplifier. A gain-switched laser diode operating at 1064 nm is amplified in an ytterbium fiber master oscillator power amplifier system and then converted to 1240 nm using a phosphosilicate Raman fiber amplifier with a conversion efficiency of up to 66%. The Raman fiber amplifier is seeded with a continuous-wave 1240 nm laser diode to obtain narrow-linewidth radiation, which is subsequently frequency-doubled in a periodically poled lithium tantalate crystal. A maximum average power of 1.5 W is generated at 620 nm, corresponding to a pulse energy of 300 nJ at a repetition rate of 5 MHz. The source has excellent beam quality (M2β€1.16) and an optical efficiency (1064 nm to 620 nm) of 20%, demonstrating an effective architecture for generating red pulsed light for biomedical imaging applications
ΠΠ»ΠΈΡΠ½ΠΈΠ΅ Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π° Π½Π° ΡΠΏΠΈΠ΄Π΅ΠΌΠΈΠΎΠ»ΠΎΠ³ΠΈΡ ΡΡΠ°Π²ΠΌ Π²ΠΎ Π²ΡΠ΅ΠΌΡ ΠΏΠ΅ΡΠ²ΠΎΠΉ Π²ΠΎΠ»Π½Ρ COVID-19 Π² ΠΠ½Π΄ΠΈΠΈ
Background. The pattern of hospital admissions and medical care changed during the COVID pandemic.
The aim of the study to describe the nature of patients attending the orthopedic emergency department of a level 1 trauma center in terms of number and proportion based on demographic characteristics and the nature of the injury before the lockdown, during the lockdown, and during the unlocking period of the nationwide lockdown for controlling the COVID-19 pandemic in India.
Methods. We conducted a longitudinal study from 01.01.2020 to 31.12.2020. Patients attending the orthopedic emergency were grouped based on cause, type, and site of injury. The median number observed each day with IQR. The distribution of the same was compared between the prelockdown with lockdown period and the lockdown period with a phased unlocking period.
Results. A total of 10513 patients were included. There was a statistically significant reduction in the proportion of patients needing inpatient care between the prelockdown phase and lockdown phase (p = 0.008). However, this was not seen between lockdown and postlockdown periods (p = 0.47). The proportion of road traffic accidents dropped from 26% to 15% during this time (p0.001). The proportion of contusions was reduced and that of soft tissue injuries increased (p0.001). The proportion of lower limb injuries decreased from the prelockdown phase to the lockdown phase, and that of spinal injury patients increased (p = 0.007). The proportion of patients with contusions increased and soft tissue injuries decreased during this period (p0.001). Lower limb injuries and road traffic accidents increased, and spinal injuries were reduced (p0.001).
Conclusion. The lockdown for controlling the spread of the pandemic affected the demographic and epidemiological aspects of injuries attending the orthopedic emergency department of a level 1 trauma center in a developing country. There was a decrease in the proportion of females and children attending the ED during the lockdown. The number of road traffic accedents s decreased during the lockdown. The number of patients with contusions attending the trauma center during the lockdown decreased, but there was an increase in the number of patients with spine injuries. We suggest that improvement in triage facilities, wider use of telemedicine, and increasing the stock of PPEs are essential for tackling such situations in the future.ΠΠ²Π΅Π΄Π΅Π½ΠΈΠ΅. ΠΠΎ Π²ΡΠ΅ΠΌΡ ΠΏΠ°Π½Π΄Π΅ΠΌΠΈΠΈ COVID-19 ΠΈΠ·ΠΌΠ΅Π½ΠΈΠ»Π°ΡΡ ΡΡΡΡΠΊΡΡΡΠ° Π³ΠΎΡΠΏΠΈΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΉ ΠΈ ΠΎΠΊΠ°Π·Π°Π½ΠΈΡ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΎΠΉ ΠΏΠΎΠΌΠΎΡΠΈ.
Π¦Π΅Π»Ρ ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°ΡΡ ΡΠΏΠΈΠ΄Π΅ΠΌΠΈΠΎΠ»ΠΎΠ³ΠΈΡ ΠΈ ΡΠΈΠΏ ΡΡΠ°Π²ΠΌ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°ΠΌΠΈ, ΠΎΠ±ΡΠ°ΡΠΈΠ²ΡΠΈΠΌΠΈΡΡ Π² ΡΡΠ°Π²ΠΌΠΎΡΠ΅Π½ΡΡ 1-Π³ΠΎ ΡΡΠΎΠ²Π½Ρ Π²ΠΎ Π²ΡΠ΅ΠΌΡ ΠΏΠ°Π½Π΄Π΅ΠΌΠΈΠΈ ΠΈ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π° Π² ΠΠ½Π΄ΠΈΠΈ.
ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. ΠΡ ΠΏΡΠΎΠ²Π΅Π»ΠΈ Π»ΠΎΠ½Π³ΠΈΡΡΠ΄Π½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Ρ 01.01.2020 ΠΏΠΎ 31.12.2020 ΠΠ°ΡΠΈΠ΅Π½ΡΡ, ΠΎΠ±ΡΠ°ΡΠΈΠ²ΡΠΈΠ΅ΡΡ Π·Π° Π½Π΅ΠΎΡΠ»ΠΎΠΆΠ½ΠΎΠΉ ΡΡΠ°Π²ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΠΎΠΌΠΎΡΡΡ, Π±ΡΠ»ΠΈ ΡΠ³ΡΡΠΏΠΏΠΈΡΠΎΠ²Π°Π½Ρ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΠΏΡΠΈΡΠΈΠ½Ρ, ΡΠΈΠΏΠ° ΠΈ ΠΌΠ΅ΡΡΠ° ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ. Π‘ΡΠ΅Π΄Π½Π΅Π΅ ΡΠΈΡΠ»ΠΎ Π΅ΠΆΠ΅Π΄Π½Π΅Π½ΡΡ
ΠΎΠ±ΡΠ°ΡΠ΅Π½ΠΈΠΉ Π±ΡΠ»ΠΎ ΡΠ°ΡΡΠΈΡΠ°Π½ΠΎ Ρ ΠΏΠΎΠΌΠΎΡΡΡ IQR (ΠΈΠ½ΡΠ΅ΡΠΊΠ²Π°ΡΡΠΈΠ»ΡΠ½ΠΎΠ³ΠΎ ΡΠ°Π·ΠΌΠ°Ρ
Π°). ΠΡΠ»ΠΎ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠΉ ΡΡΠ΅Π΄Π½Π΅Π³ΠΎ ΡΠΈΡΠ»Π° Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΠΉ ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄Π°ΠΌΠΈ Π΄ΠΎ ΠΈ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π°, Π° ΡΠ°ΠΊΠΆΠ΅ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π° ΠΈ ΠΏΠΎΡΠ»Π΅ Π΅Π³ΠΎ ΡΠ½ΡΡΠΈΡ.
Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΡΠ΅Π³ΠΎ Π² ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π±ΡΠ»ΠΎ Π²ΠΊΠ»ΡΡΠ΅Π½ΠΎ 10 513 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ². ΠΠ°Π±Π»ΡΠ΄Π°Π»ΠΎΡΡ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ Π·Π½Π°ΡΠΈΠΌΠΎΠ΅ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ Π΄ΠΎΠ»ΠΈ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², Π½ΡΠΆΠ΄Π°ΡΡΠΈΡ
ΡΡ Π² Π³ΠΎΡΠΏΠΈΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ, ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄Π°ΠΌΠΈ Π΄ΠΎ ΠΈ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π° (p = 0,008). ΠΠ΄Π½Π°ΠΊΠΎ ΡΡΠΎΠ³ΠΎ Π½Π΅ Π½Π°Π±Π»ΡΠ΄Π°Π»ΠΎΡΡ ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄Π°ΠΌΠΈ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π° ΠΈ ΠΏΠΎΡΡΠ»ΠΎΠΊΠ΄Π°ΡΠ½Π° (p = 0,47). ΠΠΎΠ»Ρ Π΄ΠΎΡΠΎΠΆΠ½ΠΎ-ΡΡΠ°Π½ΡΠΏΠΎΡΡΠ½ΡΡ
ΠΏΡΠΎΠΈΡΡΠ΅ΡΡΠ²ΠΈΠΉ ΡΠ½ΠΈΠ·ΠΈΠ»Π°ΡΡ Ρ 26% Π΄ΠΎ 15% ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄Π°ΠΌΠΈ Π΄ΠΎ ΠΈ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π° (p0,001). ΠΠΎΠ»Ρ ΡΡΠΈΠ±ΠΎΠ² ΡΠΌΠ΅Π½ΡΡΠΈΠ»Π°ΡΡ, Π° ΠΌΡΠ³ΠΊΠΎΡΠΊΠ°Π½Π½ΡΡ
ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΠΉ ΡΠ²Π΅Π»ΠΈΡΠΈΠ»Π°ΡΡ (p0,001). ΠΠΎΠ»Ρ ΡΡΠ°Π²ΠΌ Π½ΠΈΠΆΠ½ΠΈΡ
ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΡΡΠ΅ΠΉ ΡΠΌΠ΅Π½ΡΡΠΈΠ»Π°ΡΡ ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄Π°ΠΌΠΈ Π΄ΠΎ ΠΈ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π°, Π° Π΄ΠΎΠ»Ρ ΡΡΠ°Π²ΠΌ ΠΏΠΎΠ·Π²ΠΎΠ½ΠΎΡΠ½ΠΈΠΊΠ° ΡΠ²Π΅Π»ΠΈΡΠΈΠ»Π°ΡΡ (p = 0,007).
ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΠ°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠΉ Π»ΠΎΠΊΠ΄Π°ΡΠ½ ΠΏΠΎΠ²Π»ΠΈΡΠ» Π½Π° Π΄Π΅ΠΌΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈ ΡΠΏΠΈΠ΄Π΅ΠΌΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΠΈ ΡΡΠ°Π²ΠΌ Π² ΡΡΠ°Π²ΠΌΠΎΡΠ΅Π½ΡΡΠ΅ 1-Π³ΠΎ ΡΡΠΎΠ²Π½Ρ Π² ΠΠ½Π΄ΠΈΠΈ. ΠΠ°Π±Π»ΡΠ΄Π°Π»ΠΎΡΡ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ Π΄ΠΎΠ»ΠΈ ΠΆΠ΅Π½ΡΠΈΠ½ ΠΈ Π΄Π΅ΡΠ΅ΠΉ, ΠΎΠ±ΡΠ°ΡΠΈΠ²ΡΠΈΡ
ΡΡ Π² ΠΎΡΠ΄Π΅Π»Π΅Π½ΠΈΠ΅ Π½Π΅ΠΎΡΠ»ΠΎΠΆΠ½ΠΎΠΉ ΠΏΠΎΠΌΠΎΡΠΈ. ΠΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΠ’Π ΡΠΎΠΊΡΠ°ΡΠΈΠ»ΠΎΡΡ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π°. ΠΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΡΡΠΈΠ±Π°ΠΌΠΈ, ΠΎΠ±ΡΠ°ΡΠΈΠ²ΡΠΈΡ
ΡΡ Π² ΡΡΠ°Π²ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ΅Π½ΡΡ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π»ΠΎΠΊΠ΄Π°ΡΠ½Π° ΡΠΌΠ΅Π½ΡΡΠΈΠ»ΠΎΡΡ, Π° ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΡΡΠ°Π²ΠΌΠ°ΠΌΠΈ ΠΏΠΎΠ·Π²ΠΎΠ½ΠΎΡΠ½ΠΈΠΊΠ° ΡΠ²Π΅Π»ΠΈΡΠΈΠ»ΠΎΡΡ. ΠΡ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΡΠ΅ΠΌ ΡΠ»ΡΡΡΠΈΡΡ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΡΡ ΡΠΎΡΡΠΈΡΠΎΠ²ΠΊΡ, ΡΠ°ΡΡΠΈΡΠΈΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅Π»Π΅ΠΌΠ΅Π΄ΠΈΡΠΈΠ½Ρ ΠΈ ΡΠ²Π΅Π»ΠΈΡΠΈΡΡ Π·Π°ΠΏΠ°ΡΡ ΡΡΠ΅Π΄ΡΡΠ² ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΠΎΠΉ Π·Π°ΡΠΈΡΡ Π΄Π»Ρ Π±ΠΎΡΡΠ±Ρ Ρ ΠΏΠΎΠ΄ΠΎΠ±Π½ΡΠΌΠΈ ΡΠΈΡΡΠ°ΡΠΈΡΠΌΠΈ Π² Π±ΡΠ΄ΡΡΠ΅ΠΌ
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