510 research outputs found
Vacuum Squeezing in Atomic Media via Self-Rotation
When linearly polarized light propagates through a medium in which
elliptically polarized light would undergo self-rotation, squeezed vacuum can
appear in the orthogonal polarization. A simple relationship between
self-rotation and the degree of vacuum squeezing is developed. Taking into
account absorption, we find the optimum conditions for squeezing in any medium
that can produce self-rotation. We then find analytic expressions for the
amount of vacuum squeezing produced by an atomic vapor when light is
near-resonant with a transition between various low-angular-momentum states.
Finally, we consider a gas of multi-level Rb atoms, and analyze squeezing for
light tuned near the D-lines under realistic conditions.Comment: 10 pages, 6 figures; Submitted to PR
Inverse Spectral-Scattering Problem with Two Sets of Discrete Spectra for the Radial Schroedinger Equation
The Schroedinger equation on the half line is considered with a real-valued,
integrable potential having a finite first moment. It is shown that the
potential and the boundary conditions are uniquely determined by the data
containing the discrete eigenvalues for a boundary condition at the origin, the
continuous part of the spectral measure for that boundary condition, and a
subset of the discrete eigenvalues for a different boundary condition. This
result extends the celebrated two-spectrum uniqueness theorem of Borg and
Marchenko to the case where there is also a continuous spectru
Evanescent light-matter Interactions in Atomic Cladding Wave Guides
Alkali vapors, and in particular rubidium, are being used extensively in
several important fields of research such as slow and stored light non-linear
optics3 and quantum computation. Additionally, the technology of alkali vapors
plays a major role in realizing myriad industrial applications including for
example atomic clocks magentometers8 and optical frequency stabilization.
Lately, there is a growing effort towards miniaturizing traditional
centimeter-size alkali vapor cells. Owing to the significant reduction in
device dimensions, light matter interactions are greatly enhanced, enabling new
functionalities due to the low power threshold needed for non-linear
interactions. Here, taking advantage of the mature Complimentary
Metal-Oxide-Semiconductor (CMOS) compatible platform of silicon photonics, we
construct an efficient and flexible platform for tailored light vapor
interactions on a chip. Specifically, we demonstrate light matter interactions
in an atomic cladding wave guide (ACWG), consisting of CMOS compatible silicon
nitride nano wave-guide core with a Rubidium (Rb) vapor cladding. We observe
the highly efficient interaction of the electromagnetic guided mode with the
thermal Rb cladding. The nature of such interactions is explained by a model
which predicts the transmission spectrum of the system taking into account
Doppler and transit time broadening. We show, that due to the high confinement
of the optical mode (with a mode area of 0.3{\lambda}2), the Rb absorption
saturates at powers in the nW regime.Comment: 10 Pages 4 Figures. 1 Supplementar
Homogeneous singularities inside collapsing wormholes
We analyze analytically and numerically the origin of the singularity in the
course of the collapse of a wormhole with the exotic scalar field Psi with
negative energy density, and with this field Psi together with the ordered
magnetic field H. We do this under the simplifying assumptions of the spherical
symmetry and that in the vicinity of the singularity the solution of the
Einstein equations depends only on one coordinate (the homogeneous
approximation). In the framework of these assumptions we found the principal
difference between the case of the collapse of the ordinary scalar field Phi
with the positive energy density together with an ordered magnetic field H and
the collapse of the exotic scalar field Psi together with the magnetic field H.
The later case is important for the possible astrophysical manifestation of the
wormholes.Comment: 10 pages, 5 figures each of which has a),b),c),and d) sub-figures. To
be published in "Physical review. D, Particles, fields, gravitation, and
cosmology
State Transfer Between a Mechanical Oscillator and Microwave Fields in the Quantum Regime
Recently, macroscopic mechanical oscillators have been coaxed into a regime
of quantum behavior, by direct refrigeration [1] or a combination of
refrigeration and laser-like cooling [2, 3]. This exciting result has
encouraged notions that mechanical oscillators may perform useful functions in
the processing of quantum information with superconducting circuits [1, 4-7],
either by serving as a quantum memory for the ephemeral state of a microwave
field or by providing a quantum interface between otherwise incompatible
systems [8, 9]. As yet, the transfer of an itinerant state or propagating mode
of a microwave field to and from a mechanical oscillator has not been
demonstrated owing to the inability to agilely turn on and off the interaction
between microwave electricity and mechanical motion. Here we demonstrate that
the state of an itinerant microwave field can be coherently transferred into,
stored in, and retrieved from a mechanical oscillator with amplitudes at the
single quanta level. Crucially, the time to capture and to retrieve the
microwave state is shorter than the quantum state lifetime of the mechanical
oscillator. In this quantum regime, the mechanical oscillator can both store
and transduce quantum information
Towards high-speed optical quantum memories
Quantum memories, capable of controllably storing and releasing a photon, are
a crucial component for quantum computers and quantum communications. So far,
quantum memories have operated with bandwidths that limit data rates to MHz.
Here we report the coherent storage and retrieval of sub-nanosecond low
intensity light pulses with spectral bandwidths exceeding 1 GHz in cesium
vapor. The novel memory interaction takes place via a far off-resonant
two-photon transition in which the memory bandwidth is dynamically generated by
a strong control field. This allows for an increase in data rates by a factor
of almost 1000 compared to existing quantum memories. The memory works with a
total efficiency of 15% and its coherence is demonstrated by directly
interfering the stored and retrieved pulses. Coherence times in hot atomic
vapors are on the order of microsecond - the expected storage time limit for
this memory.Comment: 13 pages, 5 figure
THE ROLE OF POSTPARTUM VAGINAL BRUISING IN THE DEVELOPMENT OF ACUTE MASSIVE BLOOD LOSS
Purpose: To estimate the efficiency of the ultrasound diagnosis of postpartum vaginal hematoma in women with varicose veins of the lower extremitiesMaterials and Methods: 120 women with varicose veins of the lower extremities were examined. In 2 hours after birth for women was conducted transperineal ultrasound - research by vaginal and perineal ultrasound scanner PHILLIPS HD- 11.Results: Vaginal hematoma was detected in 31 (25.8%) women , and only 10 (8 %) had a damage of integrity of the mucous membrane. The study found that vaginal hematoma size 10,1Β±3,6 cm at the beginning of the formation can be asymptomatic , which may cause underestimation of the total blood loss in women with postpartum hemorrhage due to a variety of other competing causes.Summary: The use of analgesia in labor hinders timely diagnosis of postpartum hematomas of vulva and vagina
Modelling effects of phytobiotic administration on coherent responses to Salmonella infection in laying hens
Practice of layer poultry farming and commercial egg production relies on the optimal use and improvement of the welfare and genetically determined functional abilities of laying hens, their efficient intake of feed and its components, adaptation to housing conditions and resistance to infectious diseases including salmonellosis. Previous studies were focussed on relationships of chicken performance and resistance with the expression profiles of individual genes involved in metabolic processes and immune system, or with genetic markers that can be closely associated with these processes in chickens. In this study, mathematical models of coherent changes in laying hens were developed for the expression of eight genes involved in immunity and metabolism, on the one hand, and biochemical and immunological blood parameters, on the other hand, in response to Salmonella infection and administration of a phytobiotic Intebio. The proposed modelling approach can be a further basis for an in-depth research of the relationship between the gene expression, functional state and welfare of poultry, impact of pathogenic microorganisms and use of immunomodulatory drugs
ΠΠ°Π»Π΅ΠΆΠ½ΡΡΡΡ ΡΡΠ°Π½Ρ ΡΠΊΠ°Π½ΠΈΠ½ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ° Π²ΡΠ΄ ΠΏΠΎΠ²Π΅Π΄ΡΠ½ΠΊΠΎΠ²ΠΈΡ ΡΠ°ΠΊΡΠΎΡΡΠ² ΡΠΈΠ·ΠΈΠΊΡ Π² Π΄ΡΡΠ΅ΠΉ ΡΠΊΡΠ»ΡΠ½ΠΎΠ³ΠΎ Π²ΡΠΊΡ ΠΌ. ΠΠΎΠ»ΡΠ°Π²ΠΈ, Π²ΠΈΡΠ²Π»Π΅Π½ΠΈΡ ΡΠ· Π·Π°ΡΡΠΎΡΡΠ²Π°Π½Π½ΡΠΌ ΡΠ²ΡΠΎΠΏΠ΅ΠΉΡΡΠΊΠΈΡ ΡΠ½Π΄ΠΈΠΊΠ°ΡΠΎΡΡΠ²
The aim of the work was the definition of informativeness of European indicators in a comprehensive assessment of the state of periodontal tissues in children of school age and identification possible relationships with behavioral risk factors for periodontal disease. Analytical dental epidemiology was employed, using the EGOHID-2005 system. Oral hygiene and dental caries were assessed in 12- 15-year-old children in Poltava city. The main determinants of periodontal tissue diseases were non-observance of children a recommended regime of brushing teeth and unhealthy habits. Systematic monitoring of major dental diseases allows to determine their tendencies and, using European system of indicators of dental health, allows to identify the risk factors to be eliminated in order to prevent periodontal tissue diseases.Π¦Π΅Π»ΡΡ ΡΠ°Π±ΠΎΡΡ Π±ΡΠ»ΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΠΎΡΡΠΈ Π΅Π²ΡΠΎΠΏΠ΅ΠΉΡΠΊΠΈΡ
ΠΈΠ½Π΄ΠΈΠΊΠ°ΡΠΎΡΠΎΠ² Π² ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠΉ ΠΎΡΠ΅Π½ΠΊΠ΅ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ ΡΠΊΠ°Π½Π΅ΠΉ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ° Ρ Π΄Π΅ΡΠ΅ΠΉ ΡΠΊΠΎΠ»ΡΠ½ΠΎΠ³ΠΎ Π²ΠΎΠ·ΡΠ°ΡΡΠ° ΠΈ Π²ΡΡΠ²Π»Π΅Π½ΠΈΠ΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΡ
Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Π΅ΠΉ Ρ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ°ΠΊΡΠΎΡΠ°ΠΌΠΈ ΡΠΈΡΠΊΠ° Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ ΡΠΊΠ°Π½Π΅ΠΉ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ°. ΠΠ½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠΏΠΈΠ΄Π΅ΠΌΠΈΠΎΠ»ΠΎΠ³ΠΈΡ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ ΡΠΊΠ°Π½Π΅ΠΉ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ° Ρ Π΄Π΅ΡΠ΅ΠΉ Π΄Π²ΡΡ
ΠΊΠ»ΡΡΠ΅Π²ΡΡ
Π²ΠΎΠ·ΡΠ°ΡΡΠ½ΡΡ
Π³ΡΡΠΏΠΏ 12 ΠΈ 15 Π»Π΅Ρ ΠΏΠΎ 100 ΡΠ΅Π»ΠΎΠ²Π΅ΠΊ Π² Π³. ΠΠΎΠ»ΡΠ°Π²Π΅. ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ EGOHID β 2005 ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ², ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½Π½ΡΡ
ΠΠΠβ2013. ΠΡΠ½ΠΎΠ²Π½ΡΠΌΠΈ Π΄Π΅ΡΠ΅ΡΠΌΠΈΠ½Π°Π½ΡΠ°ΠΌΠΈ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ ΡΠΊΠ°Π½Π΅ΠΉ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ° Π±ΡΠ»ΠΎ Π½Π΅ΡΠΎΠ±Π»ΡΠ΄Π΅Π½ΠΈΠ΅ Π΄Π΅ΡΡΠΌΠΈ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠ΅ΠΆΠΈΠΌΠ° ΡΠΈΡΡΠΊΠΈ Π·ΡΠ±ΠΎΠ² ΠΈ Π½Π΅Π·Π΄ΠΎΡΠΎΠ²ΡΠ΅ ΠΏΡΠΈΠ²ΡΡΠΊΠΈ. Π‘ΠΈΡΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΌΠΎΠ½ΠΈΡΠΎΡΠΈΠ½Π³ ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
ΡΡΠΎΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΡΡ ΠΈΡ
ΡΠ΅Π½Π΄Π΅Π½ΡΠΈΠΈ ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΈΡΡΠ΅ΠΌΡ Π΅Π²ΡΠΎΠΏΠ΅ΠΉΡΠΊΠΈΡ
ΠΈΠ½Π΄ΠΈΠΊΠ°ΡΠΎΡΠΎΠ² ΡΡΠΎΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π·Π΄ΠΎΡΠΎΠ²ΡΡ Π²ΡΡΠ²ΠΈΡΡ ΡΠ°ΠΊΡΠΎΡΡ ΡΠΈΡΠΊΠ°, ΠΏΠΎΠ΄Π»Π΅ΠΆΠ°ΡΠΈΠ΅ ΡΡΡΡΠ°Π½Π΅Π½ΠΈΡ Ρ ΡΠ΅Π»ΡΡ ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠΈ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ ΡΠΊΠ°Π½Π΅ΠΉ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ°.ΠΠ΅ΡΠΎΡ ΡΠΎΠ±ΠΎΡΠΈ Π±ΡΠ»ΠΎ Π²ΠΈΠ·Π½Π°ΡΠ΅Π½Π½Ρ ΡΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠ²ΡΠΎΠΏΠ΅ΠΉΡΡΠΊΠΈΡ
ΡΠ½Π΄ΠΈΠΊΠ°ΡΠΎΡΡΠ² Ρ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΡΠΉ ΠΎΡΡΠ½ΡΡ ΡΡΠ°Π½Ρ ΡΠΊΠ°Π½ΠΈΠ½ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ° Π² Π΄ΡΡΠ΅ΠΉ ΡΠΊΡΠ»ΡΠ½ΠΎΠ³ΠΎ Π²ΡΠΊΡ ΡΠ° Π²ΠΈΡΠ²Π»Π΅Π½Π½Ρ ΠΌΠΎΠΆΠ»ΠΈΠ²ΠΈΡ
Π²Π·Π°ΡΠΌΠΎΠ·Π²βΡΠ·ΠΊΡΠ² Π· ΠΏΠΎΠ²Π΅Π΄ΡΠ½ΠΊΠΎΠ²ΠΈΠΌΠΈ ΡΠΈΠ½Π½ΠΈΠΊΠ°ΠΌΠΈ ΡΠΈΠ·ΠΈΠΊΡ Π²ΠΈΠ½ΠΈΠΊΠ½Π΅Π½Π½Ρ Π·Π°Ρ
Π²ΠΎΡΡΠ²Π°Π½Ρ ΡΠΊΠ°Π½ΠΈΠ½ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ°. ΠΠ½Π°Π»ΡΡΠΈΡΠ½Π° Π΅ΠΏΡΠ΄Π΅ΠΌΡΠΎΠ»ΠΎΠ³ΡΡ ΡΡΠ°Π½Ρ ΡΠΊΠ°Π½ΠΈΠ½ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ° Ρ Π΄ΡΡΠ΅ΠΉ Π΄Π²ΠΎΡ
ΠΊΠ»ΡΡΠΎΠ²ΠΈΡ
Π²ΡΠΊΠΎΠ²ΠΈΡ
Π³ΡΡΠΏ 12 Ρ 15 ΡΠΎΠΊΡΠ² ΠΏΠΎ 100 ΠΎΡΡΠ± Π² ΠΌ. ΠΠΎΠ»ΡΠ°Π²Ρ. ΠΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½Ρ ΠΡΠΆΠ½Π°ΡΠΎΠ΄Π½ΠΎΡ ΡΠΈΡΡΠ΅ΠΌΠΈ EGOHID β 2005 Ρ ΠΌΠ΅ΡΠΎΠ΄ΡΠ², ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½ΠΈΡ
ΠΠΠΠβ2013. ΠΡΠ½ΠΎΠ²Π½ΠΈΠΌΠΈ Π΄Π΅ΡΠ΅ΡΠΌΡΠ½Π°Π½ΡΠ°ΠΌΠΈ Π·Π°Ρ
Π²ΠΎΡΡΠ²Π°Π½Ρ ΡΠΊΠ°Π½ΠΈΠ½ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ° Π±ΡΠ»ΠΈ Π½Π΅Π΄ΠΎΡΡΠΈΠΌΠ°Π½Π½Ρ Π΄ΡΡΡΠΌΠΈ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ΡΠ΅ΠΆΠΈΠΌΡ ΡΠΈΡΠ΅Π½Π½Ρ Π·ΡΠ±ΡΠ² Ρ Π½Π΅Π·Π΄ΠΎΡΠΎΠ²Ρ Π·Π²ΠΈΡΠΊΠΈ. Π‘ΠΈΡΡΠ΅ΠΌΠ°ΡΠΈΡΠ½ΠΈΠΉ ΠΌΠΎΠ½ΡΡΠΎΡΠΈΠ½Π³ ΠΎΡΠ½ΠΎΠ²Π½ΠΈΡ
ΡΡΠΎΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΡΡΠ½ΠΈΡ
Π·Π°Ρ
Π²ΠΎΡΡΠ²Π°Π½Ρ Π΄ΠΎΠ·Π²ΠΎΠ»ΡΡ Π²ΠΈΠ·Π½Π°ΡΠΈΡΠΈ ΡΡ
ΡΠ΅Π½Π΄Π΅Π½ΡΡΡ Ρ Π·Π° Π΄ΠΎΠΏΠΎΠΌΠΎΠ³ΠΎΡ ΡΠΈΡΡΠ΅ΠΌΠΈ ΡΠ²ΡΠΎΠΏΠ΅ΠΉΡΡΠΊΠΈΡ
ΡΠ½Π΄ΠΈΠΊΠ°ΡΠΎΡΡΠ² ΡΡΠΎΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΡΡΠ½ΠΎΠ³ΠΎ Π·Π΄ΠΎΡΠΎΠ²βΡ Π²ΠΈΡΠ²ΠΈΡΠΈ ΡΠ°ΠΊΡΠΎΡΠΈ ΡΠΈΠ·ΠΈΠΊΡ, ΡΠΊΡ ΠΏΡΠ΄Π»ΡΠ³Π°ΡΡΡ ΡΡΡΠ½Π΅Π½Π½Ρ Π· ΠΌΠ΅ΡΠΎΡ ΠΏΡΠΎΡΡΠ»Π°ΠΊΡΠΈΠΊΠΈ Π·Π°Ρ
Π²ΠΎΡΡΠ²Π°Π½Ρ ΡΠΊΠ°Π½ΠΈΠ½ ΠΏΠ°ΡΠΎΠ΄ΠΎΠ½ΡΠ°
Resonant nonlinear magneto-optical effects in atoms
In this article, we review the history, current status, physical mechanisms,
experimental methods, and applications of nonlinear magneto-optical effects in
atomic vapors. We begin by describing the pioneering work of Macaluso and
Corbino over a century ago on linear magneto-optical effects (in which the
properties of the medium do not depend on the light power) in the vicinity of
atomic resonances, and contrast these effects with various nonlinear
magneto-optical phenomena that have been studied both theoretically and
experimentally since the late 1960s. In recent years, the field of nonlinear
magneto-optics has experienced a revival of interest that has led to a number
of developments, including the observation of ultra-narrow (1-Hz)
magneto-optical resonances, applications in sensitive magnetometry, nonlinear
magneto-optical tomography, and the possibility of a search for parity- and
time-reversal-invariance violation in atoms.Comment: 51 pages, 23 figures, to appear in Rev. Mod. Phys. in Oct. 2002,
Figure added, typos corrected, text edited for clarit
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