154 research outputs found
Decay of metastable current states in one-dimensional resonant tunneling devices
Current switching in a double-barrier resonant tunneling structure is studied
in the regime where the current-voltage characteristic exhibits intrinsic
bistability, so that in a certain range of bias two different steady states of
current are possible. Near the upper boundary V_{th} of the bistable region the
upper current state is metastable, and because of the shot noise it eventually
decays to the stable lower current state. We find the time of this switching
process in strip-shaped devices, with the width small compared to the length.
As the bias V is tuned away from the boundary value V_{th} of the bistable
region, the mean switching time \tau increases exponentially. We show that in
long strips \ln\tau \propto (V_{th} -V)^{5/4}, whereas in short strips \ln\tau
\propto (V_{th} -V)^{3/2}. The one-dimensional geometry of the problem enables
us to obtain analytically exact expressions for both the exponential and the
prefactor of \tau. Furthermore, we show that, depending on the parameters of
the system, the switching can be initiated either inside the strip, or at its
ends.Comment: 12 pages, 5 figures, update to published versio
Stochastic current switching in bistable resonant tunneling systems
Current-voltage characteristics of resonant-tunneling structures often
exhibit intrinsic bistabilities. In the bistable region of the I-V curve one of
the two current states is metastable. The system switches from the metastable
state to the stable one at a random moment in time. The mean switching time
\tau depends exponentially on the bias measured from the boundary of the
bistable region V_{th}. We find full expressions for \tau (including
prefactors) as functions of bias, sample geometry, and in-plane conductivity.
Our results take universal form upon appropriate renormalization of the
threshold voltage V_{th}. We also show that in large samples the switching
initiates inside, at the edge, or at a corner of the sample depending on the
parameters of the system.Comment: 21 pages, 5 figure
Magnetic system for cleaning the gamma beam at the LUE-40 electron linac output
The bremsstrahlung of accelerated electrons passing through a converter is
used to study multiparticle photo-nuclear reactions. The results of
calculations, numerical modeling, design, and testing of a special magnetic
cleaning system to obtain a "pure" beam of bremsstrahlung quanta when studying
the cross-sections of such reactions at the LUE-40 linac are presented. The
system is based on commercially available permanent magnets of rectangular
cross-sections. The maximum on-axis field is 0.9 T, which provides sufficient
separation of the electron beam and gamma rays at a distance of more than 90 mm
from the magnet.Comment: 9 pages, 8 figure
Influence of boric anhydride upon the physical and chemical properties of ferrosilicon slag
The authors study the influence of boric anhydride upon the physical and chemical properties of slag in the manufacture of ferrosilicon. It is established that adding boric anhydride to the slag changes its refractory quality and its viscosity and eases pouring slag and metal. Slags with optimal composition and properties are described
Structural data of phenanthrene-9,10-dicarbonitriles
In this data article, we present the single-crystal XRD data of phenanthrene-9,10-dicarbonitriles. Detailed structure analysis and photophysical properties were discussed in our previous study, "Intermolecular interactions-photophysical properties relationships in phenanthrene-9,10-dicarbonitrile assemblies" (Afanasenko et al., 2020). The data include the intra- and intermolecular bond lengths and angles. (c) 2019 The Author(s). Published by Elsevier Inc. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/)
Immune mechanisms of the regulation of fetoplacental complex development
The aim of the research: the evaluation of the prognostic significance of the estimation of cytokines, growth factors and vasoactive regulators in the development of fetoplacental hemodynamic damage and fetoplacental insufficiency. 57 women in progress of physiological and pathological pregnancy were examined. The main group consisted of 45 women with evident FPI in the second half of pregnancy: 17 women with compensated FPI, 15 women with subcompensated FPI accompanied by IUGR without hemodynamic problems and 13 women with subcompensated FPI accompanied by IUGR with compromised utero-placental blood flow. It has been found that the first trimester of pregnancy complicated by FPI, is characterized by the decreased production of angiogenic factors and increased levels of proinflammatory, including angiogenesis inhibitors, and markers of vasoconstriction and endothelium dysfunction. Change-over to Th1 type of immune reaction and disturbance of trophoblast invasion and placentation due to interferons hyrerproduction and deficiency of hemopoetic growth factors and receptors for them may lead to FPI development. The degree of the depression of the growth factors production directly depends on the activity if compensation processes in FPI. The damage of vascular endothelium may leads to the decrease of angiogenesis because of the decreased production of growth factors and restricted endotheliocytes sensitivity towards proangiogenic stimuli.Π¦Π΅Π»ΡΡ ΡΠ°Π±ΠΎΡΡ ΡΠ²ΠΈΠ»Π°ΡΡ ΠΎΡΠ΅Π½ΠΊΠ° ΠΏΡΠΎΠ³Π½ΠΎΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π·Π½Π°ΡΠΈΠΌΠΎΡΡΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΠΈΡΠΎΠΊΠΈΠ½ΠΎΠ², ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΡΠΎΡΡΠ° ΠΈ Π²Π°Π·ΠΎΠ°ΠΊΡΠΈΠ²Π½ΡΡ
ΡΠ΅Π³ΡΠ»ΡΡΠΎΡΠΎΠ² Π² ΡΠ°Π·Π²ΠΈΡΠΈΠΈ Π½Π°ΡΡΡΠ΅Π½ΠΈΠΉ Π³Π΅ΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ ΡΠ΅ΡΠΎΠΏΠ»Π°ΡΠ΅Π½ΡΠ°ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ° ΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ Π€ΠΠ. ΠΠ±ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΎ 57 ΠΆΠ΅Π½ΡΠΈΠ½ Π² Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ΅ ΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈ ΠΈ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈ ΠΏΡΠΎΡΠ΅ΠΊΠ°ΡΡΠ΅ΠΉ Π±Π΅ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΡΡΠΈ. ΠΡΠ½ΠΎΠ²Π½ΡΡ Π³ΡΡΠΏΠΏΡ ΡΠΎΡΡΠ°Π²ΠΈΠ»ΠΈ 45 ΠΆΠ΅Π½ΡΠΈΠ½ Ρ ΠΌΠ°Π½ΠΈΡΠ΅ΡΡΠ°ΡΠΈΠ΅ΠΉ Π€ΠΠ Π²ΠΎ Π²ΡΠΎΡΠΎΠΉ ΠΏΠΎΠ»ΠΎΠ²ΠΈΠ½Π΅ Π±Π΅ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΡΡΠΈ: 17 ΠΆΠ΅Π½ΡΠΈΠ½ Ρ ΠΊΠΎΠΌΠΏΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠΎΡΠΌΠΎΠΉ Π€ΠΠ, 15 ΠΆΠ΅Π½ΡΠΈΠ½ Ρ ΡΡΠ±ΠΊΠΎΠΌΠΏΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠΎΡΠΌΠΎΠΉ Π€ΠΠ, ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°Π²ΡΠ΅ΠΉΡΡ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ΠΌ Π‘ΠΠ Π Π±Π΅Π· Π³Π΅ΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
Π½Π°ΡΡΡΠ΅Π½ΠΈΠΉ ΠΈ 13 ΠΆΠ΅Π½ΡΠΈΠ½ Ρ ΡΡΠ±ΠΊΠΎΠΌΠΏΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠΎΡΠΌΠΎΠΉ Π€ΠΠ, ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°Π²ΡΠ΅ΠΉΡΡ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ΠΌ Π‘ΠΠ Π Ρ Π½Π°ΡΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΌΠ°ΡΠΎΡΠ½ΠΎ-ΠΏΠ»Π°ΡΠ΅Π½ΡΠ°ΡΠ½ΠΎΠ³ΠΎ ΠΊΡΠΎΠ²ΠΎΡΠΎΠΊΠ°. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΏΠ΅ΡΠ²ΡΠΉ ΡΡΠΈΠΌΠ΅ΡΡΡ Π±Π΅ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΡΡΠΈ, ΠΎΡΠ»ΠΎΠΆΠ½ΠΈΠ²ΡΠ΅ΠΉΡΡ Π²ΠΏΠΎΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠΈ Π€ΠΠ, Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅ΡΡΡ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΡΠΎΠ΄ΡΠΊΡΠΈΠΈ Π°Π½Π³ΠΈΠΎΠ³Π΅Π½Π½ΡΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ², ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΡΠΎΠ²Π½Ρ ΠΏΡΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΡΠΈΡΠΎΠΊΠΈΠ½ΠΎΠ², Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΠΎΠ² Π°Π½Π³ΠΈΠΎΠ³Π΅Π½Π΅Π·Π°, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΌΠ°ΡΠΊΠ΅ΡΠΎΠ² Π²Π°Π·ΠΎΠΊΠΎΠ½ΡΡΡΠΈΠΊΡΠΈΠΈ ΠΈ Π΄ΠΈΡΡΡΠ½ΠΊΡΠΈΠΈ ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΡ. Π Π°Π·Π²ΠΈΡΠΈΡ Π€ΠΠ ΠΌΠΎΠΆΠ΅Ρ ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΠΎΠ²Π°ΡΡ Π½Π΅ ΡΠΎΠ»ΡΠΊΠΎ ΠΏΠ΅ΡΠ΅ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅ Π½Π° ΠΈΠΌΠΌΡΠ½Π½ΡΠΉ ΠΎΡΠ²Π΅Ρ Th 1 βΡΠΈΠΏΠ°, Π½ΠΎ ΠΈ Π½Π°ΡΡΡΠ΅Π½ΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² ΠΈΠ½Π²Π°Π·ΠΈΠΈ ΡΡΠΎΡΠΎΠ±Π»Π°ΡΡΠ° ΠΈ ΠΏΠ»Π°ΡΠ΅Π½ΡΠ°ΡΠΈΠΈ, ΡΠ²ΡΠ·Π°Π½Π½ΠΎΠ΅ Ρ Π³ΠΈΠΏΠ΅ΡΠΏΡΠΎΠ΄ΡΠΊΡΠΈΠ΅ΠΉ ΠΈΠ½ΡΠ΅ΡΡΠ΅ΡΠΎΠ½ΠΎΠ² ΠΈ Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΠΉ Π²ΡΡΠ°Π±ΠΎΡΠΊΠΎΠΉ Π³Π΅ΠΌΠΎΠΏΠΎΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΡΠΎΡΡΠ° ΠΈ ΡΠ΅ΡΠ΅ΠΏΡΠΎΡΠΎΠ² ΠΊ Π½ΠΈΠΌ. Π‘ΡΠ΅ΠΏΠ΅Π½Ρ ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΡ ΠΏΡΠΎΠ΄ΡΠΊΡΠΈΠΈ ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΡΠΎΡΡΠ° Π½Π°Ρ
ΠΎΠ΄ΠΈΡΡΡ Π² ΠΏΡΡΠΌΠΎΠΉ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ Π²ΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΡΡΠΈ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² ΠΊΠΎΠΌΠΏΠ΅Π½ΡΠ°ΡΠΈΠΈ ΠΏΡΠΈ Π€ΠΠ. ΠΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΠ΅ ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΡ ΡΠΎΡΡΠ΄ΠΎΠ² ΠΌΠΎΠΆΠ΅Ρ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡΡ ΠΊ ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΡ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² Π°Π½Π³ΠΈΠΎΠ³Π΅Π½Π΅Π·Π° Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΠΏΡΠΎΠ΄ΡΠΊΡΠΈΠΈ ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΡΠΎΡΡΠ° ΠΈ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΠΎΡΠΈΡΠΎΠ² ΠΊ ΠΏΡΠΎΠ°Π½Π³ΠΈΠΎΠ³Π΅Π½Π½ΡΠΌ ΡΡΠΈΠΌΡΠ»Π°ΠΌ
Fluctuation corrections to bubble nucleation
The fluctuation determinant which determines the preexponential factor of the
transition rate for minimal bubbles is computed for the electroweak theory with
. As the basic action we use the three-dimensional
high-temperature action including, besides temperature dependent masses, the one-loop contribution which makes the phase transition first order. The
results show that this contribution (which has then to be subtracted from the
exact result) gives the dominant contribution to the one-loop effective action.
The remaining correction is of the order of, but in general larger than the
critical bubble action and suppresses the transition rate. The results for the
Higgs field fluctuations are compared with those of an approximate heat kernel
computation of Kripfganz et al., good agreement is found for small bubbles,
strong deviations for large thin-wall bubbles.Comment: 19 pages, LaTeX, no macros, no figure
A search for two body muon decay signals
Lepton family number violation is tested by searching for
decays among the 5.8 positive muon decay events analyzed by the
TWIST collaboration. Limits are set on the production of both massless and
massive bosons. The large angular acceptance of this experiment allows
limits to be placed on anisotropic decays, which can arise
from interactions violating both lepton flavor and parity conservation.
Branching ratio limits of order are obtained for bosons with masses
of 13 - 80 MeV/c and with different decay asymmetries. For bosons with
masses less than 13 MeV/c the asymmetry dependence is much stronger and
the 90% limit on the branching ratio varies up to . This is
the first study that explicitly evaluates the limits for anisotropic two body
muon decays.Comment: 7 pages, 5 figures, 2 tables, accepted by PR
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