335 research outputs found
On unbalanced Boolean functions with best correlation immunity
It is known that the order of correlation immunity of a nonconstant
unbalanced Boolean function in variables cannot exceed ; moreover,
it is if and only if the function corresponds to an equitable
-partition of the -cube with an eigenvalue of the quotient matrix.
The known series of such functions have proportion , , or of
the number of ones and zeros. We prove that if a nonconstant unbalanced Boolean
function attains the correlation-immunity bound and has ratio of the
number of ones and zeros, then is divisible by . In particular, this
proves the nonexistence of equitable partitions for an infinite series of
putative quotient matrices. We also establish that there are exactly
equivalence classes of the equitable partitions of the -cube with quotient
matrix and classes, with . These
parameters correspond to the Boolean functions in variables with
correlation immunity and proportion and , respectively (the case
remains unsolved). This also implies the characterization of the
orthogonal arrays OA and OA.Comment: v3: final; title changed; revised; OA(512,11,2,6) discusse
Characteristics of water and ion exchange of Elodea nuttallii cells at high concentrations of lanthanides
Β© 2016 Elsevier LtdChanges of diffusive permeability of membranes of Elodea nuttallii cells following a short-term (60Β min) treatment with high concentrations of lanthanides were recorded by the 1H NMR-diffusometry and conductometry methods. The 1-h infiltration of segments of Elodea nuttallii internodes in 10Β mM solutions of nitrates of La, Nd and Lu resulted in the increased leakage of electrolytes from cells, but has no effect on a water diffusive permeability of membranes. In samples subjected to a 30Β min pretreatment with a water channel inhibitor HgCl2 the water diffusive permeability of membranes (Pd) drops down under the influence of lanthanides, as well as an outcome of electrolytes. To explain the observed effects the change of spontaneous curvature of membrane lipid layer has been taken into consideration. The interaction of lanthanides with lipids of plasmalemma leads to the negative spontaneous curvature of lipid layer at which membrane channels are unclosed. Blocking of the ionic and water channels by mercury ions compensate the effect of change of spontaneous curvature of lipid layer
Magneto-gyrotropic effects in semiconductor quantum wells (review)
Magneto-gyrotropic photogalvanic effects in quantum wells are reviewed. We
discuss experimental data, results of phenomenological analysis and microscopic
models of these effects. The current flow is driven by spin-dependent
scattering in low-dimensional structures gyrotropic media resulted in asymmetry
of photoexcitation and relaxation processes. Several applications of the
effects are also considered.Comment: 28 pages, 13 figure
Navedennoe pogloΕenie nakaΔki, porog generacii i kpd lazerov na rastvorah organiΔeskih soedinenij
Case of insulinoma detected in a patient after bariatric operation for morbid obesity
The prevalence of insulinomas is 1–3 cases per million population per year of which 4–14% tumor is malignant. Weight gain is one of the symptoms of the disease, often resulting in morbid obesity with indications for surgical treatment. The presented clinical case demonstrates the successful treatment of malignant insulinoma with the manifestation of hypoglycemic syndrome after carrying out biliopancreatic bypass with longitudinal gastrectomy for morbid obesity
Gravitational Couplings of Intrinsic Spin
The gravitational couplings of intrinsic spin are briefly reviewed. A
consequence of the Dirac equation in the exterior gravitational field of a
rotating mass is considered in detail, namely, the difference in the energy of
a spin-1/2 particle polarized vertically up and down near the surface of a
rotating body is . Here is the latitude and
, where and are, respectively, the angular
momentum and radius of the body. It seems that this relativistic quantum
gravitational effect could be measurable in the foreseeable future.Comment: LaTeX file, no figures, 16 page
Geoantineutrino Spectrum, 3He/4He-ratio Distribution in the Earth's Interior and Slow Nuclear Burning on the Boundary of the Liquid and Solid Phases of the Earth's Core
The description problem of geoantineutrino spectrum and reactor antineutrino
experimental spectrum in KamLAND, which takes place for antineutrino energy
\~2.8 MeV, and also the experimental results of the interaction of uranium
dioxide and carbide with iron-nickel and silicaalumina melts at high pressure
(5-10 GP?) and temperature (1600-2200C) have motivated us to consider the
possible consequences of the assumption made by V.Anisichkin and coauthors that
there is an actinid shell on boundary of liquid and solid phases of the Earth's
core. We have shown that the activation of a natural nuclear reactor operating
as the solitary waves of nuclear burning in 238U- and/or 232Th-medium (in
particular, the neutron- fission progressive wave of Feoktistov and/or
Teller-Ishikawa-Wood) can be such a physical consequence. The simplified model
of the kinetics of accumulation and burnup in U-Pu fuel cycle of Feoktistov is
developed. The results of the numerical simulation of neutron-fission wave in
two-phase UO2/Fe medium on a surface of the Earth's solid core are presented.
The georeactor model of 3He origin and the 3He/4He-ratio distribution in the
Earth's interior is offered. It is shown that the 3He/4He ratio distribution
can be the natural quantitative criterion of georeactor thermal power. On the
basis of O'Nions-Evensen-Hamilton geochemical model of mantle differentiation
and the crust growth supplied by actinid shell on the boundary of liquid and
solid phases of the Earth's core as a nuclear energy source (georeactor with
power of 30 TW), the tentative estimation of geoantineutrino intensity and
geoantineutrino spectrum on the Earth surface are given.Comment: 28 pages, 12 figures. Added text, formulas, figures and references.
Corrected equations. Changed content of some section
The Hamiltonian Structure of the Second Painleve Hierarchy
In this paper we study the Hamiltonian structure of the second Painleve
hierarchy, an infinite sequence of nonlinear ordinary differential equations
containing PII as its simplest equation. The n-th element of the hierarchy is a
non linear ODE of order 2n in the independent variable depending on n
parameters denoted by and . We introduce new
canonical coordinates and obtain Hamiltonians for the and
evolutions. We give explicit formulae for these Hamiltonians showing that they
are polynomials in our canonical coordinates
Non-invasive comprehensive laboratory and ultrasound method for the evaluation of the functional status of the liver in patients with type 2 diabetes mellitus
The article analyzes the methods of assessment of fatty infiltration of the liver in patients with type 2 diabetes and a new non-invasive method using laboratory, echohepatodensitographic and tomographic study options. Discriminant models are developed which are used as variables in the values activity of aspartate aminotransferase, gamma-glutamiltranspeptidase, coefficient of density of the tissue in the anterior surface of the liver in echohepatodensitographic study, the density of the liver in tomographic ones study. Using the model, you can define the degree of steatoinfiltration of the liver from minimal to marked. The greatest impact of the classification in the model had the density of the liver determined by tomographic ones and echohepatodensitographicstudy.Π ΡΡΠ°ΡΡΠ΅ ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Ρ ΠΌΠ΅ΡΠΎΠ΄Ρ ΠΎΡΠ΅Π½ΠΊΠΈ ΠΆΠΈΡΠΎΠ²ΠΎΠΉ ΠΈΠ½ΡΠΈΠ»ΡΡΡΠ°ΡΠΈΠΈ ΠΏΠ΅ΡΠ΅Π½ΠΈ Ρ Π±ΠΎΠ»ΡΠ½ΡΡ
ΡΠ°Ρ
Π°ΡΠ½ΡΠΌ Π΄ΠΈΠ°Π±Π΅ΡΠΎΠΌ 2 ΡΠΈΠΏΠ° ΠΈ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ Π½ΠΎΠ²ΡΠΉ Π½Π΅ΠΈΠ½Π²Π°Π·ΠΈΠ²Π½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠ½ΡΡ
, ΡΡ
ΠΎΠ³Π΅ΠΏΠ°ΡΠΎΠ΄Π΅Π½ΡΠΈΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΡΠΎΠΌΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½Ρ Π΄ΠΈΡΠΊΡΠΈΠΌΠΈΠ½Π°Π½ΡΠ½ΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ, Π³Π΄Π΅ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΏΠ΅ΡΠ΅ΠΌΠ΅Π½Π½ΡΡ
ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΡΡΡΡ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π°ΡΠΏΠ°ΡΡΠ°ΡΠ°ΠΌΠΈΠ½ΠΎΡΡΠ°Π½ΡΡΠ΅ΡΠ°Π·Ρ, Π³Π°ΠΌΠΌΠ°-Π³Π»ΡΡΠ°ΠΌΠΈΠ»ΡΡΠ°Π½ΡΠΏΠ΅ΠΏΡΠΈΠ΄Π°Π·Ρ, ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ ΡΠΊΠ°Π½ΠΈ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΠΏΠ΅ΡΠ΅Π΄Π½Π΅ΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΏΠ΅ΡΠ΅Π½ΠΈ ΠΏΡΠΈ ΡΡ
ΠΎΠ³Π΅ΠΏΠ°ΡΠΎΠ΄Π΅Π½ΡΠΈΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ,ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ ΠΏΠ΅ΡΠ΅Π½ΠΈ ΠΏΡΠΈ ΡΠΎΠΌΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ. ΠΡΠΏΠΎΠ»ΡΠ·ΡΡ ΠΌΠΎΠ΄Π΅Π»ΠΈ, ΠΌΠΎΠΆΠ½ΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΡΡ ΡΡΠ΅ΠΏΠ΅Π½Ρ ΠΆΠΈΡΠΎΠ²ΠΎΠΉ ΠΈΠ½ΡΠΈΠ»ΡΡΡΠ°ΡΠΈΠΈ ΠΏΠ΅ΡΠ΅Π½ΠΈ ΠΎΡ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡΠ½ΠΎΠΉ Π΄ΠΎ Π²ΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠΉ. ΠΠ°ΠΈΠ±ΠΎΠ»ΡΡΠ΅Π΅ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π² ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠΌΠ΅Π»Π° Π²Π΅Π»ΠΈΡΠΈΠ½Π° ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ ΠΏΠ΅ΡΠ΅Π½ΠΈ, ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΠΌΠ°Ρ ΠΏΡΠΈ ΡΠΎΠΌΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈ Π·Ρ
ΠΎΠ΄Π΅Π½ΡΠΈΡΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ
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