359 research outputs found
Spectral and Nonlinear Properties of the Sum of Boolean Functions
Boolean functions are the mathematical basis of modern cryptographic algorithms. However, in practice, a set of interrelated Boolean functions is often used to construct a cryptographic algorithm. This circumstance makes the task of research of cryptographic quality, in particular, the distance of the nonlinearity of the sum of few Boolean functions important. The nonlinearity distance of a Boolean function is determined by the maximum value of its Walsh-Hadamard transform coefficients. In this paper, we proposed a formula that is the equivalent of the summation of Boolean functions in the Walsh-Hadamard transform domain. The application of this formula, as well as the Walsh-Hadamard spectral classification made it possible to determine the structure of WalshHadamard transform coefficients, and the distance of the nonlinearity when summing the Boolean functions lengths N 8 and N 16 , indicating valuable practical application for information protection
Non-linear Supersymmetry for non-Hermitian, non-diagonalizable Hamiltonians: II. Rigorous results
We continue our investigation of the nonlinear SUSY for complex potentials
started in the Part I (math-ph/0610024) and prove the theorems characterizing
its structure in the case of non-diagonalizable Hamiltonians. This part
provides the mathematical basis of previous studies. The classes of potentials
invariant under SUSY transformations for non-diagonalizable Hamiltonians are
specified and the asymptotics of formal eigenfunctions and associated functions
are derived. Several results on the normalizability of associated functions at
infinities are rigorously proved. Finally the Index Theorem on relation between
Jordan structures of intertwined Hamiltonians depending of the behavior of
elements of canonical basis of supercharge kernel at infinity is proven.Comment: 31 pp., comments on PT symmetry and few relevant refs are adde
Fractional Diffusion Equation for a Power-Law-Truncated Levy Process
Truncated Levy flights are stochastic processes which display a crossover
from a heavy-tailed Levy behavior to a faster decaying probability distribution
function (pdf). Putting less weight on long flights overcomes the divergence of
the Levy distribution second moment. We introduce a fractional generalization
of the diffusion equation, whose solution defines a process in which a Levy
flight of exponent alpha is truncated by a power-law of exponent 5 - alpha. A
closed form for the characteristic function of the process is derived. The pdf
of the displacement slowly converges to a Gaussian in its central part showing
however a power law far tail. Possible applications are discussed
Energy State of a Plastically Deformed Surface Layer
AbstractThe paper reports the results of experimental research on the substantiation of the criterion for steel strengthening effectiveness established on a basis of an energetic approach to the consideration of the mechanism for the surface layer formation with dynamic methods of plastic forming. Using the analogy between the processes of energy absorption of the crystal lattice under mechanical loading and under heating, the work demonstrates that the maximum specific energy which can absorb the crystal lattice corresponds to the value equal to the difference between the heat content (enthalpy) of the material in the solid state, at the melting temperature and enthalpy H_TS at 2930Π. The proposed method and experimental device allowing to estimate the stored energy in the plastically deformed surface layer as the difference between the work expended in plastic deformation of the material and the quantity of the released heat. It was established that the energy growth limit in the local plastically deformed volume of a surface occurs at making of 11-13 acts of the action force; the further increase in acts influences the energy state of the surface as it becomes stabilized
ΠΡΠΎΠ³ΡΠ°ΠΌΠΌΠ½ΡΠ΅ ΡΠ²ΡΠ·ΠΈ ΠΈ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΠ΅ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ΅Ρ Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠ°Π½ΠΈΠΏΡΠ»ΡΡΠΎΡΠ°
For the theoretical study of the dynamics of manipulation robots, define design parameters and control laws, you must have a current mechanical models that accurately describe the properties of real robots. The choice of the computational model in each case is determined by the kinematic scheme of the manipulator, mechanical properties (inertial, elastic, dissipative, and the like) parts and assemblies, type and characteristics of the drives, as well as the required accuracy of the calculation. The objective of the control is to ensure the motion of the mechanical system under some requirements that make up its program. Program motion of the system can be performed by the application to the system of control of forces, the system settings change in the process, building of special control devices (controllers) or a combination of these. The original objectives of the control theory are inverse problems of classical dynamics. From the mathematical point of view, calculation model manipulation robot is a system of differential equations. This model may include equations describing the phenomena non-mechanical nature, for example, electrical processes in the circuits of the motors of the actuators. In this article the author examines the issues of ensuring conditions of the asymptotic stability software movement mechanical and electromechanical systems with holonomic and nonholonomic constraints. For example, the three-tier model controllable electromechanical manipulator conditions of the asymptotic stability of a given movement. The described approaches to ensuring the asymptotic stability of electromechanical systems can be used in the study of stability of motion proprietary mechanical systems, mechanics of controlled motion in the solution of management tasks manipulators, transport and space systems.ΠΠ»Ρ ΡΠ΅ΠΎΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·ΡΡΠ΅Π½ΠΈΡ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ ΠΌΠ°Π½ΠΈΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΡΡ
ΡΠΎΠ±ΠΎΡΠΎΠ², ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠ²Π½ΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΈ Π·Π°ΠΊΠΎΠ½ΠΎΠ² ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ ΠΈΠΌΠ΅ΡΡ ΡΠ°ΡΡΡΡΠ½ΡΠ΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ, Ρ Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΠΉ ΡΠΎΡΠ½ΠΎΡΡΡΡ ΠΎΠΏΠΈΡΡΠ²Π°ΡΡΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΡΠ΅Π°Π»ΡΠ½ΡΡ
ΡΠΎΠ±ΠΎΡΠΎΠ². ΠΡΠ±ΠΎΡ ΡΠ°ΡΡΡΡΠ½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ Π² ΠΊΠ°ΠΆΠ΄ΠΎΠΌ ΠΊΠΎΠ½ΠΊΡΠ΅ΡΠ½ΠΎΠΌ ΡΠ»ΡΡΠ°Π΅ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ ΠΊΠΈΠ½Π΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡ
Π΅ΠΌΠΎΠΉ ΠΌΠ°Π½ΠΈΠΏΡΠ»ΡΡΠΎΡΠ°, ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ²ΠΎΠΉΡΡΠ²Π°ΠΌΠΈ (ΠΈΠ½Π΅ΡΡΠΈΠΎΠ½Π½ΡΠΌΠΈ, ΡΠΏΡΡΠ³ΠΈΠΌΠΈ, Π΄ΠΈΡΡΠΈΠΏΠ°ΡΠΈΠ²Π½ΡΠΌΠΈ ΠΈ Ρ.ΠΏ.) Π΅Π³ΠΎ Π΄Π΅ΡΠ°Π»Π΅ΠΉ ΠΈ ΡΠ·Π»ΠΎΠ², ΡΠΈΠΏΠΎΠΌ ΠΈ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°ΠΌΠΈ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΎΠ², Π° ΡΠ°ΠΊΠΆΠ΅ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΠΉΡΠΎΡΠ½ΠΎΡΡΡΡ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΡΡ
ΡΠ°ΡΡΡΡΠΎΠ². ΠΠ°Π΄Π°ΡΠ΅ΠΉ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΠ΅ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΡΠΎΠ³Π»Π°ΡΠ½ΠΎ Π½Π΅ΠΊΠΎΡΠΎΡΡΠΌ ΡΡΠ΅Π±ΠΎΠ²Π°Π½ΠΈΡΠΌ, ΠΊΠΎΡΠΎΡΡΠ΅ ΡΠΎΡΡΠ°Π²Π»ΡΡΡ Π΅Ρ ΠΏΡΠΎΠ³ΡΠ°ΠΌΠΌΡ. ΠΡΠΎΠ³ΡΠ°ΠΌΠΌΠ½ΠΎΠ΅ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΠΈΡΡΠ΅ΠΌΡ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΎΡΡΡΠ΅ΡΡΠ²Π»Π΅Π½ΠΎ ΠΏΡΠΈΠ»ΠΎΠΆΠ΅Π½ΠΈΠ΅ΠΌ ΠΊ ΡΠΈΡΡΠ΅ΠΌΠ΅ ΡΠΏΡΠ°Π²Π»ΡΡΡΠΈΡ
ΡΠΈΠ», ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠΈΡΡΠ΅ΠΌΡ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ, ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΠ΅ΠΌ ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΡΡ
ΡΠΏΡΠ°Π²Π»ΡΡΡΠΈΡ
ΡΡΡΡΠΎΠΉΡΡΠ² (ΡΠ΅Π³ΡΠ»ΡΡΠΎΡΠΎΠ²) ΠΈΠ»ΠΈ ΡΠΎΡΠ΅ΡΠ°Π½ΠΈΠ΅ΠΌ ΡΡΠΈΡ
Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠ΅ΠΉ. ΠΡΡ
ΠΎΠ΄Π½ΡΠΌΠΈ Π·Π°Π΄Π°ΡΠ°ΠΌΠΈ ΡΠ΅ΠΎΡΠΈΠΈ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΠ²Π»ΡΡΡΡΡ ΠΎΠ±ΡΠ°ΡΠ½ΡΠ΅ Π·Π°Π΄Π°ΡΠΈ ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ. Π‘ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΡΠΊΠΈ Π·ΡΠ΅Π½ΠΈΡ ΡΠ°ΡΡΡΡΠ½Π°Ρ ΠΌΠΎΠ΄Π΅Π»Ρ ΠΌΠ°Π½ΠΈΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠΎΠ±ΠΎΡΠ° ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΡΠΎΠ±ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ. ΠΡΠ° ΠΌΠΎΠ΄Π΅Π»Ρ ΠΌΠΎΠΆΠ΅Ρ ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ, ΠΎΠΏΠΈΡΡΠ²Π°ΡΡΠΈΠ΅ ΡΠ°ΠΊΠΆΠ΅ ΡΠ²Π»Π΅Π½ΠΈΡ Π½Π΅ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠΈΡΠΎΠ΄Ρ, Π½Π°ΠΏΡΠΈΠΌΠ΅Ρ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ Π² ΡΠ΅ΠΏΡΡ
ΡΠ»Π΅ΠΊΡΡΠΎΠ΄Π²ΠΈΠ³Π°ΡΠ΅Π»Π΅ΠΉ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΎΠ². Π Π΄Π°Π½Π½ΠΎΠΉ ΡΡΠ°ΡΡΠ΅ Π°Π²ΡΠΎΡΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΡΡΡΡΡ Π²ΠΎΠΏΡΠΎΡΡ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π°ΡΠΈΠΌΠΏΡΠΎΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ ΠΏΡΠΎΠ³ΡΠ°ΠΌΠΌΠ½ΠΎΠ³ΠΎ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ Ρ Π³ΠΎΠ»ΠΎΠ½ΠΎΠΌΠ½ΡΠΌΠΈ ΠΈ Π½Π΅Π³ΠΎΠ»ΠΎΠ½ΠΎΠΌΠ½ΡΠΌΠΈ ΡΠ²ΡΠ·ΡΠΌΠΈ. ΠΠ° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΡΡΡΡ
Π·Π²Π΅Π½Π½ΠΎΠ³ΠΎ ΡΠΏΡΠ°Π²Π»ΡΠ΅ΠΌΠΎΠ³ΠΎ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠ°Π½ΠΈΠΏΡΠ»ΡΡΠΎΡΠ° ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°ΡΡΡΡ ΡΡΠ»ΠΎΠ²ΠΈΡ Π°ΡΠΈΠΌΠΏΡΠΎΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ Π·Π°Π΄Π°Π½Π½ΠΎΠ³ΠΎ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ. ΠΠΏΠΈΡΡΠ²Π°Π΅ΠΌΡΠ΅ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Ρ ΠΊ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π°ΡΠΈΠΌΠΏΡΠΎΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ ΠΏΡΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ Π½Π΅ΡΠ²ΠΎΠ±ΠΎΠ΄Π½ΡΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ, Π² ΠΌΠ΅Ρ
Π°Π½ΠΈΠΊΠ΅ ΡΠΏΡΠ°Π²Π»ΡΠ΅ΠΌΠΎΠ³ΠΎ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ, ΠΏΡΠΈ ΡΠ΅ΡΠ΅Π½ΠΈΠΈ Π·Π°Π΄Π°Ρ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΠΎΠ±ΠΎΡΠ°ΠΌΠΈ-ΠΌΠ°Π½ΠΈΠΏΡΠ»ΡΡΠΎΡΠ°ΠΌΠΈ, ΡΡΠ°Π½ΡΠΏΠΎΡΡΠ½ΡΠΌΠΈ ΠΈ ΠΊΠΎΡΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠΈΡΡΠ΅ΠΌΠ°ΠΌΠΈ
Investigation of Microstructure of Oxygen-Containing Copper
The results of the study of fine structure of continuous casted bars of oxygen-containing copper produced by casting in the belt water-cooled crystallizer are presented. The character of fractures of samples of copper cast bars in different directions depending on technological parameters of continuous casting was investigated. For determination of chemical composition of samples of cast bars and detection of presence of possible impurities in copper the microspectral analysis was carried out. It is shown that removing of sources of gasing of copper melt leads to decreasing of volume fraction of eutectic Cu-Cu2O, discontinuity flaws and pores in the structure of cast bars.
Keywords: Copper, Continuos casting, Rolling, Rolled wire, Contirod method, Microstructure, Fracture, Microspectral analysis
Construction Method for Infinite Families of Bent Sequences
Bent-sequences is one of the most important classes of Boolean functions, which are widely used in modern cryptographic algorithms, and telecommunication systems that are based on CDMA and OFDM standards. The problem of synthesis of bent-sequences of large lengths is actual and widely discussed. However, in view of the high complexity and unpredictability of the class of bent-sequences, the creation of methods for their synthesis faces significant difficulties. In this paper, a recursive method for constructing infinite families of bent-sequences, based on easily synthesized bent-sequences of small length, has been developed. As the basis of this method, the operations of interleaving of elements and strings, which are widely used in the theory of synthesis of perfect binary arrays, are applied. Effective reproduction rules for bent-sequences in the time domain based on the operation of rearrangement of segments, a rotor, and dimensional changes are proposed. The method developed allows rapid acquisition of a lot of bentsequences of any predefined length. Moreover, the obtained bent-sequences belong to different classes according to Agievich classification, which is important from the cryptographic point of view
Hidden Symmetry from Supersymmetry in One-Dimensional Quantum Mechanics
When several inequivalent supercharges form a closed superalgebra in Quantum Mechanics it entails the appearance of hidden symmetries of a Super-Hamiltonian. We examine this problem in one-dimensional QM for the case of periodic potentials and potentials with finite number of bound states. After the survey of the results existing in the subject the algebraic and analytic properties of hidden-symmetry differential operators are rigorously elaborated in the Theorems and illuminated by several examples
The Poisson bracket compatible with the classical reflection equation algebra
We introduce a family of compatible Poisson brackets on the space of polynomial matrices, which contains the reflection equation algebra bracket.
Then we use it to derive a multi-Hamiltonian structure for a set of integrable
systems that includes the Heisenberg magnet with boundary conditions, the
generalized Toda lattices and the Kowalevski top.Comment: 13 pages, LaTeX with AmsFont
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