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Testing the sign-definiteness of forms-dimensional quadratic forms and forms of the fourth degree we propose using classical methods of unconstrained
Refined geometrically nonlinear equations of motion for elongated rod-type plate. These equations allow to describe the high-frequency torsional oscillation of elongated rod-type plate formed
A study of one class of NLP problems arising in parametric Semi-Infinite Programming of integers (parameters). This problem has a special form, and arises as an auxiliary problem in study
A note on the properties of associated Boolean functions of quadratic APN functionsLet F be a quadratic APN function in n variables. The associated Boolean function yf in 2n
Properties of associated Boolean functions of quadratic APN functions at most 2 solutions for all vectors a, b 6 F2n, where a is nonzero. In case when F is a quadratic APN
One-dimensional Fokker-Planck equation with quadratically nonlinear quasilocal driftThe Fokker–Planck equation in one-dimensional spacetime with quadratically nonlinear nonlocal drift
A former of a sequence of rectangular pulses with the quadratic scale of lengthsThe device forms a sequence of 16 groups of pulses of equal length. The number of pulses in a group
Some aspects of the geometry of the surfaces with the system of plane coordinate lines of the quadratic forms are presented too. The conditions, when of the plane coordinate lines are lines
Refined geometrically nonlinear equations of motion for elongated rod-type plate. These equations allow to describe the high-frequency torsional oscillation of elongated rod-type plate formed
On the contact equivalence problem of second order ODEs which are quadratic with respect to the second order derivative differential equations of the form y″2 + A(x, y, y′)y″ + B(x, y, y′) = 0 to be equivalent under the action
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