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Bohr’s inequality for harmonic mappings and beyond
with the classical Bohr inequality for bounded analytic functions defined on the unit disk centered at the origin

Caristi’s condition and existence of a minimum of a lower bounded function in a metric space. Applications to the theory of coincidence pointsWe consider a lower bounded function on a complete metric space. For this function, we obtain

Ergodicity and Related Bounds for One Particular Class of Markovian Time—Varying Queues with Heterogeneous Servers and Customer’s Impatience restrictions on the intensity functions, the quantity of interest, the total number of customers in the system

The punishing factors for convex pairs are 2n-1 with the set A(Ω, ∏) of functions f : Ω → ∏ holomorphic on Ω and we prove estimates for |f(n)(z)|, f ∈ A(Ω, Ω

An Upper Bound Solution for Axisymmetric Extrusion and Drawing Considering a Generalized Yield Criterion, the available upper bound solutions are almost all restricted to this criterion. The objective of the present

The Lower Semicontinuity of Distortion Coefficients of the Homeomorphisms Inducing Bounded Composition Operators of Sobolev–Orlicz SpacesWe determine the conditions under which the locally uniform limit of mappings generating bounded

Ergodicity and truncation bounds for inhomogeneous birth and death processes with additional transitions from and to origin possible transition intensities are assumed to be non-random functions of time and may depend on the state

NEW BOUNDS FOR SHANNON, RELATIVE AND MANDELBROT ENTROPIES VIA ABEL-GONTSCHAROFF INTERPOLATING POLYNOMIAL computing useful upper bounds for several entropic measures used in information theory. We use discrete

The punishing factors for convex pairs are 2n-1 with the set A(Ω, ∏) of functions f : Ω → ∏ holomorphic on Ω and we prove estimates for |f(n)(z)|, f ∈ A(Ω, Ω

Ergodicity and perturbation bounds for inhomogeneous birth and death processes with additional transitions from and to the origin to the origin can occur. All possible transition intensities are assumed to be non-random functions of time

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