Institute of Mathematics AS CR, v. v. i.
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    44818 research outputs found

    Editorial

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    summary:Úvodní slovo shrnuje obsah čísla.summary:The editorial presents an overview of the articles from this issue

    OBITUARY

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    Optimality conditions for interval-valued vector equilibrium problems

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    summary:In the article, one formulates Fritz John type and Karush-Kuhn-Tucker type necessary conditions for an interval-valued vector equilibrium problem having a locally LU-efficient solution, where convexificators demonstrate the solutions that are regular. Sufficient conditions for a locally weak LU-efficient solution have been entrenched by imposing appropriate assumptions along with generalized convexity. Some applications are presented for a constrained interval-valued vector variational inequality and a constrained interval-valued vector optimization problem

    Instruction for authors

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    Multilinear fractional maximal and integral operators with homogeneous kernels, Hardy-Littlewood-Sobolev and Olsen-type inequalities

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    summary:Let mNm\in \mathbb {N} and 0<α<mn0<\alpha <mn. Let TΩ,α;m\mathcal {T}_{\Omega ,\alpha ;m} be the multilinear fractional integral operator with homogeneous kernels, and let MΩ,α;m\mathcal {M}_{\Omega ,\alpha ;m} be the multilinear fractional maximal operator with homogeneous kernels. We will use the idea of Hedberg to reprove that the multilinear operators TΩ,α;m\mathcal {T}_{\Omega ,\alpha ;m} and MΩ,α;m\mathcal {M}_{\Omega ,\alpha ;m} are bounded from Lp1(Rn)×Lp2(Rn)××Lpm(Rn)L^{p_1}(\mathbb R^n)\times L^{p_2}(\mathbb R^n) \times \nobreak \cdots \times L^{p_m}(\mathbb R^n) into Lq(Rn)L^q(\mathbb R^n) provided that Ω=(Ω1,Ω2,,Ωm)[Ls(Sn1)]m\vec {\Omega }=(\Omega _1,\Omega _2,\dots ,\Omega _m)\in [L^s({\bf S}^{n-1})]^{m}, s<p1,p2,,pm<s'<p_1,p_2,\dots ,p_m<\infty , s/m<p<n/αs'/m<p<n/{\alpha }, 1p=1p1+1p2++1pmand1q=1pαn. \frac {1}{p}=\frac {1}{p_1}+\frac {1}{p_2}+\cdots +\frac {1}{p_m} \quad \text {and} \quad \frac {1}{q}=\frac {1}{p}-\frac {\alpha }{n}. This result was first obtained by Chen and Xue. We also prove that under the assumptions that Ω=(Ω1,Ω2,,Ωm)[Ls(Sn1)]m\vec {\Omega }=(\Omega _1,\Omega _2,\dots ,\Omega _m) \in [L^s({\bf S}^{n-1})]^{m}, sp1,p2,,pm<s'\leq p_1,p_2,\dots ,p_m<\infty , s/mp<n/αs'/m\leq p<n/{\alpha } and ()(*), the multilinear operators TΩ,α;m\mathcal {T}_{\Omega ,\alpha ;m} and MΩ,α;m\mathcal {M}_{\Omega ,\alpha ;m} are bounded from Lp1(Rn)×Lp2(Rn)××Lpm(Rn)L^{p_1}(\mathbb R^n)\times L^{p_2}(\mathbb R^n) \times \cdots \times L^{p_m}(\mathbb R^n) into Lq,(Rn)L^{q,\infty }(\mathbb R^n), which are completely new. Moreover, we will use the idea of Adams to show that TΩ,α;m\mathcal {T}_{\Omega ,\alpha ;m} and MΩ,α;m\mathcal {M}_{\Omega ,\alpha ;m} are bounded from Lp1,κ(Rn)×Lp2,κ(Rn)××Lpm,κ(Rn)L^{p_1,\kappa }(\mathbb R^n)\times L^{p_2,\kappa }(\mathbb R^n) \times \cdots \times L^{p_m,\kappa }(\mathbb R^n) into Lq,κ(Rn)L^{q,\kappa }(\mathbb R^n) whenever s<p1,p2,,pm<s'<p_1,p_2,\dots ,p_m<\infty , 0<κ<10<\kappa <1, s/m<p<n(1κ)/αs'/m<p<{n(1-\kappa )}/{\alpha }, 1p=1p1+1p2++1pmand1q=1pαn(1κ), \frac {1}{p}=\frac {1}{p_1}+\frac {1}{p_2}+\cdots +\frac {1}{p_m} \quad \text {and} \quad \frac {1}{q}=\frac {1}{p}-\frac {\alpha }{n(1-\kappa )}, and also bounded from Lp1,κ(Rn)×Lp2,κ(Rn)××Lpm,κ(Rn)L^{p_1,\kappa }(\mathbb R^n)\times L^{p_2,\kappa }(\mathbb R^n) \times \cdots \times L^{p_m,\kappa }(\mathbb R^n) into WLq,κ(Rn)WL^{q,\kappa }(\mathbb R^n) whenever sp1,p2,,pm<s'\leq p_1,p_2,\dots ,p_m<\infty , 0<κ<10<\kappa <1, s/mp<n(1κ)/αs'/m\leq p<{n(1-\kappa )}/{\alpha } and ()(**). These results mentioned above are also completely new. In addition, some new estimates in the limiting cases are also established. Applications to the Hardy-Littlewood-Sobolev and Olsen-type inequalities are discussed as well

    A stochastic version of Vidyasagar theorem on the stabilization of interconnected systems

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    summary:The purpose of this paper is to provide sufficient conditions for the feedback asymptotic stabilization in probability for a class of affine in the control nonlinear stochastic differential systems. In fact, under the assumptions stated in this paper we prove the existence of a control Lyapunov function that according to the stochastic version of Artstein's theorem guarantees the asymptotic stability in probability by means of a state feedback law that is smooth except eventually at the equilibrium. This result generalizes the well-known theorem of Vidyasagar concerning the feedback stabilization problem for interconnected control systems

    Honeycomb graphs for parametric identification of correlation classes in multidimensional datasets

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    summary:In the process of gaining knowledge from large sets of data, one of the most significant methods from the area of descriptive statistics - correlation analysis - is applied to determine direct functional relationships between pairs of attributes. Even though the results of correlation analysis are measured through a crisp correlation coefficient, whose values belong to the [1,1][-1,1] interval, human interpretation of these values is conventionally vague and uses linguistic classes of correlation to describe the strength of relationships between attribute pairs. However, this interpretative vagueness - and the correlation classes themselves - are not commonly employed in the decision-making processes. Therefore, this work focuses on the design and implementation of so-called Honeycomb Graphs - a visualization method for parametric identification of correlation classes in multidimensional datasets based on graphical models. After implementing the proposed visualization technique, two case studies on benchmark datasets are conducted, and the model is evaluated from both qualitative and quantitative points of view. The results of these studies highlight interactive exploration of correlation analysis while adhering to qualitative and quantitative standards of scientific visualizations and high utilization potential of the method in feature selection tasks, making it a valuable tool for predictive analysis and data exploration

    Číselná charakteristika podobných trojúhelníků

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    Characteristic forms of complex Cartan geometries III: GG-structures

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    summary:Characteristic class relations in Dolbeault cohomology follow from the existence of a holomorphic geometric structure (for example, holomorphic conformal structures, holomorphic Engel distributions, holomorphic projective connections, and holomorphic foliations). These relations can be calculated directly from the representation theory of the structure group, without selecting any metric or connection or having any knowledge of the Dolbeault cohomology groups of the manifold. This paper improves on its predecessor [17] by allowing infinite type geometric structures

    On the number of iterations in the Alternating Method for integer matrices in max-algebra

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    summary:The Alternating Method in max-algebra is an efficient approach for solving two-sided max-linear systems of the form Ax=ByA \otimes x=B \otimes y, where AA, BB are matrices and xx, yy are vectors of compatible sizes. This iterative procedure typically begins with a randomly chosen initial vector. In the case when matrices AA and BB are integer matrices and one is finite while the other has at least one finite element in each row and in each column, and provided that the initial vector is also an integer vector, an upper bound on the number of iterations can be determined. This paper proposes starting the Alternating Method with a vector selected based on the matrix elements of A~=(A)A\tilde{A}=(-A^\top) \otimes A, where AA is a finite matrix of the given system, instead of using a randomly selected vector. This choice of initial vector aims to minimize the number of iterations in the Alternating Method. We have proved that, with the proposed choice of initial vector, the number of iterations is bounded above by the expression containing the maximum element of matrix A~\tilde{A}. From this statement, we derive additional conclusions regarding this bound. Finally, we compare the number of iterations in the Alternating Method when it starts from a randomly chosen vector versus when it starts from the vector we propose in this study

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    Institute of Mathematics AS CR, v. v. i.
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