Results 311 to 320 of about 56,141 (357)
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Mathematische Annalen, 2017
We present a unified method to obtain unweighted and weighted estimates of linear and multilinear commutators with BMO functions, that is amenable to a plethora of operators and functional settings.
Á. Bényi+4 more
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We present a unified method to obtain unweighted and weighted estimates of linear and multilinear commutators with BMO functions, that is amenable to a plethora of operators and functional settings.
Á. Bényi+4 more
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Calculus of Variations and Partial Differential Equations, 2015
We consider the chemotaxis-fluid system 0.1in a bounded convex domain Ω⊂R3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek ...
M. Winkler
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We consider the chemotaxis-fluid system 0.1in a bounded convex domain Ω⊂R3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek ...
M. Winkler
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IEEE Transactions on Network Science and Engineering, 2021
Jun Cheng+3 more
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Jun Cheng+3 more
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2022
This chapter traces the troubled fate of a particular cognitive metaphor—the mind as a container for textual mental states—in American literary history. The novels that Charles Brockden Brown wrote in 1798–99 obsessively return to a curious scenario: a chest or box is supposed to hold important papers—usually letters or diaries—but either turns out to ...
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This chapter traces the troubled fate of a particular cognitive metaphor—the mind as a container for textual mental states—in American literary history. The novels that Charles Brockden Brown wrote in 1798–99 obsessively return to a curious scenario: a chest or box is supposed to hold important papers—usually letters or diaries—but either turns out to ...
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Local boundedness and Hölder continuity for the parabolic fractional p-Laplace equations
, 2021Mengyao Ding, Chao Zhang, Shulin Zhou
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1985
The general solution of linear time-invariant vibrating systems with given initial conditions and excitation function was determined in Chapter 4. However, in the engineering practice the initial conditions and the excitation function are frequently only approximately known, and because of this the general solution cannot be exactly calculated.
W. O. Schiehlen, P. C. Müller
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The general solution of linear time-invariant vibrating systems with given initial conditions and excitation function was determined in Chapter 4. However, in the engineering practice the initial conditions and the excitation function are frequently only approximately known, and because of this the general solution cannot be exactly calculated.
W. O. Schiehlen, P. C. Müller
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1996
In this chapter we study to what extent the exponential type of certain orbits of a C0—semigroup is determined by boundedness properties of the resolvent in a given right half-plane. The prototype of such results has already been proved in Section 2.2, where we showed that ω0(T) = s0(A) for C0—semigroups on Hilbert spaces.
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In this chapter we study to what extent the exponential type of certain orbits of a C0—semigroup is determined by boundedness properties of the resolvent in a given right half-plane. The prototype of such results has already been proved in Section 2.2, where we showed that ω0(T) = s0(A) for C0—semigroups on Hilbert spaces.
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1995
This section continues Section 14 from the standpoint of methods of investigation involved. The technique developed in Section 14 will be now applied to studying the regularity of sample functions of Gaussian random functions. Since our main interest here is with the properties of random functions defined on an arbitrary parametric set, we shall ...
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This section continues Section 14 from the standpoint of methods of investigation involved. The technique developed in Section 14 will be now applied to studying the regularity of sample functions of Gaussian random functions. Since our main interest here is with the properties of random functions defined on an arbitrary parametric set, we shall ...
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1977
The general solution of a vibration system has been found in chapter 3 for a given initial condition and a given forcing function. In technical applications, however, initial condition and forcing function are sometimes not exactly known, they are only specified as elements of a set of possible initial conditions or a family of forcing functions. Then,
Peter C. Müller, Werner Schiehlen
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The general solution of a vibration system has been found in chapter 3 for a given initial condition and a given forcing function. In technical applications, however, initial condition and forcing function are sometimes not exactly known, they are only specified as elements of a set of possible initial conditions or a family of forcing functions. Then,
Peter C. Müller, Werner Schiehlen
openaire +2 more sources