We study the Hermite operator H = -Delta + vertical bar x vertical bar(2) in Rd and its fractional powers H-beta, beta > 0 in phase space. Namely, we represent functions f via the so-called short-time Fourier, alia...
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We study the Hermite operator H = -Delta + vertical bar x vertical bar(2) in Rd and its fractional powers H-beta, beta > 0 in phase space. Namely, we represent functions f via the so-called short-time Fourier, alias Fourier-Wigner or Bargmann transform V(g)f (g being a fixed window function), and we measure their regularity and decay by means of mixed Lebesgue norms in phase space of V(g)f, that is in terms of membership to modulation spaces M-P,M-q, 0 < p, q <= infinity. We prove the complete range of fixed-time estimates for the semigroup e-tH(beta) when acting on M-p,M-q, for every 0 < p, q <= infinity, exhibiting the optimal global-in-time decay as well as phase-space smoothing. As an application, we establish global well-posedness for the nonlinear heat equation for H-beta with power-type nonlinearity (focusing or defocusing), with small initial data in modulation spaces or in Wiener amalgam spaces. We show that such a global solution exhibits the same optimal decay e(-ct) as the solution of the corresponding linear equation, where c = d(beta) is the bottom of the spectrum of H. Global existence is in sharp contrast to what happens for the nonlinear focusing heat equation without potential, where blow-up in finite time always occurs for (even small) constant initial data (constant functions belong to M-infinity,M-1 ). (C) 2021 Elsevier Inc. All rights reserved.
In this paper, we consider the operator e i t ϕ ( h ( D ) ) where h defined on R n is a C ∞ ( R n ∖ { 0 } ) positive homogeneous function with degree λ > 0 and ϕ : R → R is a smooth function satisfying the follo...
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In this paper, we consider the operator e i t ϕ ( h ( D ) ) where h defined on R n is a C ∞ ( R n ∖ { 0 } ) positive homogeneous function with degree λ > 0 and ϕ : R → R is a smooth function satisfying the following. (A 1 ) There exists a constant m 1 > 0 such that for all μ ∈ N 0 : = N ∪ { 0 } | ϕ ( μ ) ( r ) | ≲ r m 1 − μ , r ≥ 1 . (A 2 ) There exists a constant m 2 > 0 such that for all μ ∈ N 0 | ϕ ( μ ) ( r ) | ≲ r m 2 − μ , 0 < r < 1 . We prove the boundedness of the operator e i t ϕ ( h ( D ) ) on the modulation spaces and obtain its asymptotic estimate as t goes to infinity. As applications, we give the grow-up rate of the solutions for the Cauchy problems for the generalized wave, Klein–Gordon and Schrödinger equations.
In this paper, we obtain the sharp conditions of the inclusion relations between modulation spaces M-p,q(s) and Triebel-Lizorkin spaces F-p,F-r for p <= 1, which greatly improve and extend the results for the embed...
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In this paper, we obtain the sharp conditions of the inclusion relations between modulation spaces M-p,q(s) and Triebel-Lizorkin spaces F-p,F-r for p <= 1, which greatly improve and extend the results for the embedding relations between local Hardy spaces and modulation spaces obtained by Kobayashi, Miyachi and Tomita in [Studia Math. 192 (2009), 79- 96].
We show the existence of weak solutions in the extended sense of the Cauchy problem for the cubic nonlinear Schrodinger equation in the modulation space Ms2, q ( R), 1 = q = 2 and s = 0. In addition, for either s = 0 ...
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We show the existence of weak solutions in the extended sense of the Cauchy problem for the cubic nonlinear Schrodinger equation in the modulation space Ms2, q ( R), 1 = q = 2 and s = 0. In addition, for either s = 0 and 1 = q = 3 2 or 3 2 < q = 2 and s > 2 3 - 1 q we show that the Cauchy problem is unconditionally wellposed in Ms2, q ( R). It is done with the use of the differentiation by parts technique which had been previously used in the periodic setting.
We provide new estimates for the matrix coefficients of the metaplectic representation, inspired by a formal analogy with the Strichartz estimates which hold for several classes of evolution propagators U(t). The one ...
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We provide new estimates for the matrix coefficients of the metaplectic representation, inspired by a formal analogy with the Strichartz estimates which hold for several classes of evolution propagators U(t). The one parameter group of unitary operators U(t) is replaced by a unitary representation of a non-compact Lie group, the group element playing the role of time;the case of the metaplectic or oscillatory representation is of special interest in this connection, because the Schrodinger group is a subgroup of the metaplectic group. We prove uniform weak-type sharp estimates for matrix coefficients and Strichartz-type estimates for that representation. The crucial point is the choice of function spaces able to detect such a decay, which in general will depend on the given group action. The relevant function spaces here turn out to be the so-called modulation spaces from time-frequency analysis in Euclidean space, and Lebesgue spaces with respect to Haar measure on the metaplectic group. The proofs make use in an essential way of the covariance of the Wigner distribution with respect to the metaplectic representation.
In this paper, we study the boundedness of the Schrodinger propagator ei Delta on Wiener amalgam spaces. In particular, we determine the necessary and sufficient conditions for the propagator ei Delta to be bounded fr...
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In this paper, we study the boundedness of the Schrodinger propagator ei Delta on Wiener amalgam spaces. In particular, we determine the necessary and sufficient conditions for the propagator ei Delta to be bounded from Wp,qs to Wp,q0.
We study the Cauchy problem for an incompressible magneto-hydrodynamics (MHD) system in the modulation space M-q,sigma(s) (R-n) (n >= 2) with initial data (u(0), b(0)) is an element of PMq,sigma s (R-n) x PMq,sigma...
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We study the Cauchy problem for an incompressible magneto-hydrodynamics (MHD) system in the modulation space M-q,sigma(s) (R-n) (n >= 2) with initial data (u(0), b(0)) is an element of PMq,sigma s (R-n) x PMq,sigma s (R-n). We prove that this problem is locally well-posed in such a space when 1 <= q <= infinity, 1 <= sigma < infinity and n(sigma-1)/sigma - 1 <= s, and globally well-posed when 1 <= q <= n, n/n-1 <= sigma < infinity and max{n(sigma-1)/sigma -1, n(sigma-2)/sigma} < s < n(sigma-1)/sigma. (C) 2011 Elsevier Inc. All rights reserved.
We study the covariance property of quadratic time-frequency distributions with respect to the action of the extended symplectic group. We show how covariance is related to and in fact in competition with the possibil...
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We study the covariance property of quadratic time-frequency distributions with respect to the action of the extended symplectic group. We show how covariance is related to and in fact in competition with the possibility of damping the interferences which arise due to the quadratic nature of the distributions. We also show that the well-known fully covariance property of the Wigner distribution in fact characterizes it (up to a constant factor) among the quadratic distributions L-2(R-n) -> C-0(R-2n). A similar characterization for the closely related Weyl transform is given as well. The results are illustrated by several numerical experiments for the Wigner and Born-Jordan distributions of the sum of four Gaussian functions in the so-called diamond con figuration.
One of the most popular time-frequency representations is certainly the Wigner distribution. To reduce the interferences coming from its quadratic nature, several related distributions have been proposed, among which ...
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One of the most popular time-frequency representations is certainly the Wigner distribution. To reduce the interferences coming from its quadratic nature, several related distributions have been proposed, among which is the so-called Born-Jordan distribution. It is well known that in the Born-Jordan distribution the ghost frequencies are in fact damped quite well, and the noise is in general reduced. However, the horizontal and vertical directions escape from this general smoothing effect, so that the interferences arranged along these directions are in general kept. Whereas these features are graphically evident on examples and heuristically well understood in the engineering community, there is no at present mathematical explanation of these phenomena, valid for general signals in L-2 and, more in general, in the space S' of temperate distributions. In the present note we provide such a rigorous study using the notion of wave-front set of a distribution. We use techniques from Time-=frequency Analysis, such as the modulation and Wiener amalgam spaces, and also results of microlocal regularity of linear partial differential operators. (C) 2016 Elsevier Inc. All rights reserved.
Quantum harmonic analysis on phase space is shown to be linked with localization operators. The convolution between operators and the convolution between a function and an operator provide a conceptual framework for t...
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Quantum harmonic analysis on phase space is shown to be linked with localization operators. The convolution between operators and the convolution between a function and an operator provide a conceptual framework for the theory of localization operators which is complemented by an appropriate Fourier transform, the Fourier-Wigner transform. We use Lieb's uncertainty principle to establish a sharp Hausdorff-Young inequality for the Fourier-Wigner transform. Noncommutative Tauberian theorems due to Werner allow us to extend results of Bayer and Geochenig on localization operators. Furthermore we show that the Arveson spectrum and the theory of Banach modules provide the abstract setting of quantum harmonic analysis. (C) 2017 Elsevier Masson SAS. All rights reserved.
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