Titlebook: Spectral Geometry and Inverse Scattering Theory; Huaian Diao,Hongyu Liu Book 2023 The Editor(s) (if applicable) and The Author(s), under e

Exaltation

書目名稱Spectral Geometry and Inverse Scattering Theory影響因子(影響力)




書目名稱Spectral Geometry and Inverse Scattering Theory影響因子(影響力)學(xué)科排名




書目名稱Spectral Geometry and Inverse Scattering Theory網(wǎng)絡(luò)公開度




書目名稱Spectral Geometry and Inverse Scattering Theory網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Spectral Geometry and Inverse Scattering Theory被引頻次




書目名稱Spectral Geometry and Inverse Scattering Theory被引頻次學(xué)科排名




書目名稱Spectral Geometry and Inverse Scattering Theory年度引用




書目名稱Spectral Geometry and Inverse Scattering Theory年度引用學(xué)科排名




書目名稱Spectral Geometry and Inverse Scattering Theory讀者反饋




書目名稱Spectral Geometry and Inverse Scattering Theory讀者反饋學(xué)科排名

尾巴

peak-flow

e geometrical inverse shape problems by minimal measurements.Inverse scattering problems are a vital subject for both theoretical and experimental studies and remain an active field of research in applied mathematics. This book provides a detailed presentation of typical setup of inverse scattering

管理員

Introduction,tion that seeks to optimally combine theory with observations. In its abstract formulation, an inverse problem can be described as follows. Let (., ∥?∥.) denote the space of target objects (usually consisting of quantities or geometries) and (., ∥?∥.) denote the space of observation data. Let . deno

Concrete

Geometric Structures of Maxwellian Eigenfunctions,ongly motivated by our study of the inverse electromagnetic scattering problem. In this chapter, we follow the treatment in Diao et al. (Inverse Probl 37:035004, 2021). Further discussion on the inverse electromagnetic scattering problems can be found in Sect. .. We start with the necessary mathemat

Pageant

Path Argument for Inverse Acoustic and Electromagnetic Obstacle Scattering Problems,nd . to represent the incident, scattered and total field, respectively, where .?=?.?+?. and . with . being the incident direction and .?>?0 being the wave number. Let . be an impenetrable obstacle, where . is a general compact set in . with an open connect complement ..

側(cè)面左右

,Geometric Structures of Maxwell’s Transmission Eigenfunctions and Applications,–2224 (2021)). Let . denote the frequency, and let ., respectively, signify the electric permittivity and magnetic permeability of a uniformly homogeneous space. Throughout, we let . and . denote, respectively, the electric and magnetic fields, which are .-valued functions. We first introduce the no

Platelet

ostensible

LUCY