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    Wave Motion

    Wave Motion

    JournalISSN 0165-2125eISSN 1878-433X中科院 物理与天体物理 3区

    年发文量

    研究主题

    论文(3226)

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    1A Shear-Capillary Mixed-Flux Extension of the Benjamin-Ono Equation: Structure, Traveling Waves, and an Analytical Roadmap
    Qamar Din
    2027
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    2Generation of Hydroacoustic Waves by Localized Transient Uplift at the Bottom of Marine Sediment Layers
    P.F. Hou, D.Q. Lu
    2027
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    3New Analytical Solutions for a Variable-Coefficient Hirota Bilinear System in Fluid Dynamics
    Yu-Xin Song,Guang-Mei Wei, Hao-Qing Chen
    2027
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    4Weakly Non-Integrable Solitary Wave Collisions in the Modified Benjamin–Bona–Mahony Equation
    Marcelo V. Flamarion,Efim Pelinovsky
    2027
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    5Qualitative Imaging of Orthotropic Elastic Plates by First-Iteration Adjoint Sensitivity Maps: A Reflection–transmission Residual-Wave Interaction Indicator
    Hamza Hafidi Alaoui, Hatem Zayeni

    First-iteration adjoint-state sensitivity maps are examined for qualitative ultrasonic imaging of defects in orthotropic plates under a single pitch–catch illumination. The five signed kernels of the classical least-squares misfit are displayed as absolute-value normalised images, not as material updates of an iterative FWI reconstruction.We form a reflection–transmission residual-wave interaction indicator, correlating two fields back-propagated from residuals on opposed apertures. It is bilinear in the two residual families, where every single-residual construction is linear in one; since the degree of homogeneity in the data is invariant under linear data-space operators, no reweighting of the misfit produces it. It is not the propagator term of the first variation of any standard single-state constrained functional, both fields sharing the same time orientation. It does, however, admit an exact variational status in the perturbation variable, and a gradient in the discrete space where the maps are computed.The set-up being mirror-symmetric about the axis through the inclusion, all four C66 constructions vanish quadratically along it; reversing the source polarisation moves that zero to C11, C22 and C12, as predicted: a causal test. For the density and the three normal-block coefficients the classical maps localise the inclusion to within two tenths of a defect radius, which the indicator does not improve. Its benefit is specific to C66, whose multipolar map keeps a fitted centre of symmetry within half a defect radius of the inclusion under both apertures, against classical displacements of 0.83 and at least 1.5 radii.

    2027
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    高被引作者

    作者引用发文
    Stuart Crampin12733
    George C. Papanicolaou10219
    Joseph Bishop Keller9888
    Robert Burridge91810
    Jan D. Achenbach89216
    Andrew Norris88524
    Dan Givoli8056
    Sa Shapiro7621
    N. Gold7621
    Erik H. Saenger7621

    高产作者

    作者引用发文
    Andrew Norris88524
    Paul A. Martin34322
    Jüri Engelbrecht40921
    Richard Craster45717
    Jan D. Achenbach89216
    Jens Lothe60116
    Gérard Maugin27516
    Ian David Abrahams46415
    A. Jeffrey31514
    V. I. Alshits55614

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