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In order to be able to solve the inverse problem of electrocardiography, the lead field matrix (transfer matrix) has to be calculated.
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Impedance matrix and transfer matrix methods are often used in the analysis of linear dynamical systems.
The behaviour at the point of attachment is described by what we have called the transfer matrix M. Our transfer matrices will be real constant transfer matrices, i.e., all components will be constants.
In principle, ( hat{T} ) can be seen as a proxy transfer matrix of the true transfer matrix T to perform decoding.
The properties of the impedance matrix and the transfer matrix of symmetrical systems, reciprocal systems and conservative systems are investigated.
Their effects on the integrity of the laminate panel are accounted for by integrating the so-called interfacial transfer matrices into the global transfer matrix.
The reflection spectrum from the FBG, subjected to different strain profiles, is simulated based on the Transfer matrix (T-matrix) approach.
Generally, there are two methods, namely transfer matrix method and assemble matrix method, for obtaining the dispersion relations in laminates.
In such a representation, a transmission line is characterized by two matrix transfer functions: the propagation matrix (varvec{H}) and the characteristic impedance matrix (varvec{Z}_{C}(s)).
To illustrate the effectiveness of the techniques, we determined the two extremal eigenpairs of a cyclic matrix, the transfer matrix of the two-dimensional Ising model, and the Hamiltonian matrix of the one-dimensional Hubbard model.
In this paper, some new properties of the infinite eigenstructure of the system matrix pencil of the transfer matrix are presented.
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