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Cholesky factorization
Multichannel predictive deconvolution based on the fast iterative shrinkage-thresholding algorithm
Source estimation for wavefield-reconstruction inversion
Analysis of prior models for a blocky inversion of seismic AVA data
A parallel finite-element time-domain method for transient electromagnetic simulation
Three dimensional inversion of multisource time domain electromagnetic data
Value of information of seismic amplitude and CSEM resistivity
Electromagnetic induction in a generalized 3D anisotropic earth, Part 2: The LIN preconditioner
Uncertainty quantification for inverse problems with weak partial-differential-equation constraints
Inferring Earthquake Ground‐Motion Fields with Bayesian Networks
Polynomial equivalent layer
Time-domain modeling of electromagnetic diffusion with a frequency-domain code
Convolutional equivalent layer for magnetic data processing
Forward calculation of 3D controlled-source electromagnetic responses based on joint application of secondary field and coupled potential formulations
The simulation of finite ERT electrodes using the complete electrode model
Finite-element modeling of time-domain controlled-source electromagnetic survey with weighted Laguerre polynomials
Finite-element analysis of top-casing electric source method for imaging hydraulically active fracture zones
Abstract Conjugate-Gradient and Quasi-Newton Methods: We now will discuss two gradient-optimization methods commonly used in geophysical inversion: the conjugate-gradient (CG) method and the quasi-Newton (QN) method. Unlike the Newton method, these two methods do not explicitly compute the inverse to the Hessian; instead, they iteratively move along descent directions that reduce the data residual. Each iteration costs only O(N2) operations of a matrix-vector multiply. Another strength is that, in the case of CG and low-memory QN methods, no Hessian matrix needs to be stored or inverted explicitly. Their weakness is that fast convergence is not guaranteed. However, they are generally faster than the nonpreconditioned steepest-descent method.