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1 er of principal components (eigen-vectors or eigenfunctions).
2 available for further analyses as secondary eigenfunctions.
4 ollective variables is to relate them to the eigenfunctions and eigenvalues of the transfer operator.
5 n terms of the isotropic harmonic oscillator eigenfunctions and Hydrogen atom eigenfunctions independ
6 irm the dominant spectral frequencies of the eigenfunctions and locate them as (absolute valued) modu
8 e hydrophobic free energy sequences or their eigenfunctions; and (iii) discrete, best bases, trigonom
10 ortex knots occur frequently, even in random eigenfunctions at relatively low energy, and are constra
12 echniques to address these difficulties: (i) eigenfunction construction from the linear decomposition
13 lex-valued firing-rate model derived from an eigenfunction expansion of the Fokker-Planck equation an
15 this property by computing the ground-state eigenfunction for a simplified Schrodinger operator with
17 ey can be used to obtain the eigenvalues and eigenfunctions for the same potential, orientated at an
18 odes approximate the eigenvalue spectrum and eigenfunctions in a systematically improvable manner, an
20 oscillator eigenfunctions and Hydrogen atom eigenfunctions independently, showing that each one resu
21 ical evidence to support the conjecture that eigenfunctions inherit this property by computing the gr
22 of the leading eigenvector-derived, m(1)AChR eigenfunctions locates seven hydrophobic transmembrane s
24 The function [Formula: see text] (x) is the eigenfunction of the Kolmogorov backward operator with t
25 method explicitly finds the eigenvalues and eigenfunctions of the diffusion generator associated wit
27 kernel and its gradient, as well as for the eigenfunctions of the Laplacian and their gradient, that
29 The spectral method exploits the natural eigenfunctions of the master equation of birth-death pro
30 Hermite functions," a generalization of the eigenfunctions of the quantum harmonic oscillator and th
34 Constructions of hydrophobic free energy eigenfunctions, psil, from M-lagged, M x M autocovarianc
35 alized ensembles, extracts transfer operator eigenfunctions using a neural network ansatz and then ac
37 which allows us to obtain analytically exact eigenfunctions whose ergodicity-breaking properties can