Exemplos de uso de Eigenfunctions em Inglês e suas traduções para o Português
{-}
-
Colloquial
-
Official
-
Medicine
-
Financial
-
Ecclesiastic
-
Ecclesiastic
-
Computer
-
Official/political
Generate a gallery of the eigenfunctions.
Compute 10 eigenfunctions of the Laplacian over the knot.
The analysis of these problems involves the eigenfunctions of a differential operator.
Its eigenfunctions are| ϕ⟩{\displaystyle|\phi\rangle\,} and its eigenvalues are the energies E{\displaystyle E\.
These modes have a singular phase profile and are eigenfunctions of the photon orbital angular momentum.
As a consequence, we obtain that this model has pure point spectrum a.e. with exponentially decaying eigenfunctions.
When restricted to the standard topology of the real numbers, the eigenfunctions are curiously the Bernoulli polynomials!
The pseudo-harmonics are the eigenfunctions associated with the leakage+ removal operators in the multigroup steady-state diffusion equation.
All discretized equations were modified so that they could be treated as eigenfunctions according to the programming dynamics.
It is interesting to consider the eigenfunctions of this operator, and how they differ when restricted to different subspaces of( Ω, F){\displaystyle\Omega,{\mathcal{F.
We impose the dirichlet condition to the¿-laplacian andproof the existence of analytic curves of its eigenfunctions and eigenvalues.
Its application is shown using the to calculate autoenergias and eigenfunctions of the hydrogen atom and the dimensional harmonic oscillator in both schemes mentioned.
Work==Agmon's contributions to partial differential equations include Agmon's method for proving exponential decay of eigenfunctions for elliptic operators.
Again, it is shown that the boundary conditions that make anti-periodic eigenfunctions are illegitimate, reaffirming the results most commonly found in the literature. the low and high energies limits are fully satisfactory.
In this work we use an iterative method inspired by the inverse iteration with shift technique of linear linear algebra to find the eigenvalues and eigenfunctions of the sturm-liouville problem.
This study aims to determine the eigenfunctions or vibration modes of a system compo- sed of two beams coupled by an elastic layer and modeled mathematically by timoshenko theory for beams.
There exists a subset of physical systems for which the form of the eigenfunctions and their associated energies, or eigenvalues, can be found.
The"in"(+) and"out"(-) states are assumed to form bases too, in the distant past and distant future respectively having the appearance of free particle states,but being eigenfunctions of the complete Hamiltonian.
Since the Fock operator depends on the orbitals used to construct the corresponding Fock matrix, the eigenfunctions of the Fock operator are in turn new orbitals which can be used to construct a new Fock operator.
For Gaussian ensembles, the scaled spectral density of the matrices has a closed formfor finite matrix dimension, related to the eigenfunctions of the quantum harmonic oscillator.
Natural frequencies and their mode shapes, also called eigenfunctions, of the coupled system are obtained through a uniform beam methodology which uses the free dynamical basis to represent the solution of the the modal equation.
The observability inequality proved in this work applies to a class solutions in fourier series generated by the eigenfunctions associated with eigenvalues of the spectral problem.
In this direction, the present dissertation uses the numerov method to solve two problems:1 to find the eigenfunctions and the associated energies of a nanostructure composed by two quantum wells and three rectangular barriers inside of an infinite quantum well; 2 to find solutions of the schrödinger equation having potentials that includes the dirac delta function as a barrier.
Thus, the solution obtained to the neutron transport equation is composed by a linear combination of singular eigenfunctions associated the a set of eigenvalues analogous to determined by case to the one-dimensional slab geometry problem.
In this work the model of timoshenko is formulated in matrix terms andallows that the study of the eigenvalues and eigenfunctions be performed using a basis of a complete second order matrix modal equation, generated by a fundamental matrix solution.
The solution was developed using the generalized integral transform technic(gitt), a hybrid analytic-numerical method based in orthogonal eigenfunctions expansions,beside conventional eigenfunctions, it was proposed a solution with layer eigenfunctions to achieve better convergence rates for the method.
Edition(1962);*"Eigenfunction Expansions Associated with Second-order Differential Equations.
From the Schrödinger equation, the phase of an eigenfunction with energy E goes as e- i E t/ ℏ{\displaystyle e^{-iEt/\hbar.
The dominant eigenvalue and its eigenfunction are obtained by the power method in the eigenvalue problem. the soluti.
This intuitive picture is not quite right, because ψ(±){\displaystyle\psi^{(\pm)}}is an eigenfunction of the Hamiltonian and so at different times only differs by a phase.