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Schrodinger operators, operators on manifolds, general differential operators, numerical studies, integral operators, discrete models, resonances, non-self-adjoint operators, random operators/matrices
1
vote
Asymptotic spectrum of a complex Sturm-Liouville differential operator
This operator has been studied in the paper by
Miloslav Znojil, PT-symmetric square well, Phys. Lett. A,
285 (2001) 7-10, and then by the same and many other authors. However I did not find out whethe …
5
votes
Accepted
First Dirichlet eigenvalue of the harmonic oscillator on a bounded interval $(-a,a)$?
Your formula for the first Dirichlet eigenvalue cannot be correct: for $a=1/\sqrt{2}$, the first eigenvalue is $5$.
Indeed, the eigenfunction
$$y(x)=e^{-x^2/2}(2x^2-1)$$
is positive on $(-1/\sqrt{2},1 …
1
vote
Spectral theorem and diagonal expansion for self adjoint operators
This is easier to explain on the finite dimensional example (though the idea is the same). The spectral theorem says that for every self-adjoint (same as Hermitian, in finite dimensional case) operato …
7
votes
Accepted
Continuity of eigenvectors
Yes. Let the size of your matrix be $n$.
Your condition implies that there is an $n-1\times n-1$ submatrix whose determinant is not identically equal to $0$.
Assume without loss of generality that thi …
4
votes
Eigenvalue problem of Schrodinger equation with polynomial growth potential on the real line
It depends on what you mean by "analytical result". Even quartic oscillator $q(x)=x^4+ax^2$ was studied VERY much. See, for example,
Bender, Carl M.; Wu, Tai Tsun Anharmonic oscillator. Phys. Rev. (2 …
13
votes
Eigenvalues of the Laplace-Beltrami operator on a compact Riemannnian manifold
A modern "simple philosophical" explanation is that this problem can be restated as an eigenvalue problem for a compact operator in an appropriate Hilbert space, whose eigenvalues are reciprocal to th …
1
vote
Accepted
sum of positive definite matrix
Yes, this follows from the Maximin characterization of eigenvalues of symmetric matrices. If $A$ is an $n\times n$ symmetric matrix, form the Rayleigh ratio
$R(x)=(x,Ax)/(x,x),$ where $(.,.)$ is the s …
1
vote
Accepted
Does asymptotic behavior guarantee uniqueness?
Under your assumption on the potential, there is indeed such a unique solution,
(I assume you mean $x\to+\infty$ in your boundary condition. This is proved by reducing your differential equation to an …
2
votes
Accepted
Limit (at infinity) for the lowest eigenvalue of a perturbed harmonic oscillator
Consider two operators $L_1w=-w''+U(x)w$ with eigenvalues $\lambda_k$ and $L_2w=-w''+V(x)w$
with eigenvalues $\mu_k$. If $U\geq V$ then $\lambda_k\geq \mu_k$.
To prove this consider the Rayleigh ratio …
2
votes
Ground state has always constant sign?
If $V(x)\to+\infty$ as $x\to\pm\infty$ then the spectrum is discrete, $\lambda_n\to+\infty$, and
the ground state (the eigenfunction corresponding to the smallest eigenvalue)
does not change sign. Mor …
1
vote
Accepted
Pseudo-polynomial potentials for Schrödinger operators
The answer is yes. Suppose your $V$ equals to a polynomial $P$ when $|x|$ is large. Then there is a constant $c$ such that we have
$P-c<V<P+c$, which implies that $\lambda_k^\prime-c<\lambda_k<\lambda …
2
votes
Accepted
Meromorphic solutions to Legendre's equation
Solutions of the equation you wrote are not polynomials. Legendre polynomials
are solutions of the equation
$$(1-x^2)y''-2xy'+l(l+1)y=0.$$
This equation is written in the same article you refer to. It …
1
vote
discrete spectrum of Schrödinger operator
The number of bound states is indeed finite. This can be proved as follows. First of all, for a bound state your eigenvalue $-k^2$ must be real. This is because your
operator with real $u$ and zero bo …
7
votes
Accepted
Existence of a real eigenvalue
It will be better if you write the definition of your matrix in a more readable way.
From what you wrote, it seems that your matrix satisfies $M(k,k+1)M(k+1,k)\geq 0$.
With this condition, all eigenva …
1
vote
Accepted
Spectrum of Mathieu equation
A good reference is Whittaker Watson, vol. 2.