<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom" xmlns:content="http://purl.org/rss/1.0/modules/content/"><channel><title>Inverse-Spectral-Theory on Unsalvageable Proofs</title><link>https://saddle196883.github.io/personalpage/tags/inverse-spectral-theory/</link><description>Recent content in Inverse-Spectral-Theory on Unsalvageable Proofs</description><generator>Hugo -- 0.147.1</generator><language>en-us</language><lastBuildDate>Sun, 16 Aug 2026 00:00:00 +0000</lastBuildDate><atom:link href="https://saddle196883.github.io/personalpage/tags/inverse-spectral-theory/index.xml" rel="self" type="application/rss+xml"/><item><title>Inverse Spectral Theory Part 02: Properties of the Fundamental Solutions</title><link>https://saddle196883.github.io/personalpage/posts/inverse-spectral-theory-02/</link><pubDate>Sun, 16 Aug 2026 00:00:00 +0000</pubDate><guid>https://saddle196883.github.io/personalpage/posts/inverse-spectral-theory-02/</guid><description>&lt;p>In the &lt;a href="https://saddle196883.github.io/personalpage/posts/inverse-spectral-theory-01">previous part&lt;/a> we have constructed our two &lt;em>fundamental solutions&lt;/em> $y_1$ and $y_2$ to the ODE
$$
-y_j^{\prime\prime} + q(x)y_j = \lambda y_j,
$$
with initial data
$$
y_1(0) = y_2^\prime(0) = 1,\quad y_1^\prime(0) = y_2(0) = 0.
$$&lt;/p>
&lt;p>The goal of this section is to establish useful facts about the $y_j$, for we need to use them in the later sections to establish meaningful results. These facts come in the form of estimates, knowledge about the (partial) derivatives of the $y_j$, as well as analyticity properties.&lt;/p></description></item><item><title>Inverse Spectral Theory Part 00: Introduction</title><link>https://saddle196883.github.io/personalpage/posts/inverse-spectral-theory-00/</link><pubDate>Sun, 09 Aug 2026 00:00:00 +0000</pubDate><guid>https://saddle196883.github.io/personalpage/posts/inverse-spectral-theory-00/</guid><description>&lt;p>A while ago, while I was doing some readings, I found a result that worked for &amp;lsquo;&amp;lsquo;an open dense set of nonlinearities&amp;rsquo;&amp;rsquo;. Putting aside what this really means, I found out that to establish this fact, one had to effectively reconstruct a differential operator from its eigenvalues. I found it rather fascinating, and took a shallow dive into this topic.&lt;/p>
&lt;p>Unfortunately, a lot of these were not getting into my head, and so I volunteered to do a talk series in my university&amp;rsquo;s unofficial mathematics Discord chat. But to do so would require me to prepare notes, which I did, but they were not to my standard, and so I am redoing them, this time in an online format here, so that I can finally do the talks and finally learn inverse spectral theory.&lt;/p></description></item><item><title>Inverse Spectral Theory Part 01: Power Series Methods for ODEs</title><link>https://saddle196883.github.io/personalpage/posts/inverse-spectral-theory-01/</link><pubDate>Sun, 09 Aug 2026 00:00:00 +0000</pubDate><guid>https://saddle196883.github.io/personalpage/posts/inverse-spectral-theory-01/</guid><description>&lt;p>The problem that will concern us for the next two parts will be the initial value problem
$$\begin{cases}
\tag{\#}
-y^{\prime\prime} + q(x)y = \lambda y \text{ for $x\in[0,1]$,} \\
y(0) = a, y^{\prime}(0) = b.
\end{cases}$$
Here $q(x)$ lies in $L^2_\mathbb{C}([0,1])$, which we will recall to be the space of &lt;em>complex&lt;/em>-valued square-integrable functions on $[0,1]$. Also, $\lambda, a, b$ are complex numbers. In the future, we will only concern ourselves with real-valued $q$, but it is very convenient to work with complex-valued $q$ now, as it will let us avail ourselves of complex-analytic tools.&lt;/p></description></item></channel></rss>