<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Blog Posts on Edgar Ivan Hinojosa</title><link>https://edgarivanhinojosa.xyz/blogs/</link><description>Recent content in Blog Posts on Edgar Ivan Hinojosa</description><generator>Hugo</generator><language>en-us</language><lastBuildDate>Sun, 15 Feb 2026 23:35:59 -0600</lastBuildDate><atom:link href="https://edgarivanhinojosa.xyz/blogs/index.xml" rel="self" type="application/rss+xml"/><item><title>The Reflection Identity of the Gamma Function via Complex Integration</title><link>https://edgarivanhinojosa.xyz/blogs/gamma-identidad/</link><pubDate>Sun, 15 Feb 2026 23:35:59 -0600</pubDate><guid>https://edgarivanhinojosa.xyz/blogs/gamma-identidad/</guid><description>&lt;p>The reflection identity of the gamma function is:&lt;/p>
&lt;p>\begin{equation}
\Gamma( z ) \Gamma( 1-z ) = \frac{\pi}{\sin( \pi z ) }
\end{equation}&lt;/p>
&lt;p>We can start from the definition of $\beta( 1- \alpha, \alpha ) $&lt;/p>
&lt;p>\begin{align}
\Gamma( 1- \alpha ) \Gamma( \alpha ) &amp;amp;= \beta ( 1- \alpha, \alpha ) = \int^\infty_0 \frac{t ^{1- \alpha-1}dt}{( 1+ t )^{1- \alpha+ \alpha} } \\
&amp;amp;= \int^\infty_0 \frac{t ^{-\alpha} dt}{1 + t} \\
&amp;amp;= \int^\infty_{-\infty} \frac{e ^{-\alpha x} e^x dx}{1+ e^x} = \int^\infty_{-\infty} \frac{e ^{( 1-\alpha )x }}{ 1 + e^{x}} = I
\end{align}&lt;/p></description></item><item><title>General Lorentz Transformation via Group Generators</title><link>https://edgarivanhinojosa.xyz/blogs/lorentz-transform/</link><pubDate>Thu, 12 Feb 2026 15:52:52 -0600</pubDate><guid>https://edgarivanhinojosa.xyz/blogs/lorentz-transform/</guid><description>&lt;p>In this post we derive the functional form of a generic Lorentz transformation from its group generators.
At first glance I considered this trivial, as I was unaware of the role played by their non-commutativity — which made it an interesting exercise to present.
We follow Chapter 11 of Jackson (Third Edition), which makes use of the mathematical properties of Minkowski spacetime.
Clarifications missing from the book are supplied with original arguments.&lt;/p></description></item></channel></rss>