<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Quantum Mechanics on gdpark.blog</title><link>https://gdpark.blog/tags/quantum-mechanics/</link><description>Recent content in Quantum Mechanics on gdpark.blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Wed, 19 Aug 2015 00:00:00 +0000</lastBuildDate><atom:link href="https://gdpark.blog/tags/quantum-mechanics/index.xml" rel="self" type="application/rss+xml"/><item><title>Introduction to Quantum Mechanics: On Probability [Quantum Mechanics I Studied #1]</title><link>https://gdpark.blog/posts/quantum-mechanics-01-introduction-to-quantum-mechanics-on-probability/</link><pubDate>Mon, 10 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-01-introduction-to-quantum-mechanics-on-probability/</guid><description>Two weeks into quantum mechanics and already in full hair-loss mode — here&amp;rsquo;s my honest attempt to make sense of the Schrödinger equation and what a wave function even is.</description></item><item><title>Normalization [Quantum Mechanics I Studied #2]</title><link>https://gdpark.blog/posts/quantum-mechanics-02-normalization/</link><pubDate>Mon, 10 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-02-normalization/</guid><description>Why normalizing your wavefunction once is enough — turns out the Schrödinger equation secretly guarantees it stays normalized for all time.</description></item><item><title>The Momentum Operator [Quantum Mechanics I Studied #3]</title><link>https://gdpark.blog/posts/quantum-mechanics-03-the-momentum-operator/</link><pubDate>Tue, 11 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-03-the-momentum-operator/</guid><description>Cranking through the math to differentiate ⟨x⟩ with respect to time — and stumbling our way into the momentum operator.</description></item><item><title>The Time-Independent Schrödinger Equation [Quantum Mechanics I Studied #4]</title><link>https://gdpark.blog/posts/quantum-mechanics-04-the-time-independent-schr-dinger-equation/</link><pubDate>Tue, 11 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-04-the-time-independent-schr-dinger-equation/</guid><description>A breezy play-by-play of how Planck, Einstein, de Broglie, and Schrödinger loaded the bases and derived the time-independent Schrödinger equation — no mysticism required!</description></item><item><title>The Time-Independent Schrödinger Equation, Part 2 [Quantum Mechanics I Studied #5]</title><link>https://gdpark.blog/posts/quantum-mechanics-05-the-time-independent-schr-dinger-equation-part-2/</link><pubDate>Tue, 11 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-05-the-time-independent-schr-dinger-equation-part-2/</guid><description>We assume the wave function splits into space and time parts, plug it into the Schrödinger equation, and crank out two way simpler ODEs — same trick as E&amp;amp;M!</description></item><item><title>The Infinite Square Well [Quantum Mechanics I Studied #6]</title><link>https://gdpark.blog/posts/quantum-mechanics-06-the-infinite-square-well/</link><pubDate>Tue, 11 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-06-the-infinite-square-well/</guid><description>We dive into the infinite square well, crank through boundary conditions on the Schrödinger equation, and land on quantized wave functions — same moves as E&amp;amp;M, surprisingly!</description></item><item><title>The Harmonic Oscillator and Ladder Operators [Quantum Mechanics I Studied #7]</title><link>https://gdpark.blog/posts/quantum-mechanics-07-the-harmonic-oscillator-and-ladder-operators/</link><pubDate>Thu, 13 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-07-the-harmonic-oscillator-and-ladder-operators/</guid><description>We tackle case 2 of V(x) — the harmonic oscillator — unpack why springs are &lt;em>everywhere&lt;/em> in physics, then get into ladder operators to solve it.</description></item><item><title>Ladder Operators [Quantum Mechanics I Studied #8]</title><link>https://gdpark.blog/posts/quantum-mechanics-08-ladder-operators/</link><pubDate>Thu, 13 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-08-ladder-operators/</guid><description>We pick up the ladder-operator trick to climb from the ground state through every ψ_n, then chase down the normalization constants c_n and d_n purely in terms of n.</description></item><item><title>Algebraic Solution to the Harmonic Oscillator [Quantum Mechanics I Studied #9]</title><link>https://gdpark.blog/posts/quantum-mechanics-09-algebraic-solution-to-the-harmonic-oscillator/</link><pubDate>Fri, 14 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-09-algebraic-solution-to-the-harmonic-oscillator/</guid><description>Picking up right where we left off — muscling through the harmonic oscillator&amp;rsquo;s Schrödinger equation with a slick substitution and some algebraic tricks!</description></item><item><title>The Free Particle [Quantum Mechanics I Studied #10]</title><link>https://gdpark.blog/posts/quantum-mechanics-10-the-free-particle/</link><pubDate>Mon, 17 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-10-the-free-particle/</guid><description>We crack open the free particle case (V(x) = 0 everywhere) — it looks deceptively easy until two existential problems crash the party almost immediately.</description></item><item><title>The Delta-Function Potential [Quantum Mechanics I Studied #11]</title><link>https://gdpark.blog/posts/quantum-mechanics-11-the-delta-function-potential/</link><pubDate>Mon, 17 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-11-the-delta-function-potential/</guid><description>Time for the delta-function potential — we sort out bound vs. scattering states, meet the Dirac delta, and motivate why V(x) = −αδ(x) is a solid model for electrons in a material.</description></item><item><title>Delta-Function Potential: Scattering States and Quantum Tunneling [Quantum Mechanics I Studied #12]</title><link>https://gdpark.blog/posts/quantum-mechanics-12-delta-function-potential-scattering-states-and-quantum-tunne/</link><pubDate>Mon, 17 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-12-delta-function-potential-scattering-states-and-quantum-tunne/</guid><description>Tackling the E&amp;gt;0 case of the delta-function potential — scattering states, complex exponentials that refuse to die, and how tunneling actually works.</description></item><item><title>The Finite Square Well [Quantum Mechanics I Studied #13]</title><link>https://gdpark.blog/posts/quantum-mechanics-13-the-finite-square-well/</link><pubDate>Mon, 17 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-13-the-finite-square-well/</guid><description>Tackling the finite square well — the sneaky middle ground between the infinite well and the delta function — through bound states, boundary conditions, and all that fun stuff.</description></item><item><title>Formalism: Hilbert Space [Quantum Mechanics I Studied #14]</title><link>https://gdpark.blog/posts/quantum-mechanics-14-formalism-hilbert-space/</link><pubDate>Mon, 17 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-14-formalism-hilbert-space/</guid><description>We finally crack open the math behind quantum mechanics — why it works, where it came from, and how Heisenberg&amp;rsquo;s beach epiphany kicked the whole thing off.</description></item><item><title>Formalism: Observables and Hermitian Operators [Quantum Mechanics I Studied #15]</title><link>https://gdpark.blog/posts/quantum-mechanics-15-formalism-observables-and-hermitian-operators/</link><pubDate>Mon, 17 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-15-formalism-observables-and-hermitian-operators/</guid><description>Why measurement in QM always spits out real numbers — and how that forces every observable to be a Hermitian operator. (Daggers are literally knives, lol.)</description></item><item><title>Formalism: Determinate States [Quantum Mechanics I Studied #16]</title><link>https://gdpark.blog/posts/quantum-mechanics-16-formalism-determinate-states/</link><pubDate>Mon, 17 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-16-formalism-determinate-states/</guid><description>Transcribing Griffiths on determinate states — turns out demanding zero standard deviation just pops out the eigenvalue equation, and it all chains together beautifully.</description></item><item><title>The Uncertainty Principle [Quantum Mechanics I Studied #17]</title><link>https://gdpark.blog/posts/quantum-mechanics-17-the-uncertainty-principle/</link><pubDate>Tue, 18 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-17-the-uncertainty-principle/</guid><description>We derive the generalized uncertainty principle and chase down exactly when it hits its minimum — turns out the answer is when ψ is Gaussian, and here&amp;rsquo;s why!</description></item><item><title>Two-Level Systems [Quantum Mechanics I Studied #18]</title><link>https://gdpark.blog/posts/quantum-mechanics-18-two-level-systems/</link><pubDate>Tue, 18 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-18-two-level-systems/</guid><description>We set up a two-state quantum system with a 2×2 Hermitian Hamiltonian and crank out the eigenvalues and eigenvectors using the Schrödinger equation.</description></item><item><title>The Schrödinger Equation in Spherical Coordinates (3D) [Quantum Mechanics I Studied #19]</title><link>https://gdpark.blog/posts/quantum-mechanics-19-the-schr-dinger-equation-in-spherical-coordinates-3d/</link><pubDate>Wed, 19 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-19-the-schr-dinger-equation-in-spherical-coordinates-3d/</guid><description>We bump quantum mechanics up to 3D for the hydrogen atom, watch Cartesian coordinates immediately implode, and brace ourselves for the spherical coordinate nightmare.</description></item><item><title>The Hydrogen Atom [Quantum Mechanics I Studied #20]</title><link>https://gdpark.blog/posts/quantum-mechanics-20-the-hydrogen-atom/</link><pubDate>Wed, 19 Aug 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-20-the-hydrogen-atom/</guid><description>We finally plug the real hydrogen electric potential into the radial equation, grind through the algebra, and find R(r) — normalization and all.</description></item></channel></rss>