<?xml version="1.0" encoding="utf-8"?><feed xmlns="http://www.w3.org/2005/Atom" ><generator uri="https://jekyllrb.com/" version="3.10.0">Jekyll</generator><link href="https://minghaoguo.org/feed.xml" rel="self" type="application/atom+xml" /><link href="https://minghaoguo.org/" rel="alternate" type="text/html" /><updated>2026-10-09T05:56:07+00:00</updated><id>https://minghaoguo.org/feed.xml</id><title type="html">Minghao Guo</title><subtitle>personal description</subtitle><author><name>Minghao Guo (郭明浩)</name><email>minghao.g@columbia.edu</email><uri>https://minghaoguo.org/</uri></author><entry><title type="html">Cyclic Zoom</title><link href="https://minghaoguo.org/posts/2025/07/cyclic-zoom/" rel="alternate" type="text/html" title="Cyclic Zoom" /><published>2025-07-08T00:00:00+00:00</published><updated>2025-07-08T00:00:00+00:00</updated><id>https://minghaoguo.org/posts/2025/07/cyclic-zoom</id><content type="html" xml:base="https://minghaoguo.org/posts/2025/07/cyclic-zoom/"><![CDATA[<h1 id="in-n-out">In-N-Out</h1>

<p>The challenge of simulating accretion and feedback from SMBHs to galactic scales is the vast range of spatial and temporal scales. To tackle this problem, we repeatedly zoom out (derefine) and zoom in (refine) the simulation domain, which we denote as the ‘‘cyclic zoom’’ method. The spatial resolution is correspondingly decreased (increased) when we zoom out (in) using AMR to alleviate the time step constraints while keeping the same relative resolution \(\Delta x/x\) for the region of interest. A mask region in the center is used to preserve the small-scale physics. 
The cyclic zoom method in a spacetime diagram behaves like a ‘’\(\Lambda\)-cycle’’ in the spacetime diagram (or ‘‘V-cycle’’, depending on what we choose as the starting point of the simulation). A complete simulation typically consists of tens to hundreds of \(\Lambda\)-cycles.</p>]]></content><author><name>Minghao Guo (郭明浩)</name><email>minghao.g@columbia.edu</email><uri>https://minghaoguo.org/</uri></author><category term="cycle of life" /><category term="numerical method" /><category term="GRMHD" /><summary type="html"><![CDATA[In-N-Out]]></summary></entry><entry><title type="html">Zoom In</title><link href="https://minghaoguo.org/posts/2024/10/zoom-in/" rel="alternate" type="text/html" title="Zoom In" /><published>2024-10-01T00:00:00+00:00</published><updated>2024-10-01T00:00:00+00:00</updated><id>https://minghaoguo.org/posts/2024/10/zoom-in</id><content type="html" xml:base="https://minghaoguo.org/posts/2024/10/zoom-in/"><![CDATA[<h1 id="all-the-way-down-to-the-event-horizon">All the way down to the event horizon</h1>

<p>The challenge of simulating accretion and feedback from SMBHs to galactic scales is the vast range of spatial and temporal scales. To tackle this problem, we repeatedly zoom out (derefine) and zoom in (refine) the simulation domain, which we denote as the ‘‘cyclic zoom’’ method. The spatial resolution is correspondingly decreased (increased) when we zoom out (in) using AMR to alleviate the time step constraints while keeping the same relative resolution \(\Delta x/x\) for the region of interest. A mask region in the center is used to preserve the small-scale physics. 
The cyclic zoom method in a spacetime diagram behaves like a ‘’\(\Lambda\)-cycle’’ in the spacetime diagram (or ‘‘V-cycle’’, depending on what we choose as the starting point of the simulation). A complete simulation typically consists of tens to hundreds of \(\Lambda\)-cycles.</p>]]></content><author><name>Minghao Guo (郭明浩)</name><email>minghao.g@columbia.edu</email><uri>https://minghaoguo.org/</uri></author><category term="galaxy to horizon" /><category term="numerical method" /><category term="GRMHD" /><summary type="html"><![CDATA[All the way down to the event horizon]]></summary></entry></feed>