<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Concomitant on Bughht Blog</title><link>https://bughht.github.io/tags/concomitant/</link><description>Recent content in Concomitant on Bughht Blog</description><generator>Hugo</generator><language>zh-CN</language><managingEditor>hhong6@mgh.harvard.edu (Haotian Hong)</managingEditor><webMaster>hhong6@mgh.harvard.edu (Haotian Hong)</webMaster><lastBuildDate>Thu, 09 Jul 2026 15:09:46 +0800</lastBuildDate><atom:link href="https://bughht.github.io/tags/concomitant/index.xml" rel="self" type="application/rss+xml"/><item><title>ACDC Dynamic B0 Field Control — Gordon Conference Showcase</title><link>https://bughht.github.io/intern_mgh/gordon_conference_acdc_showcases/</link><pubDate>Thu, 09 Jul 2026 15:09:46 +0800</pubDate><author>hhong6@mgh.harvard.edu (Haotian Hong)</author><guid>https://bughht.github.io/intern_mgh/gordon_conference_acdc_showcases/</guid><description>&lt;h1 id="acdc-dynamic-b0-field-control-additional-showcase"&gt;ACDC Dynamic B0 Field Control: Additional Showcase&lt;/h1&gt;
&lt;p&gt;&lt;strong&gt;Related Repositories:&lt;/strong&gt;&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;&lt;a href="https://github.com/bughht/ACDC_Optim"target="_blank" rel="external nofollow noopener noreferrer"&gt;bughht/ACDC_Optim&lt;/a&gt; — Shim waveform optimization solvers&lt;/li&gt;
&lt;li&gt;&lt;a href="https://github.com/bughht/concomitant_sim"target="_blank" rel="external nofollow noopener noreferrer"&gt;bughht/concomitant_sim&lt;/a&gt; — Concomitant field simulation toolkit&lt;/li&gt;
&lt;/ul&gt;
&lt;hr&gt;
&lt;h2 id="1-short-term-eddy-current-compensation-correcting-epi-edge-ghosts"&gt;1. Short-Term Eddy Current Compensation: Correcting EPI Edge Ghosts&lt;/h2&gt;
&lt;h3 id="the-problem"&gt;The Problem&lt;/h3&gt;
&lt;p&gt;In single-shot EPI, rapidly switching gradient waveforms induce &lt;strong&gt;short-term eddy currents&lt;/strong&gt;
(decay $\tau \sim 1$–$10$ ms) in the cryostat and surrounding conductors. These eddy
currents create a time-varying gradient bias during the EPI readout train that
manifests as &lt;strong&gt;Edge ghosts&lt;/strong&gt; superimposed on the primary image.&lt;/p&gt;</description></item><item><title>Concomitant Field Simulation</title><link>https://bughht.github.io/intern_mgh/concomitant_sim/</link><pubDate>Sat, 20 Dec 2025 15:09:46 +0800</pubDate><author>hhong6@mgh.harvard.edu (Haotian Hong)</author><guid>https://bughht.github.io/intern_mgh/concomitant_sim/</guid><description>&lt;h1 id="mri-concomitant-field-simulation-tool"&gt;MRI Concomitant Field Simulation Tool&lt;/h1&gt;
&lt;blockquote&gt;
&lt;p&gt;&lt;strong&gt;GitHub Repository&lt;/strong&gt;: &lt;a href="https://github.com/bughht/concomitant_sim"target="_blank" rel="external nofollow noopener noreferrer"&gt;bughht/concomitant_sim&lt;/a&gt;&lt;/p&gt;
&lt;/blockquote&gt;
&lt;p&gt;&lt;strong&gt;&lt;code&gt;concomitant_sim&lt;/code&gt;&lt;/strong&gt; is a fast, backend-agnostic Python package for simulating the phase accumulation caused by concomitant fields (Maxwell Terms) in MRI. It enables high-performance computations on both CPU and GPU by natively supporting NumPy arrays, PyTorch tensors, and CuPy arrays. The library uses an intelligent dispatching mechanism to adapt array operations to your inputs seamlessly.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 id="theoretical-modeling"&gt;Theoretical Modeling&lt;/h2&gt;
&lt;p&gt;The phase accumulation $\Phi_c$ caused by concomitant fields is modeled by integrating the magnetic field variation $\Delta B_c$ over time. Following the standard framework established by Bernstein et al. (1998), for a system with primary linear gradients, the concomitant field $B_c$ is approximated by second-order spatial terms:&lt;/p&gt;</description></item></channel></rss>