<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Project on ElectroOptical Innovations</title><link>https://electrooptical.net/tags/project/</link><description>Recent content in Project on ElectroOptical Innovations</description><generator>Hugo</generator><language>en-US</language><lastBuildDate>Fri, 20 Jun 2025 16:39:43 +0000</lastBuildDate><atom:link href="https://electrooptical.net/tags/project/index.xml" rel="self" type="application/rss+xml"/><item><title>SiPM Module</title><link>https://electrooptical.net/projects/sipm-module/</link><pubDate>Wed, 24 Feb 2021 20:21:59 +0000</pubDate><guid>https://electrooptical.net/projects/sipm-module/</guid><description>&lt;h3 id="specifications"&gt;Specifications&lt;/h3&gt;
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					&lt;td&gt;&lt;strong&gt;3dB Bandwidth&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;From DC–200 kHz to DC–300 MHz&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Rise Time&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;4ns (highest bandwidth configuration)&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Gain Control Method&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;Gain settable by serial or analog voltage. Analog voltage control profile mimics behaviour of similar PMT modules.&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Detector Type&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;Hammamatsu S13361/S13362 series or On Semi MicroFC series SiPm&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Coupling&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;DC&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Output Impedance&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;50 Ω&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Dynamic Range&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;All configurations support analog and photon counting&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Power Requirements&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;+5V 100mA, -5V 10mA&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Signal Output&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;SMA&lt;/td&gt;
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					&lt;td&gt;&lt;strong&gt;Applications&lt;/strong&gt;&lt;/td&gt;
					&lt;td&gt;Flow cytometry, Microplate readers, TOF Lidar&lt;/td&gt;
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&lt;p&gt;In the last year or two we&amp;rsquo;ve been doing a lot of work aimed at replacing photomultiplier tubes (PMTs) in instruments, using &lt;em&gt;avalanche photodiodes&lt;/em&gt; (APDs) and &lt;em&gt;silicon photomultipliers&lt;/em&gt; (SiPMs).  These devices are arrays of single-photon detectors, so they&amp;rsquo;re also known as &lt;em&gt;multi-pixel photon counters&lt;/em&gt; (MPPCs).  Our main application areas include biomedical instruments such as flow cytometers and microplate readers, which have to measure low light levels very precisely but don&amp;rsquo;t need the ultralow dark current of PMTs. (Follow-on articles will talk about our SiPM work in airborne lidar and SEM cathodoluminescence, as well as on improving the performance of actual PMTs.)&lt;/p&gt;</description></item><item><title>Silicon Photomultiplier (SiPM, MPPC) System for Cathodoluminescence</title><link>https://electrooptical.net/articles/silicon-photomultiplier-cathodoluminescence-detector/</link><pubDate>Thu, 30 Jan 2020 11:57:07 +0000</pubDate><guid>https://electrooptical.net/articles/silicon-photomultiplier-cathodoluminescence-detector/</guid><description>&lt;p&gt;In &lt;a href="https://electrooptical.net/articles/how-we-work/"&gt;How We Work&lt;/a&gt;, we gave an overview of how we build instruments, from the initial feasibility calculation (or &lt;em&gt;photon budget&lt;/em&gt;) to delivery of the first production units.&lt;/p&gt;
&lt;p&gt;Each project is different, of course, but there are common themes. Here&amp;rsquo;s a description of these steps from our most recent one at this writing (late January 2020), which is a low-cost cathodoluminescence detection system for use in scanning electron microscopes (SEMs).&lt;/p&gt;
&lt;h3 id="photon-budget"&gt;Photon Budget&lt;/h3&gt;
&lt;h4 id="cathodoluminescence-principles"&gt;Cathodoluminescence Principles&lt;/h4&gt;
&lt;p&gt;A SEM works by scanning a tightly-focused beam of high-energy electrons (1 keV - 30 keV) across a sample, and looking at the stuff that comes out. For ordinary imaging you usually look at backscattered and secondary electrons, but there are other modes. For instance, you can get a lot of information about the sample&amp;rsquo;s chemical composition by looking at the x-rays it emits. Most samples will also emit some amount of light, a process called &lt;a href="https://en.wikipedia.org/wiki/Cathodoluminescence"&gt;&lt;em&gt;cathodoluminescence&lt;/em&gt;&lt;/a&gt; .&lt;/p&gt;</description></item><item><title>How We Work: An Example</title><link>https://electrooptical.net/articles/how-we-work/</link><pubDate>Mon, 27 Jan 2020 17:00:58 +0000</pubDate><guid>https://electrooptical.net/articles/how-we-work/</guid><description>&lt;p&gt;&lt;em&gt;At EOI, we&amp;rsquo;ve been building advanced instruments very successfully for a long time. One reason for our success is our large inventory of working designs, and another is the way we go about doing it. This post walks through a typical sort of development plan for a challenging customer requirement. Here are the usual steps, in the form of a hypothetical email proposal outline for a fibre-coupled noninvasive glucose sensor similar to &lt;a href="https://electrooptical.net/blog/transcutaneous-blood-glucose-a-war-story/"&gt;this one.&lt;/a&gt;&lt;br&gt;
(You can also read about a &lt;a href="https://electrooptical.net/articles/silicon-photomultiplier-cathodoluminescence-detector/"&gt;recent project&lt;/a&gt; that went a lot like this, except with a single prototype stage.)&lt;/em&gt;&lt;/p&gt;</description></item></channel></rss>