<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Products on ElectroOptical Innovations</title><link>https://electrooptical.net/categories/products/</link><description>Recent content in Products on ElectroOptical Innovations</description><generator>Hugo</generator><language>en-US</language><lastBuildDate>Tue, 06 Jan 2026 20:40:16 +0000</lastBuildDate><atom:link href="https://electrooptical.net/categories/products/index.xml" rel="self" type="application/rss+xml"/><item><title>Featured Product: LA-22 Low Noise Lab Amplifier</title><link>https://electrooptical.net/blog/new-product-la-22-low-noise-lab-amplifier/</link><pubDate>Tue, 06 Jan 2026 13:08:08 +0000</pubDate><guid>https://electrooptical.net/blog/new-product-la-22-low-noise-lab-amplifier/</guid><description>&lt;h3 id="the-la-22-low-noise-laboratory-amplifier-800-hz22mhz-11-nv--hz"&gt;The LA-22 Low-Noise Laboratory Amplifier, 800 Hz–22 MHz, 1.1 nV / √Hz&lt;/h3&gt;
&lt;p&gt;One problem that comes up again and again in doing measurements is that we need the apparatus to be quieter than the thing we&amp;rsquo;re measuring, ideally by at least a factor of two.   Besides quiet, it should be wideband, have an accurately known gain that&amp;rsquo;s flat with frequency, have a clean step response, and generally do its job while keeping itself out of the way.  There&amp;rsquo;s a wealth of detail in our &lt;a href="https://electrooptical.net/media/uploads/photoreceiver_testing_system_0_1_2.pdf"&gt;app note AN-1&lt;/a&gt;
 on photoreceiver testing.&lt;/p&gt;</description></item><item><title>A High-Performance Time Domain Reflectometer</title><link>https://electrooptical.net/blog/a-high-performance-time-domain-reflectometer/</link><pubDate>Wed, 05 Mar 2025 15:22:56 +0000</pubDate><guid>https://electrooptical.net/blog/a-high-performance-time-domain-reflectometer/</guid><description>&lt;p&gt;In &lt;a href="https://electrooptical.net/blog/150-ps-tdr-for-under-2/" title="A 150-Picosecond- TDR Sampler for $2"&gt;a previous article&lt;/a&gt;, we described an ultralow-cost time-domain reflectometer (TDR) that  is used as a radar dipstick for fuel gauges in heavy equipment.  Its 150-ps edges were better than good enough, and its rock-bottom BOM cost ($1.30 @ 100 pcs) made it possible for the whole gauge to retail for under $40.  That performance is far from the limit for low-cost samplers, as we&amp;rsquo;ll see.&lt;/p&gt;</description></item><item><title>Product Announcement: QL03 Photoreceiver</title><link>https://electrooptical.net/blog/product-announcement-ql03-photoreceiver/</link><pubDate>Wed, 19 Feb 2025 18:33:55 +0000</pubDate><guid>https://electrooptical.net/blog/product-announcement-ql03-photoreceiver/</guid><description>&lt;p&gt;&lt;a href="https://hobbs-eo.com/products/ql03-photoreceiver" title="QL03 Photoreceiver"&gt;&lt;img src="https://hobbs-eo.com/cdn/shop/files/IMG_4895.jpg?v=1739847977" alt="" loading="lazy"&gt;&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;We’ve got a new photoreceiver available over at our sister site, &lt;a href="https://hobbs-eo.com/"&gt;&lt;strong&gt;Hobbs ElectroOptics&lt;/strong&gt;&lt;/a&gt;. The &lt;strong&gt;QL03 Photoreceiver&lt;/strong&gt; comes out of several proof-of-concept systems where we needed a high-sensitivity, low-noise optical receiver for low-light applications.&lt;/p&gt;
&lt;p&gt;It features a &lt;strong&gt;massive 150 mm² photodiode&lt;/strong&gt; with slight magnification from an immersion lens, making it especially effective for diffuse light measurements, spectroscopy, and fluorescence detection—plus, setup is a breeze since you’re aiming at a barn door.&lt;/p&gt;</description></item><item><title>Silicon Photomultiplier Module Design</title><link>https://electrooptical.net/blog/silicon-photomultiplier-module-design/</link><pubDate>Mon, 25 Jan 2021 16:30:28 +0000</pubDate><guid>https://electrooptical.net/blog/silicon-photomultiplier-module-design/</guid><description>&lt;p&gt;Internal Developments&lt;/p&gt;
&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></channel></rss>