random thoughts of an engineer

 Introduction External cavity diode laser (ECDL) combines benefits of laser diodes and DPSS lasers. The semiconductor chip provides easy to pump, efficient, high gain medium while the external cavity allows tailoring device performance.  Wavelength selective elements, like diffraction gratings or etalons can be added to the resonator to reduce emission spectrum, saturable absorber can be added for mode-locking, partially reflective mirror in conjunction with RF modulation can be used for frequency comb generation and many more. In this article, we will try to design simplest, ECDL that'll be used in future experiments so state tuned! How it works There are many great internet sources describing how ECLD works, so let's just quickly recap. Out of the box laser diode has relative wide emission bandwidth, usually around 1-2nm. This is because the gain bandwidth of diode is relative wide and the resonator works with relatively weak coupling (output mirror has reflectivity of 32

But why? Recently, I decided to implement digital emulation of all my current eurorack modules . That way, I'll be able to share them with everyone to play and experiment before they decided to spend cash on an actual module. There's just one big obstacle in a way - SSH uses analog switches driven by comparators in the signal path. While analog switches can be nicely modeled with multiplication, I was unable to find any publications regarding accurate modeling of comparators. Naive approach The simplest way to try to model an analog comparator would be to use a digital comparator. Unfortunately, while simple, this solution suffers from a great amount of aliasing. It can be thought of in two different ways. One is that digital comparator outputs bandwidth unlimited step at the output leading to great aliasing, another is that digital comparator works in discrete time so can't sense when exactly the threshold has been crossed. Oversampling One, often thrown around, method of

The inspiration I'd like to share the details of my journey in acquiring an orange laser for my desk. Some of you might know that I initially dabbled with dye lasers. While they are impressive in terms of the range of colors they can produce (with a single dye capable of spanning half the rainbow, and a mixture of dyes covering nearly the entire visible spectrum), they come with the drawback of requiring Q-switched pumping or a complex setup involving dye jets and recirculation. These setups tend to be neither compact nor quiet. Furthermore, every lab I visited with dye lasers seemed to have tables and floors stained with dyes, creating a fluorescent environment. Clearly, I needed to explore alternative options. Another options Ideally, using a laser diode would be the best solution. Unfortunately, due to technical limitations, there are no laser diodes available between 525nm and 630nm at room temperature.. The AlGaInP have quite high temperature dependence of up to

 What is ModuGlow?  ModuGlow is modern, modular, organic lamp that can be anything between night lamp to art sculpture. It's built from 10x10cm panels containing 25 blinking bulbs. It can be stacked in 2 axis to provide arbitrary size lamp. Video showing 2x2 combination working. Neon behavior Neon bulbs exhibit S type dynamic negative resistance. If you understood last sentence feel free to skip this paragraph. Negative dynamic resistance is a behavior of some electric circuits when with increasing current current decreases or the other way around with increasing voltage current decreases. In neon bulbs it manifests itself between strike and maintain voltage. When bulb strikes the voltage starts to drop due to series resistor. Dropping voltage makes bulb want to draw more power further lowering voltage until negative resistance region ends near maintain voltage. That way bulb "turns on" at higher, striking voltage while "maintains on" at lower maintaining voltag

The purpose of this blog post is to describe the process of connecting a MEMS microphone with PDM to a microcontroller, and the steps taken to optimize the PDM-to-microcontroller data processing for better performance. Introduction In my latest research I'm in need to connect MEMS microphone with Pulse Density Modulation (PDM) to micro-controller to evaluate their parameters. In contrary to more popular Pule Code Modulation (PCM) that sends data at reasonable sample rate (40-192khz) with wide words (8-24 bits) PDM sends one bit stream at Mhz sample rate straight from sigma-delta modulator. To do anything useful with this stream it needs to be decimated to lower sample rate while increasing word width and filtering out high frequency noise. My microphone generates PDM stream at around 3Mhz. I want to downsample it around 40khz to feed my "standard" software DSP to have enough time to process data. Why? Decimating signal is as simple as selecting one sample every N and d

 As promised this is update to last post about our PCB holders. Technical difficulties It turns out that if I want tapped hole every 10mm that's a lot of tapping. Additionally tapping steel is quite hard, especially with such small tap. Most companies decided that they don't want to do such job, one that agreed is research institution so I guess they're used to nontrivial requirements. After some negotiations we got price of almost 5k euro for 300x300mm sheet. That's a bit too much for this project. Required changes My changing steel to aluminum and moving holes onto 15x15 grid we considerably reduced required engineering time. After initial testing it turned out that 15x15 hole spacing is more than sufficient, but swapping to aluminum means magnetic mounts are no longer an option. I guess it's low price to pay to reduce manufacturing cost to 740 euros. plates when they first arrived in our lab   Designed mounts We designed few mounts for plates to mount things on t