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Category Archives: PMT/Scintillation Processor

A Custom Base for using the EMI/Thorn 9816B Photomultiplier Tube with the Products for Research Model TE-182 Thermoelectrically-Cooled PMT Housing for Ultra-Low Light Level Experiments

Posted on May 27, 2021 by David Prutchi Posted in Photomultipliers, PMT/Scintillation Processor

For a detailed writeup in pdf format please CLICK HERE

I’ve been planning some experiments with single-photon and ultra-low light levels. For these experiments I want the collection area to be large and for the detector to have very broad spectral response, so my preference is to use a photomultiplier tube (PMT) instead of a “silicon photomultiplier” avalanche single-photon detector.

I found a brand new EMI 9816B PMT on eBay® which meets my requirements. The 9816B is a 51 mm (2”) diameter end-window photomultiplier, with an S20 infrared-sensitive photocathode, and 14 BeCu dynodes of linear focused design. This tube features a very high gain of 25×106 A/lm under nominal conditions (2,200V) with a quantum efficiency of 21% at the peak response wavelength.

Integration time, and ultimately resolution and sensitivity for detecting single-photons or ultra-weak light levels are dependent on the noise floor (dark counts) which is a function of temperature. Cooling the PMT dramatically reduces its dark current and counts.

I bought a surplus thermoelectrically-cooled housing by Products for Research (Model TE-182) which is made for 2” end-window PMTs. I could not find a surplus base for the EMI 9816B 14-dynode PMT, so I decided to buy a surplus base for a different tube and modify it for the 9816B.

Products for Research TE-182 Thermoelectrically-Cooled Housing for 2″ PMTs

Clearing the inside of the base was a very messy affair. This is because the dynode voltage divider chain is partially potted in silicone, and the rest of the base is filled with expanding thermal-isolation foam. Part of the base is made of plastic, so the use of harsh chemical solvents or heat to remove the silicone rubber and expanding foam were not possible. I thus had to use a scalpel and dental picks to remove all this insulation and be able to disassemble the tube socket.

I built a new divider on a piece of phenolic breadboard . The base is wired for high voltage (-2,300V) applied to the cathode (through a 33kΩ resistor). The dynode_1-to-dynode_14 divider is built with 330kΩ resistors. As suggested by EMI, the cathode-to-focus (and dynode_1) is set at a fixed 300V difference using two 150V Zener diodes in series.

Results from a characterization run are shown in the following table. The room-temperature dark current agrees with the specified value. A very dramatic drop in dark current and dark count rate can be observed when the PMT is cooled.

For a detailed writeup in pdf format please CLICK HERE

Elegant Experiment to Measure Planck’s Constant using Photons from Distant Star

Posted on March 9, 2021 by David Prutchi Posted in Chapter 2 - Light as Particles, PMT/Scintillation Processor

Javier De Elias Cantalapiedra from Madrid, Spain posted the YouTube video above to show his very elegant experiment in which he measured Planck’s constant using photons from a distant star.  As in the e/m measurement he had previously shared with us, his experimental technique is very rigorous, which yielded Planck’s constant with just 5% error.  This is remarkable given the method he applied.

Javier is an industrial engineer who works in the telecommunications industry.  However, his passion is physics, which he pursues at a (very high) amateur level.

Thank you Javier for sharing!

Using the $79 SainSmart DSO201 Pocket Oscilloscope and GammaGrapher with the PMT/Scintillation Probe

Posted on September 21, 2012 by David Prutchi Posted in Chapter 2 - Light as Particles, Chapter 3 - Atoms and Radioactvity, Chapter 5 - Wave-Particle Duality, Compton Scattering, MCA/PHA, Photomultipliers, PMT/Scintillation Processor, Scintillation Detector, Single-Photon Experiments

Connects directly to PMT probe shown in the book’s Figure 30 with no need for PMT amplifier!

 

Freeware Gamma Grapher MCA with diy PMT Scintillation Probe by David and Shanni Prutchi diyPhysics.com

The nice guys at the Yahoo GammaSpectrometry Group developed multichannel analyzer software for the $79 SainSmart DSO201 Pocket-Sized Digital Oscilloscope.  The upload of the MCA software to the oscilloscope is really easy (via USB), and it allows the PMT probe shown in the book’s Figure 30 to be connected directly to the oscilloscope’s input with no need for a PMT amplifier!

Continue reading→

Simple d.i.y. Bias-T for Scintillation Probes with Single Connector

Posted on February 20, 2012 by David Prutchi Posted in Chapter 3 - Atoms and Radioactvity, Chapter 4 - The Priciple of Quantum Physics, MCA/PHA, Photomultipliers, PMT/Scintillation Processor, Radio-Isotope Identification

diy Signal/High-Voltage Splitter for Scintillation Probe with Single Connector David Prutchi www.diyphysics.comMany surplus scintillation probes have a single connector through which the PMT is fed with high voltage and the anode signal is output.  However, this may require an external “Bias-T” (a high voltage / signal splitter) to connect the probe to a high-voltage power supply that is separate from the PMT amplifier/processor. Continue reading→

Simple d.i.y. Low-Pass Filter for Interfacing PMT Amplifier to PC Sound Card (Used with Free “Pulse Recorder and Analyser” Software MCA)

Posted on February 20, 2012 by David Prutchi Posted in Chapter 5 - Wave-Particle Duality, MCA/PHA, PMT/Scintillation Processor, Radio-Isotope Identification

diy low pass filter interface between photomultiplier scintillation probe amplifier and PRA by David Prutchi Ph.D. www.diyPhysics.comFigure 34 in the book shows the schematic diagram for our photomultiplier tube (PMT) signal processing circuit has an analog output that is suitable for use with a sound-card-based multichannel pulse-height analyzer (MCA).  However, if you already have a commercial scintillation processor that you would like to use with PRA, then you will somehow need to extend the typically narrow output pulses (e.g. 1 to 10 microseconds) so that they can be acquired through the sound card. Continue reading→

Converting a DT-590A/PDR-56F “X-Ray” Probe into a General-Purpose NaI(Tl) Gamma Probe

Posted on February 1, 2012 by David Prutchi Posted in Chapter 3 - Atoms and Radioactvity, Ionizing Radiation Detection, PMT/Scintillation Processor, Scintillation Detector

PDR56 probe modification for general-purpose gamma detection

The military Radiac Set, AN/PDR-56 is a portable scintillation type instrument used for detection of alpha contamination. The system includes a large and small interchangeable probe with a probe extension.  This system is being phased out by the US Air Force, so new probes are becoming widely available in the surplus market.

The “x-ray” probe for the AN/PDR-56 uses a CaF2(Eu) scintillator/photomultiplier combination to detect the 14-21 keV gammas from Pu-239. The x-ray probe is an assembly which includes the amplifier-discriminator circuits integral to the phototube scintillator housing. The discriminator is a single channel analyzer adjusted to detect Pu-239 gamma rays. Continue reading→

d.i.y. Handheld Multichannel Analyzer (MCA) based on 16F877 PIC Microcontroller and LCD

Posted on February 1, 2012 by David Prutchi Posted in Ionizing Radiation Detection, MCA/PHA, PMT/Scintillation Processor, Radio-Isotope Identification

Isotope gama spectra obtained with d.i.y. multichannel analyzer (MCA)

Some time ago I was developing a medical instrument which required histogramming, which got me in the mood to retake my own PIC MCA project(http://home.comcast.net/~prutchi/index_files/scint.htm ).   I used the variable RAM in the microcontroller (16F877), so I limited the number of channels to 95 and let the histogram run until some channel reaches 240 counts (the highest 8-bit number that yields an integer when divided by 8 which is also divisible by the 30 pixel height of the LCD). The firmware then displays the spectrum as a bar with a maximum height of 30 pixels for each one of the 95 channels. Continue reading→

Prototyping PCB for d.i.y. Photomultiplier (PMT) Amplifier/Processor

Posted on January 31, 2012 by David Prutchi Posted in Chapter 2 - Light as Particles, Chapter 3 - Atoms and Radioactvity, Chapter 7 - Schrödinger's Wave Equation, Compton Scattering, Ionizing Radiation Detection, Photomultipliers, PMT/Scintillation Processor, Scintillation Detector, Single-Photon Experiments

Printed circuit board for diy PMT amplifier, processor, discriminator and scintillator detector

We built the bulk of our PMT amplifier/processor/discriminator on a Universal PDIP Operational Amplifier Evaluation Module by Texas Instruments (model OPAMPEVM-PDIP).  Click on the picture above for a full-size version of the picture.

The diagram in the following pdf file shows the connection layout for the circuit shown in the book’s Figure 34: PMT Processor PCB  Continue reading→

diy PMT Pulse Processor Suitable For Use With “Pulse Recorder and Analyser (PRA)” MCA

Posted on January 20, 2012 by David Prutchi Posted in Chapter 2 - Light as Particles, Chapter 5 - Wave-Particle Duality, Compton Scattering, Ionizing Radiation Detection, MCA/PHA, Photomultipliers, PMT/Scintillation Processor, Scintillation Detector, Single-Photon Experiments 2 Comments

diy Photomultiplier Processor

Figure 34 in the book shows the schematic diagram for the photomultiplier tube (PMT) signal processing circuit that amplifies the narrow pulses detected by the PMT probe.  The discriminator stage removes small pulses produced by thermal noise in the tube.  A pulse stretcher outputs pulses that can be heard on a speaker.  In addition, the analog output is suitable for use with a sound-card-based multichannel pulse-height analyzer (MCA). Continue reading→

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