Building a LaBr3:Ce Gamma Spectrometer
Posted: 20 Aug 2020, 04:01
So far my gamma spectroscopy setup consists of a HPGe and a NaI(Tl) scintillation detector.
The first costs me almost 2€ per day to run, assuming I keep it cold all the time, the other one has a resolution of “only” 6.8% FWHM.
As everyone who’s been bitten by the radbug I am always hunting for better resolution, ideally without a constant supply of liquid nitrogen.
A good solution for this are novel high resolution scintillators based on lanthanide halogenides.
Lanthanum Bromide is one of the cheapest in that class, but it suffers from high ¹³⁸La Background, an alternative to that would be Cerium Bromide.
A mixture of Lanthanum Bromide and Chloride is sold as LBC by Scionix, and it appears to offer the best resolution over all.
Sadly most of those are out of the price range of a hobbyist, but Ost Photonics (https://www.ost-photonics.com/) is selling LaBr3:Ce for a price that’s almost affordable by hobbyists.
I could not resist and bought their smallest variant, a 10×20 mm crystal in its hermetic seal.
When I bought it I was quickly informed that it will be produced now and a few days later I got a shipping notification, and the information that the crystal was measured at 2.57%(!) with a Hamamatsu R6231-100.
The important part is the -100, indicating a Super-Bialkali Photocathode, with a higher quantum efficiency. This results in a higher resolution, and with regular Bialkali “only” 3.1 to 3.4% can be achieved.
When the crystal arived it was packaged well, but the overall finish had a few things left to wish for. It was covered in epoxy, with some even on the window, and the Al case has some scratch marks. To be fair, those issues are of a purely cosmetic nature and don’t impact the crystals performance.
I decided to use this crystal with a Hamamtsu R9420-20 Bialkali PMT, because it is my best known-good tube.
Dow Corning high vacuum grease was used as optical coupling gel, because of its high viscosity and because it has proven itself in many detectors I’ve built so far. After coupling I wrapped the remaining area of the photocathode with teflon tape to reflect any stray photons. For the detector case I went with a proven method of aluminium endcaps on a stainless steel tube, as this provides both complete shielding and mechanical stability, as well as a low self absorption of gamma photons.
First I machined the endcap the detector would sit in, here it was important to make sure the walls were thin and the size was correct so the PMT would not sit with its photocathode right against it. Inside the cap the scintillator rests on a piece of sponge rubber, that gives a bit of mechanical padding but is basically invisible to gammas.
The outside wall of the endcap is 1 mm thick, the front surface has a thickness of 0.5 mm, giving me an absorption of about 50% at 19 keV, about 93% at 10 keV and ~5% at 30 keV.
I glued this endcap with black-colored epoxy to garantuee no light leaks, and after letting it cure over night I cleaned it up on the lathe. The other endcap housed connectors for high voltage and signal, namely SHV and BNC.
It is held in by three screws and made light-tight with an o-ring seal. And here we are, the mechanical part is finished! I really like how it turned out, almost looks like a professional detector.
Maybe the stainless steel parts needs a bit of engraving with the basic data on it, but that’s outside of my abilities at the moment.
First tests were successful, and I reached an astonishing 3.2% FWHM @ 609 keV!
My goal going into this was to get <4% to make the investment over NaI(Tl) worth it, and I have well surpassed that. A high resolution spectrometer makes it possible to separate more peaks in a compex spectrum, aiding in nuclide identification, as well as allowing for a quicker “first glance”, as narrower peaks stand out faster.
Here is where we get to the downsides of this detector.
Due to the small size it has a very low detection efficiency and needs a long time to collect a spectrum, especially at energies above a few 100 keV. This is a simple fact of the size and can’t be changed by a different PMT or similar measures, only by a bigger crystal.
Lanthanum bromide also suffers of a ¹³⁸La background, introducing both gamma peaks and beta continua. (intrinsic background of LaBr3:Ce
[broken link removed - Steven]
Because of the crystal size there’s low Lanthanum activity and the detection efficiency of its own gammas is not very high, so it only becomes visible after a long measurement. But then again, so do all higher energy gamma peaks.
The following two images are 10 hour background spectra, taken behind 5 cm of lead in every direction, the most dominant feature is the lead fluorescense, but one can see the bg spectrum shown above pretty well. The following spectrum is of ²³²Th and its decay products, one can nicely see all the peaks of its decay chain. Most notably are the two ²²⁸Ac peaks at 911 and 969 keV respectively , which are hard to separate with NaI(Tl), but go down to the baseline with LaBr.
Compare this to the spectrum taken by NaI(Tl): One interesting note is that LaBr is so bright that my 8 dynode PMT only needed a bias of ~500V to get a good spectrum, where others need almost twice that for NaI. This might pave the way for low power devices running at lower voltages, well in the range of where Geiger Müller counters usually are the standard.
Overall I am very happy how this detector turned out and I am sure that many more experiments will follow with it!
I’d love to see more hobbyists be motivated to spend the extra on high resolution spectrometers as they get more affordable. This detector was a total of about 500€ in materials cost, plus ~10 hours for manufacture and assembly of the housing.
I'd also want to thank Luuk, who has helped me a lot here and always pointed me in the right way, as there are many new things to learn with those high rez scintillators!
Best regards,
Lukas
(Copied from: https://gigabecquerel.wordpress.com/202 ... ctrometer/)
The first costs me almost 2€ per day to run, assuming I keep it cold all the time, the other one has a resolution of “only” 6.8% FWHM.
As everyone who’s been bitten by the radbug I am always hunting for better resolution, ideally without a constant supply of liquid nitrogen.
A good solution for this are novel high resolution scintillators based on lanthanide halogenides.
Lanthanum Bromide is one of the cheapest in that class, but it suffers from high ¹³⁸La Background, an alternative to that would be Cerium Bromide.
A mixture of Lanthanum Bromide and Chloride is sold as LBC by Scionix, and it appears to offer the best resolution over all.
Sadly most of those are out of the price range of a hobbyist, but Ost Photonics (https://www.ost-photonics.com/) is selling LaBr3:Ce for a price that’s almost affordable by hobbyists.
I could not resist and bought their smallest variant, a 10×20 mm crystal in its hermetic seal.
When I bought it I was quickly informed that it will be produced now and a few days later I got a shipping notification, and the information that the crystal was measured at 2.57%(!) with a Hamamatsu R6231-100.
The important part is the -100, indicating a Super-Bialkali Photocathode, with a higher quantum efficiency. This results in a higher resolution, and with regular Bialkali “only” 3.1 to 3.4% can be achieved.
When the crystal arived it was packaged well, but the overall finish had a few things left to wish for. It was covered in epoxy, with some even on the window, and the Al case has some scratch marks. To be fair, those issues are of a purely cosmetic nature and don’t impact the crystals performance.
I decided to use this crystal with a Hamamtsu R9420-20 Bialkali PMT, because it is my best known-good tube.
Dow Corning high vacuum grease was used as optical coupling gel, because of its high viscosity and because it has proven itself in many detectors I’ve built so far. After coupling I wrapped the remaining area of the photocathode with teflon tape to reflect any stray photons. For the detector case I went with a proven method of aluminium endcaps on a stainless steel tube, as this provides both complete shielding and mechanical stability, as well as a low self absorption of gamma photons.
First I machined the endcap the detector would sit in, here it was important to make sure the walls were thin and the size was correct so the PMT would not sit with its photocathode right against it. Inside the cap the scintillator rests on a piece of sponge rubber, that gives a bit of mechanical padding but is basically invisible to gammas.
The outside wall of the endcap is 1 mm thick, the front surface has a thickness of 0.5 mm, giving me an absorption of about 50% at 19 keV, about 93% at 10 keV and ~5% at 30 keV.
I glued this endcap with black-colored epoxy to garantuee no light leaks, and after letting it cure over night I cleaned it up on the lathe. The other endcap housed connectors for high voltage and signal, namely SHV and BNC.
It is held in by three screws and made light-tight with an o-ring seal. And here we are, the mechanical part is finished! I really like how it turned out, almost looks like a professional detector.
Maybe the stainless steel parts needs a bit of engraving with the basic data on it, but that’s outside of my abilities at the moment.
First tests were successful, and I reached an astonishing 3.2% FWHM @ 609 keV!
My goal going into this was to get <4% to make the investment over NaI(Tl) worth it, and I have well surpassed that. A high resolution spectrometer makes it possible to separate more peaks in a compex spectrum, aiding in nuclide identification, as well as allowing for a quicker “first glance”, as narrower peaks stand out faster.
Here is where we get to the downsides of this detector.
Due to the small size it has a very low detection efficiency and needs a long time to collect a spectrum, especially at energies above a few 100 keV. This is a simple fact of the size and can’t be changed by a different PMT or similar measures, only by a bigger crystal.
Lanthanum bromide also suffers of a ¹³⁸La background, introducing both gamma peaks and beta continua. (intrinsic background of LaBr3:Ce
[broken link removed - Steven]
Because of the crystal size there’s low Lanthanum activity and the detection efficiency of its own gammas is not very high, so it only becomes visible after a long measurement. But then again, so do all higher energy gamma peaks.
The following two images are 10 hour background spectra, taken behind 5 cm of lead in every direction, the most dominant feature is the lead fluorescense, but one can see the bg spectrum shown above pretty well. The following spectrum is of ²³²Th and its decay products, one can nicely see all the peaks of its decay chain. Most notably are the two ²²⁸Ac peaks at 911 and 969 keV respectively , which are hard to separate with NaI(Tl), but go down to the baseline with LaBr.
Compare this to the spectrum taken by NaI(Tl): One interesting note is that LaBr is so bright that my 8 dynode PMT only needed a bias of ~500V to get a good spectrum, where others need almost twice that for NaI. This might pave the way for low power devices running at lower voltages, well in the range of where Geiger Müller counters usually are the standard.
Overall I am very happy how this detector turned out and I am sure that many more experiments will follow with it!
I’d love to see more hobbyists be motivated to spend the extra on high resolution spectrometers as they get more affordable. This detector was a total of about 500€ in materials cost, plus ~10 hours for manufacture and assembly of the housing.
I'd also want to thank Luuk, who has helped me a lot here and always pointed me in the right way, as there are many new things to learn with those high rez scintillators!
Best regards,
Lukas
(Copied from: https://gigabecquerel.wordpress.com/202 ... ctrometer/)