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Author Archives: David Prutchi

Using Surplus Photonis XP2422/SN PMTs in Scintillation Probes

Posted on April 8, 2013 by David Prutchi Posted in Chapter 2 - Light as Particles, Chapter 5 - Wave-Particle Duality, Ionizing Radiation Detection, MCA/PHA, Photomultipliers, Radio-Isotope Identification, Scintillation Detector

XP2422/SN PMT Photomultiplier David Prutchi PhD

We prepared a short note on how to build a dynode voltage divider network for inexpensive surplus XP2422/SN photomultiplier tubes.  The XP2422/SN PMT is especially suited for gamma-ray spectral analysis when coupled to a NaI(Tl) scintillation crystal because of its high pulse-height resolution (PHR).  The XP2422/SN is available from Sphere Research in Canada.

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Schematics for Fast Pulse Amplifier for Macroscopic Entanglement Detection

Posted on April 7, 2013 by David Prutchi Posted in Chapter 8 - Entanglement, Entanglement, Photon/Coincidence Counter, Single-Photon Counting Modules (SPCMs)

Fast pulse amplifier for macro entanglement detectionA recent paper entitled “Displacing entanglement back and forth between the micro and macro domains” discusses the experimental possibility of displacing quantum entanglement into the domain where it involves two macroscopically distinct states, i.e. two states characterized by a large enough number of photons.  Specifically, the authors describe the process by which they start with two entangled spatially separated optical modes at the single photon level and subsequently displace one of these modes up to almost a thousand photons.

With so many photons, it would be possible, at least in principle, to see entangled photon pulses with our eyes.  This would also make it possible to perform entanglement experiments with linear coarse-grain detectors (NOT single-photon detectors).

Mathieu Stephan, a high speed electronics engineer at the Swiss quantum information systems company id Quantique SA (and prolific hardware hacker) designed the very fast pulse amplifiers needed to acquire signals from avalanche photodiodes for this experiment.  He has posted a thorough description of his design on his blog: http://www.limpkin.fr.

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In Memoriam – Dr. Akira Tonomura (1942-2012)

Posted on April 2, 2013 by David Prutchi Posted in Chapter 5 - Wave-Particle Duality, Single-Electron Experiments

photo_tonomuraWe recently learned the sad news that Dr. Akira Tonomura – a truly great experimentalist – passed away on May 2, 2012 during the course of treatment on pancreatic cancer.

We have been great admirers of Dr. Tonomura.  Our blog’s banner is a cartoon representation of an experimental setup developed by Dr. Tonomura, through which in 1986 he showed single-electron buildups of electron wave interference fringe patterns. This experiment clearly revealed the dual nature of electrons and was described by Physics World magazine as the world’s most beautiful physics experiment, ranking above the historical experiments of Galileo Galilei and Robert Millikan.

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Construction of a d.i.y. Thermoelectrically-Cooled Photomultiplier Tube (PMT) Housing

Posted on March 31, 2013 by David Prutchi Posted in Photomultipliers

diy thermoelectrically cooled PMT housing David Prutchi PhD www.diyPhysics.com

The photomultiplier tubes (PMT) is the workhorse detector in particle physics and many other fields that require detection of light at extremely low levels.  However, the long-wavelength response of PMTs is not only low because of low quantum efficiency, but also because thermionic emission at room temperature causes swamps low-level signals with noise.

Reducing dark counts is especially important in photon-counting applications, especially when attempting to detect photons in the near-infrared. For example, the dark count of many PMTs rated for a wavelength range from 400 to 1200 nm, is in the hundred of thousands of counts when not cooled—making it virtually useless for detecting almost anything but the strongest signal. When cooled to -20 °C, the dark count is reduced to just a few tens counts. As such, in general, the use of PMTs that detect above 600 nm almost mandate a cooled housing.

We constructed a thermoelectrically-cooled housing to experiment with cooling a standard 2” face-on PMT. Although appropriate PMT noise reduction was achieved (one order of magnitude), the thermal efficiency of the do-it-yourself housing design was low, so lessons learned from this build will be used in a second-generation cooled housing.

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diy Scintillation Probe for Ludlum Ratemeters Using Surplus XP3312/SQ PMT

Posted on March 22, 2013 by David Prutchi Posted in CDV700 Pro Geiger-Müller Counter, Chapter 3 - Atoms and Radioactvity, Ionizing Radiation Detection, Photomultipliers, Scintillation Detector

 

Low-Cost Scintillation Probe Based on a Surplus XP3312 PMT for Ludlum Ratemeters www.diyPhysics.com prutchi

Ludlum general-purpose ratemeters are professional-grade instruments that are available on the secondary market at affordable prices.  They are compatible with a wide variety of probes, making them a great choice for educators, surveyors, and advanced amateur users.  However, probes for Ludlum ratemeters are often as expensive as the meter instrument itself, making it worthwhile to build comparable versions from surplus components.

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diy Wu-Shaknov Experiment: Cheapest Demonstration of Quantum Entanglement?

Posted on February 16, 2013 by David Prutchi Posted in Uncategorized

diy Wu-Shaknov experiment by George Musser www.diyphysics.com

George Musser – an editor at Scientific American (and author of “The Complete Idiot’s Guide to String Theory”) – developed a diy version of the Wu-Shaknov Experiment.  If George’s setup truly manages to measure the relative linear polarization of gamma rays from positron-electron annihilation, then he would have accomplished the most inexpensive demonstration of quantum entanglement!

The idea is to measure the relative linear polarization of gamma-ray photons emitted with opposite parity from the annihilation of positrons produced by the decay of Na-22 using Compton polarimetry and coincidence counting.  The predicted results in the number of coincidences are different when assuming quantum entanglement than when basing the calculations on local hidden variables theories.

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80 µCi Americium-241 Sources Inside Old Pyrotronics F3/5A Smoke Detectors

Posted on January 20, 2013 by David Prutchi Posted in Chapter 3 - Atoms and Radioactvity, Radioisotopes

Pyrotronics F3/5A 80uCi Am-241 Source

These are pictures of the Americium-241 sources inside some old Pyrotronics F3/5A smoke detectors that were being decommissioned.  The activity of the Am-241 sources at the time of manufacture (1970s) totaled  80 µCi, so they should still have some ~70 µCi left in them.

80uCi Am-241 Label on Pyrotronics F3/5A smoke detector

The Pyrotronics F3/5A smoke detectors were manufactured in the early 1970s. The radioactive sources consist of americium oxide mixed with gold powder and formed into a small billet. This billet was then placed between a sheet of silver and a sheet of gold and rolled into a foil under high heat and pressure.  Americium-241 decays primarily by alpha particle emission to neptunium-237, along with low energy gamma radiation, with a 59.5 keV gamma emission being most prominent.

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I Really Understand QM…

Posted on January 20, 2013 by David Prutchi Posted in Physics Humor

I really understand Quantum Physics, or may be not...  www.diyPhysics.com  David and Shanni Prutchi

A Low-Cost, Super-Sensitive Paint Can Scintillation Probe for the Prutchi CDV700-Pro

Posted on January 12, 2013 by David Prutchi Posted in CDV700 Pro Geiger-Müller Counter, Chapter 3 - Atoms and Radioactvity, Scintillation Detector

 

Shanni Prutchi Paint Can Scintillator PMT www.diyphysics.com

We just finished constructing a low-cost, yet highly sensitive gamma-ray scintillation probe for our CDV700-Pro counter.  The probe is based on a Philips XP5312/SN photomultiplier tube (that is available from Sphere Research) and a piece of scintillation plastic.  The probe yields a background count of approximately 1,000 counts/minute (cpm) in our lab, and 7,400 cpm from a 137Cs 6.7 µCi exempt source at a distance of 30 cm.  The probe’s sensitivity, portability and rugged construction make it an ideal choice for surveying.

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