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Scintillator

physical science Maturity 11-13 Next article →

A scintillator is a specialized material that exhibits scintillation, also known as radioluminescence. This process occurs when the material is excited by ionizing radiation. When an incoming particle strikes the scintillator, the material absorbs the particle's energy. It then re-emits that absorbed energy in the form of light.

FZU scintillators 1
FZU scintillators 1

In some materials, the excited state is metastable. This means the relaxation back to lower energy states is delayed. This delay can last from a few nanoseconds to several hours. Depending on the type of transition and the wavelength of the emitted photon, this phenomenon is classified as either delayed fluorescence or phosphorescence.

To turn these flashes of light into data, scientists use a scintillation detector. This device couples the scintillator to an electronic light sensor. A common sensor is the photomultiplier tube, or PMT. The PMT absorbs the light from the scintillator and re-emits it as electrons via the photoelectric effect. These photo-electrons undergo multiplication to create an electrical pulse. This pulse can be analyzed to reveal information about the original particle.

Other sensors include vacuum photodiodes, which do not amplify the signal, or silicon photodiodes. Silicon photomultipliers use an array of reverse-biased photodiodes operating in avalanche mode. This allows each pixel to be sensitive to even a single photon.

Scintillators are categorized by their chemical makeup. Organic scintillators are aromatic hydrocarbon compounds containing benzene ring structures. Common examples include anthracene, stilbene, and naphthalene. Anthracene is often used as a reference because it has the highest light output of all organic scintillators. These organic crystals are durable, but they are difficult to machine or grow in large sizes. Another type is organic liquids. These consist of organic scintillators, called solutes, dissolved in an organic solvent. Solutes like p-terphenyl or PPO are mixed with solvents like toluene or benzene to create these liquid solutions.

Plastic scintillator
Plastic scintillator

The history of this technology began in 1903. Sir William Crookes built the first device using a ZnS screen. He called this instrument a spinthariscope. To use it, a person had to view the scintillations through a microscope in a darkened room. This method was very tedious for researchers. The field changed significantly in 1944. Researchers Curran and Baker replaced the human eye with the newly developed PMT. This transition from visual observation to electronic measurement marked the birth of the modern scintillation detector.

When selecting a material, scientists must balance many different properties. High density is a major requirement. High density reduces the size of particle showers and decreases the range of Compton scattered photons. This leads to better spatial resolution. Materials with heavy ions, like lead or cadmium, increase the photoelectric effect. High stopping power is also necessary for compact detectors. Scientists also look for fast operation speeds. Precision in timing is proportional to the inverse of the decay time. Short decay times are essential for fast coincidence circuits and high event rates.

US Navy 070208-N-9132D-002 Electronics Technician 2nd Class Shea Thompson tests an Alpha Particle Dection Probe
US Navy 070208-N-9132D-002 Electronics Technician 2nd Class Shea Thompson tests an Alpha Particle Dection Probe

Scintillators have a wide range of practical applications. In medicine, they are used in CT scanners and gamma cameras for diagnostics. The American government utilizes them for Homeland Security radiation detectors. They are also used in the petroleum industry for Gamma Ray logs during oil exploration. In particle physics, they help detect rare events. Even everyday technology uses them, such as in older CRT computer monitors and television sets. Some researchers even propose using them in nuclear batteries to harness gamma-ray energy.

Efficiency and light output are critical for a detector's performance. Light output is often measured as the number of photons produced per keV of deposited energy. For example, plastic scintillators produce about 10 photons/keV. Bismuth germanate produces about 8 photons/keV. Anthracene produces approximately 40 photons/keV. However, quenching can reduce this efficiency. Quenching occurs when radiationless deexcitation processes turn the excitation into heat instead of light. Additionally, the overall signal depends on the quantum efficiency of the PMT, which is typically around 30% at its peak. Scientists must also consider how temperature affects the material, especially in high-temperature environments like oil drilling.

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🖼️ Images & Media (4)
File:SGCat24454-scint-gris.noirEtBlanc.jpg
SGCat24454-scint-gris.noirEtBlanc.jpg
File:Plastic scintillator.jpg
Plastic scintillator.jpg
File:FZU_scintillators_1.jpg
FZU_scintillators_1.jpg
File:US Navy 070208-N-9132D-002 Electronics Technician 2nd Class Shea Thompson tests an Alpha Particle Dection Probe.jpg
US Navy 070208-N-9132D-002 Electronics...
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