Detectors Flashcards
Gas filled detectors include these 3 types
ionization chamber
proportional counter
geiger müller
In detectors, recombination occurs when __________ voltages are use
low
Ionization chambers operate in the __________ region
saturation
When the voltage becomes sufficient to cause complete collection of all of the charges produced, the curve enters a plateau called the
saturation region
The saturation region voltage ranges from
~ 50 - 300 V
The amount of energy to produce an ionization in air is
34 eV
Ionization chambers generally contain a cap which can be removed in order to
measure non-penetrating radiation such as beta particles, low energy photons (<10 keV) and alpha particles
A typical survey meter can measure exposure rates down to approximately
1 mR/hr
Unlike other types of ionization chambers dose calibrators employ sealed and pressurized chambers filled with ______.
argon gas
A device that records total charge collected over time is a
pocket dosimeter
Percentage of photons actually interacting in an ionization chamber
<1%
Unsealed ioniation chambers must be corrected for the effects of
temperature and pressure
In an unsealed ionization chamber pressure and density are
proportional
In an unsealed ionization chamber, density and temperature are
inversely related
The pressure and temperature correction factor for an ionization chamber
(Pref x T) / (P x Tref)
T is in Kelvin (273 + °C)
In the proportional region, gas amplification can be as high as
106
In a GM counter, the center wire has this voltage sign
+
(anode)
Gas amplification occurs in the GM counter as in a proportional counter. In addition to ionizing gas molecules, the accelerating electrons also can cause excitation of gas molecules through collisions. These excited gas molecules quickly (~10−9 sec) return to the ground state through the emission of photons at
visible or ultraviolet wavelengths
The role of quenching gas in an ionization chamber
Neutralize positive ions by donating electrons
Absorb UV radiation from the positive ions to prevent a second avalanche
In a GM system, gas amplification can be as high as
1010
The curve for three main regions of ionization chambers as a function of voltage
Occurs with voltages above the GM range
spontaneous discharge
The wire screen on the detector is meant to
protect the fragile layer of mica (0.01-mm thick) that is sufficiently thin to permit passage of particles and low-energy photons into the counter
GM meters are about _________ times more sensitive than ionization chamber survey meters
10
The removeable cover on GM meter is meant to
help distinguish between penetrating and non-penetrating radiations
GM counters designed for counting only relatively penetrating radiations, such as γ rays and high-energy βparticles, have thicker, sturdier windows made of
0.1-mm-thick aluminum or stainless steel
Because the solid detector materials used in semiconductor detectors are ___________ more dense than gases
2000 to 5000
The most commonly used semiconductor detector materials are
silicon (Si) and germanium (Ge)
Newer semicondutor detecting materials include
cadmium telluride (CdTe) or cadmium zinc telluride (CZT)
In semiconductor detectors, the amount of energy to produce an ionization is
3 to 4 eV
(roughly 1/10 of an ionization chamber)
For the same absorbed energy, a semiconductor detector can produce a signal ______ times large than an ionization chamber
10
One problem with Si and Ge (especially Ge) detectors is
production of thermal noise
Impurities in Si and Ge detectors can
create electron traps, absorbing electrons from ionization events
The thickness of Si Ge detectors is limited by
impurities which create electron traps and greatly reduce the signal
Deliberately doping or introducing Li impurities into Si or Ge detectors can compensate for electron traps by
donating electrons
Because Li ions tend to “condense” at room temperatue Si(Li) and Ge(Li) detectors must be
super-cooled with liquid nitrogen
CdTe and CZT (which has properties very similar to CdTe) are more recently developed semiconductor materials that overcome two of the major disadvantages of Si and Ge:
(1) they can be operated at room temperature without excessive electronic noise, and (2) their high atomic number means that even relatively thin detectors can have good stopping efficiency for detecting γ rays.
CdTe or CZT detection elements are usually small because of
difficulty and expense of growing large pieces with the required purity
The scintillator materials used for detectors in nuclear medicine are of two general types: inorganic substances in the form of solid crystals and organic substances dissolved in liquid solution.
inorganic substances in the form of solid crystals and organic substances dissolved in liquid solution
A characteristic common to all scintillators is that the amount of light produced following the interaction of a single γ ray, β particle, or other ionizing radiation, is
proportional to the energy deposited by the incident radiation in the scintillator
For a single scintillator γ-ray interaction within the energy range of interest for nuclear medicine imaging, the number of photons produced is
few hundred to a few thousand