29. Nuclear measurement technique. Flashcards
Nuclear measurement technique. Measuring devices.
Describe the parts of a scintillation counter and their function
Consists of three parts:
- Scintillator: Th activated NaI crystal converts Ekin of charged particles into Eexcitation of the scintillator → fluorescence: photons → ground state
- Photomulitplier tube (PMT): photoelectrode converts light (scintillations) via photoelectric effect to flow of e- multiplied further by secondary e- emission between the dynodes of the PMT → output voltage an be measured
- Electronics: sort amplitudes and eliminate noise caused by electronics, or background interferences (i.e. radioactive stain, cosmic rays, walls, furniture, etc.)
Describe the basic principle of gas-ionization detectors and explain the differences between measuring devices. Refer to the diagram below
Gas-ionization detectors:
- U is connected to 2 electrodes
- radiation entering the chamber ionizes the noble gas molecules
- charges are attracted towards the oppositely charged electrode
- movement of charges → current is measured → change of charge (exposure) is proportional to the dose (can be calculated)
Difference between measuring devices:
U applied to electrodes (none of devices work when too low U is applied → recombination (ion+ + e- → atom)
Explain the function of an ionization chamber
Ionization chamber:
- U high enough → no recombination
- measures amount of U pulses (change of charge) produced by radiation (→ exposure → dose)
Explain the function of a Geiger-Müller (GM) tube
Geiger-Müller (GM) tube:
- high U between the electrodes accelerates charges
- gain E to further ionize → avalanche of charges (primary, secondary, tertiary ion pairs)
- current can be measured → **no. of particles **
**BUT: **relatively insensitive to γ-radiation, but extremely sensitive to α-, β-radiation
Explain the function of a thermoluminescent dosimeter (TLD). Refer to the diagram below
Thermoluminescent dosimeter (TLD):
contain one or more impurities (Mg or Mn) to produce trap states for energetic e-
- radiation → e- in the crystal’s atoms jump to higher E states, where they stay trapped until heated
- heating → e- to drop back to their ground state, releasing a photon of E equal to ∆E between the trap state and the ground state (= luminescence)
Explain the function of a semiconductor detector and the advantages compared to a gas detector
Semiconductor detectors:
- Ionizing radiation → free e- and holes (e- from valence to conduction band, holes in valence band)
- Electric field → e- and holes travel to the electrodes
- Pulse can be measured
- no. of e--hole pairs proportional to J of **incident radiation **
Advantages:
- E required to produce e--hole-pairs very low compared to E required to produce paired ions in gas detectors → variation of the pulse height smaller and E resolution higher
- e- travel fast → very good time resolution