Detectors Flashcards

1
Q

Gas filled detectors include these 3 types

A

ionization chamber

proportional counter

geiger müller

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2
Q

In detectors, recombination occurs when __________ voltages are use

A

low

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3
Q

Ionization chambers operate in the __________ region

A

saturation

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4
Q

When the voltage becomes sufficient to cause complete collection of all of the charges produced, the curve enters a plateau called the

A

saturation region

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5
Q

The saturation region voltage ranges from

A

~ 50 - 300 V

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6
Q

The amount of energy to produce an ionization in air is

A

34 eV

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7
Q

Ionization chambers generally contain a cap which can be removed in order to

A

measure non-penetrating radiation such as beta particles, low energy photons (<10 keV) and alpha particles

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8
Q

A typical survey meter can measure exposure rates down to approximately

A

1 mR/hr

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9
Q

Unlike other types of ionization chambers dose calibrators employ sealed and pressurized chambers filled with ______.

A

argon gas

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10
Q

A device that records total charge collected over time is a

A

pocket dosimeter

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11
Q

Percentage of photons actually interacting in an ionization chamber

A

<1%

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12
Q

Unsealed ioniation chambers must be corrected for the effects of

A

temperature and pressure

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13
Q

In an unsealed ionization chamber pressure and density are

A

proportional

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14
Q

In an unsealed ionization chamber, density and temperature are

A

inversely related

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15
Q

The pressure and temperature correction factor for an ionization chamber

A

(Pref x T) / (P x Tref)

T is in Kelvin (273 + °C)

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16
Q

In the proportional region, gas amplification can be as high as

A

106

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17
Q

In a GM counter, the center wire has this voltage sign

A

+

(anode)

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18
Q

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

A

visible or ultraviolet wavelengths

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19
Q

The role of quenching gas in an ionization chamber

A

Neutralize positive ions by donating electrons

Absorb UV radiation from the positive ions to prevent a second avalanche

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20
Q

In a GM system, gas amplification can be as high as

A

1010

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21
Q

The curve for three main regions of ionization chambers as a function of voltage

A
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22
Q

Occurs with voltages above the GM range

A

spontaneous discharge

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23
Q

The wire screen on the detector is meant to

A

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

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24
Q

GM meters are about _________ times more sensitive than ionization chamber survey meters

A

10

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25
Q

The removeable cover on GM meter is meant to

A

help distinguish between penetrating and non-penetrating radiations

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26
Q

GM counters designed for counting only relatively penetrating radiations, such as γ rays and high-energy βparticles, have thicker, sturdier windows made of

A

0.1-mm-thick aluminum or stainless steel

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27
Q

Because the solid detector materials used in semiconductor detectors are ___________ more dense than gases

A

2000 to 5000

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28
Q

The most commonly used semiconductor detector materials are

A

silicon (Si) and germanium (Ge)

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29
Q

Newer semicondutor detecting materials include

A

cadmium telluride (CdTe) or cadmium zinc telluride (CZT)

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30
Q

In semiconductor detectors, the amount of energy to produce an ionization is

A

3 to 4 eV

(roughly 1/10 of an ionization chamber)

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31
Q

For the same absorbed energy, a semiconductor detector can produce a signal ______ times large than an ionization chamber

A

10

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32
Q

One problem with Si and Ge (especially Ge) detectors is

A

production of thermal noise

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33
Q

Impurities in Si and Ge detectors can

A

create electron traps, absorbing electrons from ionization events

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34
Q

The thickness of Si Ge detectors is limited by

A

impurities which create electron traps and greatly reduce the signal

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35
Q

Deliberately doping or introducing Li impurities into Si or Ge detectors can compensate for electron traps by

A

donating electrons

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36
Q

Because Li ions tend to “condense” at room temperatue Si(Li) and Ge(Li) detectors must be

A

super-cooled with liquid nitrogen

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37
Q

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:

A

(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.

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38
Q

CdTe or CZT detection elements are usually small because of

A

difficulty and expense of growing large pieces with the required purity

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39
Q

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.

A

inorganic substances in the form of solid crystals and organic substances dissolved in liquid solution

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40
Q

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

A

proportional to the energy deposited by the incident radiation in the scintillator

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41
Q

For a single scintillator γ-ray interaction within the energy range of interest for nuclear medicine imaging, the number of photons produced is

A

few hundred to a few thousand

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42
Q

electronic tubes that produce a pulse of electrical current when stimulated by very weak light signals

A

photo multiplier tubes (PMTs)

43
Q

This is an illustration of

A

Photo-multiplier Tube (PMT)

44
Q

In photocathodes, the conversion efficiency for visible light to electrons, also known as the quantum efficiency, is typically

A

1 to 3 photoelectrons per 10 visible light photons striking the photocathode

45
Q

A common photo emissive substance coating the photomultiplier tube

A

Cesium antimony (CsSb)

46
Q

The dynode is maintained at a positive voltage, typically __________ relative to the photocathode

A

200-400 V

47
Q

Successive dynodes are maintained at voltages _________ higher than the previous dynode

A

50-150 V

48
Q

PM tubes often are wrapped in metal foil for magnetic shielding, called ________ an alloy composed of iron, nickel, and small amounts of copper and chromium

A

Mu-metal

49
Q

PMTs used in nuclear medicine may range in size from

A

1 to 7.5 cm in diameter

50
Q

An alternative to a PMT is

A

light-sensitive semiconductor detector, such as a Si photodiode

51
Q

While Si photodiodes have high quantum detection efficiency (60-80%) they have _________ gain

A

unity

requiring very low-noise electronics for readout

52
Q

Si avalanche photodiode (APD) uses a very high internal electric field which enables it to

A

amplify the signal

53
Q

Si avalanche photodiode (APD) detectors can reach gains of ____________but still require low-noise electronics for successful operation

A

102 to 103

54
Q

APDs also can be operated at higher bias voltages in

A

geiger mode

55
Q

APDs are often found in these systems

A

small animal scanners

56
Q

Inorganic scintillators are crystalline solids that scintillate because of characteristics of their

A

crystal structure

57
Q

Order from lowest to highest density for LSO, BGO, NaI

A

NaI

BGO

LSO

58
Q

Peak emission wavelength of NaI scintillator

A

415 nm

59
Q

The most commonly used scintillator for detectors in nuclear medicine

A

NaI(Tl)

60
Q

Dimensions of crystals for gamma cameras that use NaI(Tl) crystals that are typically

A

30-50 cm in diameter by 1-cm thick

61
Q

With efficient optical coupling, good reflective surfaces, and a crystal free of cracks or other opacifying defects, approximately ___________ of the light emitted by the NaI(Tl) crystal actually reaches the cathode of the PM tube

A

30%

62
Q

Single crystals of NaI(Tl) for radiation detectors are “grown” from molten sodium iodide to which a small amount of thallium (__________ mole percent) has been added

A

0.1 - 0.4

63
Q

5 reasons to use NaI(Tl) scintillators in NM

A
  1. It is relatively dense (Δ = 3.67 g/cm3) and contains an element of relatively high atomic number (iodine, Z = 53). Therefore it is a good absorber and a very efficient detector of penetrating radiations, such as x rays and γ rays in the 50- to 250-keV energy range. The predominant mode of interaction in this energy range is by photoelectric absorption.
  2. It is a relatively efficient scintillator, yielding one visible light photon per approximately 30 eV of radiation energy absorbed.
  3. It is transparent to its own scintillation emissions. Therefore there is little loss of scintillation light caused by self-absorption, even in NaI(Tl) crystals of relatively large size.
  4. It can be grown relatively inexpensively in large plates, which is advantageous for imaging detectors.
  5. The scintillation light is well-matched in wavelength to the peak response of the PM tube photocathode

7.

64
Q

Important inorganic scintillator characteristics

A

efficiency

index of refraction

emission spectrum

65
Q

Maximum event rate of a scintillator to prevent event “pileup”

A

1 / 2τ where τ is the decay time for the scintillator

66
Q

Liquid scintillation solutions consist of

A

Organ solvent

primary solute (or primary fluor)

sceondary solute or waveshifter

additives to improve performance

67
Q

All liquid scintillation counters suffer from

A

quenching - any mechanism that reduces the amount of light output from the sample

68
Q

Three types of quenching in liquid scintillation systems

A

chemical (compete with primary fluor for energy absorption)

color (substances absorb the primary emissions, e.g., blood)

dilution (large volume of sample added decreasing output efficiency)

69
Q

The iodine escape peak appears at

A

30 keV below the photopeak

70
Q

Photopeak

A

peak in spectra for energy of the emission

71
Q

Can be set to allow only certain photon energy levels to be counted, decreasing Compton scatter and pulse pile-up in the image

A

Pulse Height Analyzer (PHA)

72
Q

As count rate increases in NM spectroscopy

A

dead time losses increase

general broadening of the photopeak due to pile-up

shift of the photopeak toward lower energyies beasue of baseline shift in the amplifier

73
Q

As x-ray energy increases it becomes __________ to separate the photopeak from the scatter

A

easier

(less contribution from lower energies in the photopeak)

74
Q

Refers to the proportionality between output pulse amplitude and energy absorbed in the detector

A

Energy linearity

Most NaI(Tl) systems are quite linear for energies between .2 and 2 MeV

75
Q

Energy resolution in NM spectroscopy is decreased due to

A

random statistical variations:

  1. number of scintillation light photons per keV
  2. number of photoelectrons released from photocathode
  3. variation in electron multiplication factors from dynodes
  4. nonuniform sensitivity across scintillator from PMTs
  5. nonuniform light collection efficiency
  6. nonlinear response of scintillator
  7. electronic noise
76
Q

FWHM(%) is

A

(ΔE at FWHM / Eγ) * 100%

77
Q

A reasonable energy resolution in NM gamma cameras with Tc-99m and Cs-137 is

A

10% for Tc-99m at 140 keV

6% for Cs-137 at 662 keV

78
Q

For a gaussian shaped curve, the FWHM is approximately

A

2.35 x standard deviation

79
Q

typical integration time for a NM camera

A

approximately 1 usec

80
Q

The best energy resolution is obtained with

A

semiconductor detectors

due to approximately 1 charge per 3 eV of radiation vs. 10 photoelectrons per keV for NaI

81
Q

Number of photoelectrons for keV in NaI(Tl) PMT system

A

10 per keV

82
Q

The larger number of charges generated in a semiconductor detector decreases

A

statistical variation and increases energy resolution

83
Q

A Ge(Li) detector resolution at 140 keV for Tc-99m

A

.42% versus 10 %

84
Q

For a CZT detector spectrum of Tc-99m, what is the bump at around 20 keV?

A

K x-rays of Tc-99m emitted after internal conversion

85
Q

Liquid scintillators provide __________ energy resolution relative to NaI(Tl)

A

poor

86
Q

geometric efficiency

A

efficiency with which the detector intercepts radiation emitted from the source. This is determined mostly by detector size and the distance from the source to the detector

87
Q

intrinsic efficiency

A

amount absorbed / amount striking detector

Refers to the efficiency with which the detector absorbs incident radiation events and converts them into potentially usable detector output signals. This is primarily a function of detector thickness and composition and of the type and energy of the radiation to be detected.

88
Q

To combine efficiencies you

A

multiply them

geometric * intrinsic * …

89
Q

Surface area of sphere

A

4πr2

90
Q

Volume of sphere

A

4/3 π r3

91
Q

geometric efficiency is approximately

A

.5 (1-cosθ)

92
Q

Dead time losses occur due to

A

overlapped pulses falling outside the selected analyzer window

93
Q

typical dead times for

GM tube

NaI(Tl ) and semiconductors

liquid scintillation and gas proportional counters

A

50-200 usec

.5 - 5 usec

.1 - 1 usec

94
Q

non paralyzeable system

A

if an event occurs within the dead time, τ, of a preceding event, it is not counted

95
Q

paralyzable system

A

if an event occurs within the dead time, τ, of a preceding event, it is not counted AND it introduces a dead time τ.

Essentially an “extendable” dead time is created

96
Q

Most radiation detectors are

paralyzable or nonparalyzable?

A

paralyzable

97
Q

For a nonparalyzable system the observed counting rate, Ro, is

A
98
Q

For a paralyzable system the observed count rate is

A
99
Q

Another word for the “resolving time”

A

dead time

100
Q

In a paralyzable system, at very high true counting rates the observed counting rate

A

approaches zero

101
Q

For a paralyzable system, the observed counting rate rises to a maximum value given by

A

e = 2.718… the base of natural logarithms

102
Q

For small values of true count rate as dead time (<.1) the percentage loss is approximately

A

True count rate * dead time * 100%

103
Q

When measuring dead time with a system that has a pulse height analyzer, you must account for the

A

window fraction

the relationship between the true dead time and apparent dead time is

τa = τ / wf

(does not apply when doing 2 source method)