Computed Tomography RAD309 Data Acquisition. Data acquisition represents the first step in process...
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Transcript of Computed Tomography RAD309 Data Acquisition. Data acquisition represents the first step in process...
Data Acquisition
Data acquisition represents the first step in process of image production
X-ray tube & detectors collect information systematically
Collect large number of x ray transmissions around the patient
Data Collection Basics
X-ray source & detector must be in & stay in alignment
Beam moves (scans) around patientmany transmission
measurements taken
Patient
X-Ray beams
Data Collection Basics
Pre-patient beamcollimated to pass only through slice of interestshaped by special filter for uniformity
Data Collection Basics (cont) Beam attenuated by patient Transmitted photons detected by scanner Detected photon intensity converted to
electrical signal (analog) Electrical signal converted to digital value
A to D converter Digital value sent to reconstruction
computer
Each CT Ray
attenuated by patient projected onto one detector
detector produces electrical signalproduces single data sample
DA Geometries
1. Parallel beam, translate rotate motion2. Fan beam, translate rotate motion3. Fan beam, complete rotation tube/detector4. Fan beam, complete rotation of tube around
stationary ring of detectors5. Special: high speed CT, stationary/stationary,
multiple targets tube6. Spiral, rotate/translate 7. Multiple detector rows
Spiral Geometry
X-ray tube rotates continuously around patient
Patient continuously transported through gantry
No physical wiring between gantry & x-ray tube
Requires “Slip Ring” technology
Tube
DetectorSlipRings
InterconnectWiring
X Ray System
Initially used low energy gamma rays Problem: low radiation intensity rate, large
source size, low source strength, high cost
Use of X ray tubes Benefit: high radiation intensity, high
contrast ct scanning Problem: heterogeneous beam , does not
obay Lamber-Beer Exponential Law
Radioactive Source instead of an X-Ray Tube?
High intensity requiredX-ray tubes produce higher intensities than
sources Single energy spectrum desired
Produced by radioactive sourceX-ray tubes produce spectrum of energies
Patient
CT Beam Filtration
Shapes beam to appear monochromatic and satisfy
reconstruction process 1. Hardens beam
Removes greater fraction of low-energy photons than high energy photons
reduces patient exposure
2. Shapes energy distribution to produce uniform intensity & beam cross section
Filter
Patient Protection
Pre-collimatorsbetween tube & patient Tube
Detector
Post-collimators• between patient &
detector
Pre-Collimation
Constrains size of beam Reduces amount of scatter produced Designed to minimize beam divergence Often consists of several stages or sets of
jawsTube
Detector
Pre-collimator
Post-Collimation
Helps define slice (beam) thickness Reduces scatter radiation reaching detector Improves image quality
Tube
Detector
Post-collimator
Detectors
Capture radiation from patient Converts to electrical signal Then they are converted to binary
coded information
Efficiency Componentsa. Capture efficiencya. Capture efficiency
Efficiency of detector to obtain transmitted photons from patient
Size of detector area, distance between 2 detectors
b. Absorption efficiencyb. Absorption efficiencyno. of photons absorbedZ , density, size, thickness of detector
c. Conversion efficiencyc. Conversion efficiencyfraction of absorbed energy which produce signal
2. Response Time
“Speed with which detector can detect an x ray event and recover to detect the next one”
Minimum time after detection of 1st event when detector can detect 2nd event
If time between events shorter than response time, second event may not be detected
Shorter response time better
3. Dynamic Range
Ability to faithfully detect large range of intensities
“Ratio of largest signal to be measured to the precision of the smallest signal to be discriminated”
Typical dynamic range: 1,000,000:1much better than film
4. Stability
“Steadiness” of detector system Consistency of detector signal over
time The less stable, the more frequently
calibration required
Detector Types
2 principles: Convert x-ray into light ---electrical
signal Scintillation detector
Convert x-ray directly into electrical signal
Gas ionization detector
Scintillation Detectors
Crystal couple to photomultiplier tube X ray falls on crystal ---light flashes
(glow) Light directed to PM Light hits Photocathode in PM and
releases electrons
Scintillation
X-ray energy converted to light Light converted to electrical signal
X-Rays
Photomultiplier Tube
Light ElectricalSignal
ScintillationCrystal
Photomultiplier Tubes Light incident on PhotocathodePhotocathode of PM tube Photocathode releases electrons
X-Rays Light
ScintillationCrystal PM
TubePhotocathode
-+
Dynodes
Gas Ionization Detector
Series of individual chambers separated by tungsten plates
X ray falls on each chamber– (+/- ions) + ions move to – plate, - ions to + plate The migration produces electrical signal
Gas Ionization
X-rays converted directly to electrical signal
X-Rays
IonizationChamber
ElectricalSignal
-+
+ -
Filled with Air
CT Ionization Detectors
Many detectors (chambers) used adjacent walls shared between
chambers Techniques to increase efficiency
Increase chamber thickness• x-rays encounter longer path length
Pressurize air (xenon)• more gas molecules encountered per unit
path length
X-Rays thickness
Detector Array
Slice by Slice – one arc of detector array Volume – one arc of detector array,
acquires volume of tissue then separated by computed to slice by slice
DAS
Detector electronics Location: between detector and computer Role of translator
Measure transmitted radiation beamEncodes measurement to binary dataTransmits binary data to computer
Components of DAS
Amplifier Log Amplifier Analog to Digital Converter (digital data) Digital Transmission to computer
Log Amplification
Transmission measurement data must be changed into attenuation and thickness data
Attenuation = log of transmission x thickness
Detector Electronics
Amplifier
Analog to DigitalConverter
Logarithmic Amplifier
FromDetector
ToComputer
Compresses dynamic range;
Converts transmission intensity into
attenuation data
Increases signal strength for
later processing
DA and Sampling
Radiation falling on detector Each samples the beam intensity on it Not enough samples = artifacts
appear To increase number of
measurement/samples available for reconstruction and improve image quality