Imaging technique that uses digital sensors to capture and process radiographic images instead of traditional photographic film
Acceleration to all digital imaging continues because of its undeniable advantages
Several approaches might be used to produce digital radiographs
It is not clear, yet which one is the best one
Digital imaging vocabulary is not yet standard or universally accepted
Use of digital radiography
Helps to eliminate a lot of limitations that were present with screen film technology
Capture element
Where the x-rays are captured
Coupling element
Where the x-ray-generated signal transferred to the collection element
Collection element
Where the x-ray generated signal collected and sent out via electronics for digitalization and processing
Scanned Projection Radiography (SPR)
1. Patient is positioned on CT couch and is driven through the gantry
2. Tube and IR (array) are stationary
3. Result is digital radiograph
Scanned Projection Radiography (SPR)
Collimation to the fan x-ray beam with associated scatter radiation rejection
Improvement of the image contrast
Scanning motion required several seconds, resulting in patient motion blur
At present time, SPR is regaining its importance with some modifications as an adjunct to digital radiographic tomosynthesis (DRT)
The purpose of all forms of tomography is to improve image contrast
Charge-Coupled Device (CCD)
Light-sensing element for most digital cameras
High sensitivity
Wide dynamic range
Small size
CCD
Silicon based semiconductor
Sensitivity is the ability to detect and respond to very low levels of visible light
Size is very small, making it highly adaptable to DR in its various forms
Dynamic range
Ability of the CCD to respond to a wide range of light intensity, from very dim to very bright
CCD has high sensitivity to X-ray exposure and a very wide dynamic range
CCD radiation response is linear
With use of CCD, image contrast is unrelated to image receptor X-ray exposure
CCD system response to very low X-ray exposure, leading to possibility of lowering patient dose
CCD
Photosensitive receptor and electronics embedded in a substrate material in a silicon chip
Incident light from a scintillator strikes the detector, and electron–hole pairs are produced in the silicon
The amount of electron–hole pairs is related to the amount of light absorbed
The electrons are held by electrostatic forces in the array until the charge is read out to form the image
Cesium Iodide/Charge Coupled device
Can be tiled to receive the light from an area x-ray beam as it interacts with scintillation phosphor
Tiled CCD receives light from a scintillator and allows the use of an area x-ray beam, so that exposure time is short
The scintillator light is efficiently transmitted through the fiber-optic bundles to the CCD array
Results in a high x-ray capture efficiency and good spatial resolution (up to 5 lp/mm)
Cesium Iodide/Charge Coupled device
CCD is indirect DR process: 1) x-ray converted to light, 2) light converted into electronic signal
Assembly of multiple CCDs to view the area that x-ray beam presents creates a challenge to provide fidelity image at the edges of each CCD
This challenge is overcome by the interpolation of pixel values at each tile interspace
Scintillator
Determines how many of the incident x-ray photons are absorbed, how much light is produced, and the wavelength or color of the light
Scintillator types
Structured (CsI) - needle-like crystals focus light onto a narrow area, reducing light spread and allowing thicker scintillators
Unstructured (Gd2O2) - powder-like grains produce more light spread, resulting in decreased efficiency of the detector
Quantum efficiency
The number of electrons produced related to the incident light from the scintillator
Detective Quantum Efficiency (DQE)
Ratio of output signal to signal-to-noise ratio, measure of the efficiency and fidelity with which detector can perform its task
DQE for a perfect digital detector is 1 or 100%, but since some amount of noise is always present it's impossible to have 100% DQE
Focus light
Onto a very narrow area
Reducing light spread
Allowing the use of thicker scintillators
Minimizing the loss of spatial resolution
Gd2O2
Considered unstructured because of its powder-like grains
Turbid phosphors
Produce more light spread
Resulting in decreased efficiency of the detector
Quantum efficiency
Represents the absolute efficiency of the light collection and signal created in the chip
Quantum efficiency
Affects detective quantum efficiency (DQE)
DQE
The ratio of output signal to signal-to-noise ratio
DQE
A measure of the efficiency and fidelity with which a detector can perform its task
DQE for a perfect digital detector is 1 or 100%, that would mean that there is no loss of information however, since some amount of noise is always present it's impossible to have 100% DQE
CCD
Built to be as efficient as possible
The polysilicon layer must be transparent enough so that light passes through to the deeper substrate storage area but not so deep that it cannot be captured in the potential well
The spectrum sensitivity must match the spectral output of the phosphor
The less sensitive the CCD to the light spectrum of the scintillator, the less efficient the CCD
TFT flat-panel array
First devices to move beyond the cassette into detectors that would reside in the table or wall stand
These detectors are no longer permanent fixtures and can be used portably as a wireless device