Digital Radiography System Explained (step-by-step) - YouTube

Channel: Clover Learning

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In this video, we'll be covering cassette-less digital
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radiography systems.
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Cassette-less digital radiography
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is different from CR radiography in that there is no cassette
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or imaging plate reader.
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Cassette-less digital radiography
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can be broken down into either direct or indirect systems.
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Indirect radiography can be further broken down
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into either thin flat-panel transistors called
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TFTs or charged-coupled device systems called CCDs.
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Indirect TFT systems are composed of three main layers--
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the top scintillation layer, a middle photodiode layer,
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and the bottom TFT array.
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The top scintillation layer or light layer
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is where the incoming incident X-ray photons are
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converted into light photons.
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A scintillation is nothing more than a burst
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of light, which is why this layer is
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called the scintillation layer.
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Each photon that strikes the scintillation layer
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creates a small burst of light energy.
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Unfortunately, one downfall of using a scintillation layer
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is that it produces light isotropically or in all
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directions.
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The isotropic nature of this layer
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thus acts to decrease spatial resolution,
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since the converted light photons
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are of a greater size than the incoming incident X-ray
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photons.
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Basically, the scintillation layer
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create a small amount of blur on each image.
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The scintillation layer is comprised
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of either the ionic compound cesium
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iodide or the chemical element gadolinium.
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Cesium iodide is preferred over gadolinium,
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since it can be formed into very small rods.
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These small cesium iodide rods are
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able to produce a smaller, more focused light
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beam, which in turn serves to increase spatial resolution.
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After the scintillation layer comes the photodiode layer.
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The photodiode layer is comprised
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of a semiconducting material known as amorphous silicon.
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The photodiode layer works by converting the incoming light
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photons from the scintillation into electric charge.
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The electric signal or electrons produced
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by the photodiode layer are then transferred
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to the thin-film transistor or TFT layer.
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The TFT layer is comprised of an array or matrix
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of very small detector elements, or DELs for short.
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Each DEL is comprised of a capture element or pixel
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detector, which is the active element within each DEL,
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a storage capacitor, which stores
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the electric charge produced by the capture element,
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and a thin-film transistor or switch that
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acts to open and close the release of electric charge
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leaving each DEL, thus producing the digital image.
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The ability of each DEL to produce
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a high spatial resolution radiograph
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is designated by the percentage of the active pixel area
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within each DEL.
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The percentage of DEL to active pixel
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is known as the fill factor.
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There is a direct relationship between fill factor
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and spatial resolution in that as the active area increases--
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that is, takes up a greater percentage
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of space within the DEL--
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spatial resolution increases.
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The charged-coupled device, or CCD system,
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is the other form of cassette-less digital
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radiography.
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CCD systems differ from the TFT systems
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in that, with the CCD system, there is no photocathode or TFT
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layer.
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The scintillation layer within CCD systems
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are optically coupled to each CCD sensor
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chip by either lenses or fiber optics.
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The CCDs are able to both convert light photons
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into electrical signals as well as send the electrical signals
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to the computer for processing.
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The final cassette-less digital radiography system
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is the direct conversion radiography system
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or non-scintillation system.
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This system is comprised of an amorphous selenium-based
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semiconductor and a TFT.
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This system works by applying a high-voltage charge
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to the top surface nanoseconds before the extra exposure is
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made.
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The interaction between the incident X-ray photons
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and the high-voltage charge causes the selenium atoms
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to release their electrons, which
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are then able to be collected and processed by the TFT layer.
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This final image gives a visual illustration
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of each type of cassette-less digital radiography system.
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