X-ray Detection & Aspects of Image Formation Flashcards
Creating a Digital Image
We have seen that when we expose a patient to a uniform beam of X-ray photons, the photons are selectively attenuated depending on the anatomy of a patient.
This creates a beam whose intensity varies as a function of spatial location
We refer to this as the latent image
Latent - (of a quality or state) existing but not yet developed or manifest; hidden or concealed.
What is a digital X-ray image receptor ?
A digital X-ray image receptor (or detector) is responsible for detecting the X-ray photons incident upon it and forming a digital image from the latent image
The image is divided into pixels, and each pixel has a value proportional to the X-ray dose incident upon it
A Simple Image Receptor
Energy from X-ray photons incident on a pixel are converted to electrical charge in the pixel electronics
A number of intermediate stages may be involved
This charge is passed via an amplifier into an analogue-to-digital convertor
Entrance Surface Dose Incident on Detector Pixel Element and Digital Value relationship
Pixel response to dose is usually linear, but can have a logarithmic relationship in some cases.
The gain of the amplifier defines the sensitivity of the imaging system
A Simple Image Receptor: The digital (number) value
The digital (number) value produced is proportional to the energy absorbed by the pixel
In practice a square matrix of pixel detector elements is used to produce digital values that are stored in a computer
Typical detector pixel dimensions are 0.1 – 0.2 mm square
Creating a Digital Image: pixels
These stored values can be displayed on a monitor
Each pixel element of the image has an associated X and Y position in a matrix
The value of each pixel (i.e. the digital number) defines the shade of grey which is displayed
Creating a Digital Image: the size of the displayed image
Note that the size of the displayed image is not generally the same as the size of the detected image
once stored in a computer the image is merely recorded as numbers in a matrix (sometimes called an array)
these numbers can be represented in many different ways before displaying the final image (magnified/reduced)
Creating a Digital Image: grey level values
Note that the grey level values (displayed pixel values) of the displayed image are not generally the same as the pixel values initially recorded for the detected image
once stored in a computer the image is merely recorded as numbers in a matrix (sometimes called an array)
these numbers can be manipulated in many different ways before displaying them – for example by adding or subtracting a number to all the values to make the image brighter or darker
Energy band concepts of conductors
Looking at electrons right at the outer shell of the atoms of the material.
The valence band- electrons still bound to the atoms.
Have this energy band where electrons can occupy it if they have sufficient energy of the material allowed it.
conduction band- where electrons are still in the material but they’re not bound to the individual atoms, they’re free to move around.
They are then free to conduct the flow of charge is what electrical current is all about.
There’s no gap between the valence band and the conduction band.
Some valence electrons can jump up into the conduction band, but be immediately filled with free electrons from the conduction band.
Grey Level Range (Pixel Depth)
The range of values an image pixel can have is quantized and finite
Generally there will be 2N levels possible, where N is the number of binary bits used to store the value in the computer
Typical values of N being 12 or 14
The range will go from 0 to (2N-1)
Energy band concepts of insulators
Insulators are different in that their valence band was full, there was no gaps and the conduction band was empty.
There was an energy zone whereby electrons just couldn’t occupy you would need to put in lots of energy into this material before you could get electrons to jump up into this conduction band..
Energy band concepts of Luminescence
If electrons drop from there conduction band into the valence band and recombined with a hole, you ocould get light given off depending on what the energy gap was and that’s how light emitting diodes work and that is called luminescence.
Energy band concepts of
semiconductors
The in between material is the semiconductor material so it can conduct under certain circumstances.
We do have some electrons in the conduction band.
We can increase the electrons in the conduction band by pumping little bits of energy into the system. And the electrons jump into that conduction band even at room temperature.
A few vacancies (gaps) in the valence band. We call that a semi conductor.
If we apply negative potential here on the left and positive on the right the electrons going to move in the right direction.
Energy band concepts of Photostimulated luminescence
Photo stimulated luminescence is what we us in CR image plate readers, the modified material by using small amounts of impurities in the material to create these little charge traps which are between the valence band and the conduction band. In terms of their energy .
Electrons can be stimulated by absorbing x-ray photons into the conduction band.
But when they want to try and drop down back to the valence band we can trap them in the charge traps.
That charge can hold the charge for hours.
Those trap charges correspond to where we absorbed a lot of x-rays.
We want to read where the charge was and we can do that by using some light of a particular wavelength to give that charge a nudge out of that trap, encourage it to recombine into the valence band.
It produces some more lights, but a different colour, a different coloured light for the light which is stimulated
We use a lasor light to get those charges to drop down into the valence band and release some light of a different colour.
2 different types of light: the stimulating lasor light to get this charge to jump out of the trap,
And the stimulated the light that we stimulated are emitted and that is slightly different colour.
We can collect that light at a particular point on a CR plate
CR Principles
Uses an imaging plate to store a latent X-ray image
The imaging plate is later scanned by a laser beam which causes the latent image to be released as light
This light is detected and converted to electrical charge using a photomultiplier tube
The charge is readout, amplified and converted to a digital image using an analogue-to-digital (ADC) convertor
CR Image Acquisition
Image plate, expose it in this case a neon lasor of a particular wavelength and we scan our lasor across our plate as we are scanning across our plate, we are also moving the plate through the reader as well.
As that’s happening were collecting the stimulated light where the lasor beam actually was at any particular time.
You’ll be stimulating light out of the CR plate and then will use a light guide to guide those stimulated light photons into this this photomultiplier tube which converts the light into charge.
We can then convert that into a digital number by amplifying it and using an analogue to digital converter.
And we got our final image at the end which we cn display on a monitor.
Indirect Detectors
Indirect
x-rays
CsI scintillator – converts X-ray photons to light
Light photons converted to electrical charge
charge- Readout electronics
2 types of detector was the direct detector which is a photoconductor (can absorb photons).
We can collect that charge and once we got charge we can convert it to a digital number.
Indirect- we us a a scintillate material which we talk about luminescence. Then we absorb an x-ray, we get light photons. We can convert that light using a photo diode that will produce charge from our light.
Direct detectors
Direct
x-rays
a-Se photoconductor converts X-ray photons to electron-hole pairs
charge- Readout electronics
They have conversion layer which is a scintillator. A phosphor converts the x-ray photons to light when you’ve got something like cesium iodide is with a material called palium.
The material has grown as a layer like a crystal.
These columns channel the light down from where the initial x-ray photon was absorbed.
Scintillator
The CsI scintillator used on indirect detectors is often around 500 µm thick.
This gives an absorption of the incoming X-ray beam of about 80%.
Each absorbed X-ray photon in the scintillator causes ~3000 light photons to be emitted
Thicker CsI would increase efficiency, thinner CsI would increase resolution.
A 500 mm CsI layer is well matched to a read out matrix with a pixel pitch of around 200 mm.
Readout
In turn this causes release of charge carriers in the photodiode (~1500 charge carriers/X-ray photon) which are stored locally on a capacitor
TFT switches control the timing of readout, allowing the charge to be sent to a charge sensitive amplifier
The signal is then digitised by an ADC and readout to the computer for storage and display