Module2 Transcript
Module2 Transcript
Module 2 Transcript
1. ASRT Animation
2. Welcome
Welcome to Essentials of Digital Imaging – Module 2 Processing.
3. License Agreement
4. Objectives
After completing this module, you will be able to:
Describe how photostimulable phosphor image receptors extract data.
Discuss the analysis of image data extracted from image receptors.
Identify and describe the most common exposure indicators for image detectors.
Explain how automatic rescaling affects image quality.
5. Introduction
In digital radiography, a receptor serves the same function as film. It receives the remnant x-ray beam
after the beam passes through the patient. When electronic detector elements in the receptor absorb x-
rays from the remnant beam, an electrical signal is produced. The electrical signal from the detector
elements is an analog signal. The analog signal must be converted into digital data that can be used for
image display, archiving, and transfer.
Following exposure of a PSP plate, the plate must be scanned to extract the image data. These pictures
show both sides of a PSP plate outside the cassette. The technologist doesn’t routinely touch the imaging
PSP plate. The front, or white side shown on the left, contains the photostimulable phosphors and holds
the latent image until processing occurs in the image reader. The back side is black and has two bar-code
stickers. The cassette containing the PSP is read immediately following the exposure.
Scanning the bar code is extremely important to ensure that the image links the patient to the correct
exam. It doesn’t matter when the bar code is scanned with the cassette-based digital imaging system.
The PSP bar code may be scanned before or after an exam is performed. However, be careful when
scanning multiple bar codes before an exam because a processing error occurs when a bar code isn’t
used for the designated scanned exam. For example, if a plate is scanned for a PA chest image but is
used for a lateral chest radiograph, the image won’t display properly because of incorrect processing
codes.
©2016 ASRT. All rights reserved. Essentials of Digital Imaging Module 2 – Processing
department manager makes this decision based on current workflow, space requirements, distance from
the main department and economics. In the picture on this slide, the bar-code scanning hardware and
software, along with the plate reading device, are located near the control panel.
There are varying possibilities in the configuration of a PSP plate reader. In some, one section is the
reading area and another is the plate erasure area and the plate moves through the reader; however, not
all readers transport the plate through the device. In some cassette-based readers, the cassette is
stationary and the equipment moves around the plate as the plate is read.
At this time, a laser light strikes the plate and the F-trap releasing electrons, which in turn produce the
photostimulated luminescence used to create the image. Often electrons are left behind in the F-trap and
this is the reason why plates must be erased after each exposure. Exposing the plate to very bright white
light releases the electrons left in the F-trap back to the valence band so the plate is ready to use again.
The light guide assembly is a single piece of highly engineered acrylic resin approximately 7 mm thick at
its end. The device works much like fiber optic technology to move information from the PSP to the
photomultiplier tube. The light the PSP emits during the image extraction process is not exceptionally
bright. This is the reason most of the photons must be collected and then converted in the photomultiplier
tube. This is also why routinely cleaning the light guide assembly is important to make a PSP plate reader
operate efficiently.
The dual-head flying-spot scanner reads dual-sided PSP plates. This configuration offers the benefit of
reading data from both sides of the plate at the same time. Dual-sided reading increases the detective
quantum efficiency (DQE) of the system and reduces image noise.
©2016 ASRT. All rights reserved. Essentials of Digital Imaging Module 2 – Processing
13. Line Scanner
A cassette-less PSP system is more likely to use a line scanning process. In this system, one of two
things occurs to extract data from the plate. The plate is either pulled underneath the linear scanner or the
plate remains stationary and the laser scanner moves across the plate.
The scanning process and data extraction are the same regardless of whether a system is cassette-
based or cassette-less. The laser beam scans across the plate, which causes the electrons elevated to F-
traps by the x-ray beam to drop back down into their normal orbit. When the electrons return to their
normal orbit, they emit light.
The light guide collects the light and directs it into a device that converts the light photons into an
electrical signal. The device can be a photomultiplier tube, photodiode, or a CCD. The electrical signal is
sent to an ADC where the signal is sampled and assigned a discrete numerical value.
An erasure lamp mechanism’s high intensity light erases the PSP plate. Although it's not a terribly
sophisticated device, when the bulbs are defective or dirty the device can’t completely erase plates and
subsequent images are of poor quality.
Although some equipment is designed to handle a single cassette, other PSP readers allow cassettes to
be stacked so that multiple cassettes can be placed in a reader simultaneously, and the reader processes
the plates in order. This feature is very convenient for a busy department with centrally located PSP
readers.
There are numerous bar code scanning devices and PSP plate reader options from a variety of
manufacturers such as Fuji, Carestream, and Konica. No one configuration is recognized as better than
the other. Each device looks and operates differently on the outside but the devices are very similar when
it comes to internal function. For example, all plate readers require PSP cassettes to be inserted in the
reader in a certain way. The insertion requirement is based on how the reader opens the cassette to pull
out the plate and extract the image.
©2016 ASRT. All rights reserved. Essentials of Digital Imaging Module 2 – Processing
18. PSP Image Extraction Steps
The steps a PSP plate reader takes during image extraction occur regardless of whether the plate is inside
a cassette that a technologist manually loads into a reader or whether the plate is permanently installed
inside a radiographic table.
Once the plate is prepared for image extraction, a laser beam strikes the PSP plate and interacts with the
phosphors located in the plate’s phosphor layer. The energy trapped in the phosphor layer, or the latent
image, is released in the form of light during this interaction. The light guide collects the light photons. The
photons are then sent to a photomultiplier tube, photodiode, or CCD and then to the ADC, where the
photons are converted into a digital signal. Any remaining energy on the plate is removed during the
erasure process when exposing the plate to bright white light removes the remaining electrons.
Flat-panel detectors can be either indirect or direct capture. As you can see from this illustration, the
indirect detector uses a scintillator, usually cesium iodide (CsI) or gadolinium oxysulfide (Gd2O2S). The
scintillator converts the x-rays to light and the amorphous silicon (aSi) photodiode converts the light to
electrons, that are then collected by the thin film transistor. The signal is sent to the ADC. The other
indirect system also uses a scintillator to convert the x-rays to light. The light is directed to a CCD or
CMOS where it is converted into electrons and sent to the ADC.
The direct method of image capture, doesn’t convert the x-rays to light. In this receptor, the x-rays strike
an amorphous selenium (aSe) photoconductor and are directly converted to electrical charges that are
collected by the thin-film transistor and sent to the ADC.
Once the patient and exam are identified in the exam work list, the exposure is made and the image is
extracted in a matter of seconds.
©2016 ASRT. All rights reserved. Essentials of Digital Imaging Module 2 – Processing
21. Thin-film Transistor
The thin-film transistor is an important piece of equipment, regardless of whether it's used in a scintillator
or a nonscintillator detector. Each square in the matrix is known as a detector element, or DEL. Each DEL
is a pixel, or picture element.
An image is created on a flat-panel detector over the thin film transistors. The DEL collects electrons that
are extracted from the detector assembly. The electrons are converted into a digital value by an ADC.
That process creates the image that displays on the monitor. DEL size controls the recorded detail, or
spatial resolution, for the flat-panel device. The technologist can’t change the size of the DEL, which is
fixed for that piece of equipment.
During the exposure, electrons are collected across the area of the image receptor that's exposed to
radiation. Shortly after the exposure, the DELs read out the electrons in a sequential pattern that matches
their location within the detector matrix. As the electrons are removed from the thin-film transistor array,
they’re sent to the ADC, which relays the digital signal to the computer. Once the DELs are read, the flat-
panel detector refreshes and is ready for another exposure.
A CMOS, which is a chip with p-type (positive) and n-type (negative) semiconductor transistors, is another
technology that converts light into electrical charges. Semiconductors are used in many computer
memory systems. The charge in the CMOS is read row by row, and then, as with a CCD, the signal is
sent to the ADC.
The plate reader scans the entire plate, so it scans both the exposed and unexposed areas. If the
computer analysis fails to recognize an exposure field border, or collimation, it can create an image
processing error. In other words, the computer looks at the entire plate, if the data analysis includes all
the information outside the collimation border it can result in poor image quality.
When the exposure field borders, or collimation borders, are recognized everything outside of the black
should be clear. The fingers in these images represent two similarly placed exposure fields. However,
notice how dark the area is where the fingers are located and all the gray area outside of the exposure
field borders. In this instance, the exposure fields weren’t recognized and a rescaling error occurred when
the analysis incorporated the extra exposure outside the collimation field.
©2016 ASRT. All rights reserved. Essentials of Digital Imaging Module 2 – Processing
To extract image data from an analysis of flat-panel receptor DEL values, much like the PSP receptor, the
flat-panel receptor must identify the exposure field. The receptor recognizes the exposure field by the
number of electrons present in the DEL. Unlike the PSP system, however, which looks at the entire plate,
the flat-panel receptor only analyzes the exposed area inside the collimation borders.
The exposure level controls the number of electrons, or electrical charges, that the DEL collects. A
portion of the analysis involves looking for the uniform edge of the exposure field, represented by the
difference between values found in adjacent DELs.
The edge is recognized as a collimation border when the difference between the DELs indicates a well-
defined boundary on the image receptor. When the exposure field is identified, the exposure outside that
border is not included in creating the displayed image.
Histograms graphically represent a collection of exposure values extracted from the receptor. The x axis,
which is the horizontal line, indicates receptor exposure, and the y axis and vertical lines display the
number of pixels for each exposure.
The sampling frequency for PSP plates or the detector elements for flat-panel receptors affects the
number of pixels in the matrix. The small red line, with an assortment of blue bars underneath it,
represents digital values matching points on the line.
Remember, the ADC must quantize, or convert, the continuous stream of electrons into unique digital
values. The histogram provides a tally of the digital signal values extracted from the receptor. The pattern
of values or histogram varies for each anatomical part.
Two formats can extract and analyze the data that create the final digital image viewed on a monitor. The
first format is called “a priori histogram analysis,” and the second is the “neural histogram analysis.”
This ankle is a classic image created using a type 1 histogram. The exposure distributions range from
completely white, representing the maximum attenuation by bone, to the dark areas past the skin line
where unattenuated radiation hit the receptor.
©2016 ASRT. All rights reserved. Essentials of Digital Imaging Module 2 – Processing
The type 2 histogram analysis displays the values of interest from the maximum attenuator up through the
maximum value of the main histogram. But in this case, the skin line doesn’t represent the maximum
value. Type 2 histograms are used for torso, spine, skull, and pelvic examinations.
A type 2 histogram analysis was used to process this image of the abdomen. The maximum attenuator is
the spine and has the brightest displayed intensity; the least attenuating structure appears darker on the
display because it receives the most radiation. In this particular case, a skin line is not important, so the
anchoring point for the maximum intensity is represented by the least attenuating structure.
On the histogram shown here, the far left peak represents the values for barium or metal. To accurately
display the image, we must exclude that area from the values of interest and show the maximum
attenuator as bone and the least-attenuating object as bowel gas, lung tissue, or some other structure.
The least-attenuating structure represents the high end of our values of interest. If the high-attenuation
object, such as barium, is included in the values of interest, it affects image processing.
This image shows barium and air in the stomach. When the image is processed by the computer, the
barium should not be included as a value of interest or the image won’t display properly.
A series of 4 pediatric chest radiographs can result in 4 histograms that are similar in shape but differ
based on the anatomy included in the collimated field. Below each histogram displayed here is the
anatomy included in the collimated field that produced each graph. Notice how the varying pixel values of
the digital images translate into differently shaped neural histograms.
If the captured values don’t match the standardized values, the captured values are rescaled to match the
standardized ones as closely as possible to display an acceptable image. The process of matching the
captured image values to standardized values is called automatic rescaling.
At the bottom of the graph, the white line is a reference histogram for a specific body part when the
correct exposure is delivered to an image receptor. The histogram in black simulates the data collected
when an image receptor is overexposed resulting in higher exposure values.
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39. Automatic Rescaling
Exposure is measured in mR on the graph’s horizontal axis. The vertical axis represents the signal
strength for each exposure level. The oblique line demonstrates the receptor’s response to the specific
units of exposure on the horizontal axis. On the right is a graph that shows the data output presented to a
technologist on a digital display monitor.
Reference lines indicate where the white “proper exposure data” appears in the exposure range. The raw
data value peak on the display monitor is indicated where the white exposure reference line intersects
with the oblique line representing the receptor luminescence levels.
Follow the tracing for the properly exposed histogram to see the tracings for an overexposure. First,
notice that the black line tracing for the overexposure falls within the image receptor’s exposure and
response range. Now there is a data range for the proper exposure and overexposure plotted on the raw
digital output scale of values from 0 to 1,023. The overexposure plot follows the same slope as the proper
exposure plot, but at a higher amplitude, or height. The program automatically rescales the image when it
detects this gap between expected and received amplitude.
An automatic adjustment of the overexposure data plot, which brings the overexposure data and
histogram in line with the proper exposure histogram. The image viewed on the display monitor doesn’t
look overexposed, but in fact, the brightness and gray-scale levels appear as expected.
Rescaling the image pixel values to display properly doesn’t prevent overexposure to the patient. The
technologist has no visual cue that overexposure occurred. With an analog system, a technologist would
have seen the image on the left as it came out of the processor and the excessive density on the image
would be a visual cue to repeat the exam.
The LUT changes the numerical values of the pixels to the contrast levels that are best for each
anatomical part. For example, the matrix of pixel values that would display as low contrast, after the LUT
is applied, change from 40 to 20 and from 60 to 80, resulting in higher contrast than the original.
Automatic rescaling and the LUT work best if the image is acquired with the correct technique factors,
collimation, and source-to-image receptor distance for the anatomical part.
©2016 ASRT. All rights reserved. Essentials of Digital Imaging Module 2 – Processing
A histogram analysis of the distribution of radiation intensities is used to calculate an EI. Remember that
the histogram represents a frequency distribution of discrete values within an image. The EI value is not
absolute; the value represents an approximation of the dose a receptor receives.
The EI is calculated using a mathematical analysis. A mathematical analysis determines the EI based on
the distribution of radiation intensities between those two values. Any changes in the values of bone and
skin line results in a change to the EI. If the histogram is shifted to the right, more exposure was used, so
the EI would reflect a high exposure value.
Here’s an example of the 2 points used to calculate the EI of a type 2 histogram. The type 2 histogram is
useful when a skin line isn’t present in the image field. Notice that point 2 on this histogram is in a
different position than it was on the type 1 analysis. The values of interest for a type 2 histogram analysis
are different than the values of interest for a type 1 histogram analysis. Therefore, when a type 1 image is
processed as a type 2 image, you get an error or the incorrect EI.
This example of a type 3 histogram includes an attenuator which in this case is barium. The attenuator is
represented by the large peak on the left of the histogram. Notice that the number 1 is located to the right
of the attenuating object. If a type 3 histogram analysis wasn’t used, the number 1 would include the low
level exposure in the histogram analysis. This low level of exposure would have indicated to the computer
that the image was underexposed and caused an error in the EI calculation. The inaccurate calculation
also could make the image display incorrectly. The exposure indicator must be calculated over specific
values of interest or it will produce a calculation error.
Fuji and Konica use a sensitivity number to represent the EI which is called an S number. With S-number
EIs, when exposure to the receptor increases, S-number indicator values decrease. Philips uses an
exposure index abbreviated EI that is inversely proportional to exposure. As the exposure to the receptor
increases, the EI value decreases.
Carestream, formerly known as Kodak, uses an exposure indicator known as the exposure index, and
also is abbreviated by the manufacturer as EI. With the exposure indicator, as exposure to the receptor
increases, EI values increase.
Siemens uses a value called the EXI. The EXI value directly relates to the exposure level the receptor
receives. Essentially, increasing the exposure increases the EXI value.
Canon uses a value known as the REX. The REX value also directly relates to the exposure level that the
receptor receives, which means increasing the exposure increases the REX value.
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The DI will indicate whether or not the correct technique was used to acquire the image. A deviation
index, or DI, of 0 is an ideal exposure, but the target range is anywhere between -0.5 to +0.5. A DI of +1.0
to +3.0 indicates overexposure. If the anatomy of interest is too dark, consider repeating the image. Any
DI greater than +3.0 suggests excessive radiation exposure to the patient. Again, a repeat radiograph
should only be performed if the anatomy of interest is too dark. Underexposure is represented by a DI of -
1.0 or less. The radiologist reading the image will determine is a repeat exam is necessary. If the DI falls
below -3.0, a repeat radiograph is required.
For example, the EI could be miscalculated if the collimation margins, or exposure fields, aren’t
recognized. In this case, values outside the collimated borders are included in the distribution used to
create the EI and caused an error in image display.
An unexpected exposure variation recorded on the receptor, that is, an unexpected attenuator, can
change how values are distributed in the histogram. The result can alter the EI and produce a rescaling
error that distorts the displayed appearance of the image.
A prosthetic device can impact the distribution of pixel intensities in a histogram. The area of the
prosthesis in the histogram represents an underexposed area of the image and is included in the
calculation of the EI. The end result is that the EI shows a decrease in receptor exposure when in fact the
image was properly exposed.
The addition of metal into the image data set alters the acquired image histogram compared with the
standard histogram of a knee without a prothesis. Although not shown above, the result is an image that
does not display with correct brightness and contrast and a miscalculation of the EI. The EI indicates the
image was underexposed. In the radiograph shown above, the image brightness and contrast has been
corrected to prevent an additional exam from being performed.
The DAP meter calculates the dose by determining the entrance dose in centigray multiplied by the field
area, or exposure field size, used to create the image. The meter is located in the collimator box and is
commonly used with cassette-less systems. It has a detector interface with the generator.
Because the DAP meter measures the entrance skin exposure delivered to the patient, DAP readouts can
be considered part of a patient's image record.
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52. Flat-panel Detector Dose Area Product
Reducing the exposure field size affects the entrance skin exposure to the patient as measured by a DAP
meter. The problem with the DAP meter is that the readout depends on collimated beam size, which can
vary according to the examination or the facility. Changing the collimated field results in different DAP
readout values. DAP meters require frequent calibration, and defining a proper DAP value also is a
problem. Patient exposure level doesn't equal an appropriate receptor exposure.
53.Exposure Indicator
When technologists view digital images, they can’t rely on the appearance of the image for visual
feedback regarding exposure to the patient. However, given the EI of the digital image receptor,
technologists can determine the accuracy of technical factors used to expose the receptor.
The EI is a way to let the technologist know whether the correct exposure technique was used and,
therefore, is a valuable tool to evaluate radiation protection quality control. If department EIs are
chronically high, it indicates possible overexposure of patients and poor technique selection. Carefully
monitoring EI values helps to ensure that radiation exposure to the patient is as low as reasonably
achievable. But, remember that EIs are not measurements of actual patient dose.
56. Conclusion
This concludes Essentials of Digital Imaging ̶ Module 2 Processing. You should now be able to:
Describe how photostimulable phosphor image receptors extract data.
Discuss the analysis of image data extracted from image receptors.
Identify and describe the most common exposure indicators for image detectors.
Explain how automatic rescaling affects image quality.
57. References
AAPM Report No. 116. An exposure indicator for digital radiography. July 2009. American Association of
Physicists in Medicine website. http://www.aapm.org/pubs/reports/RPT_116.pdf. Accessed February 14,
2013.
Bushong SC. Radiologic Science for Technologists: Physics, Biology, and Protection. 10th ed. St Louis,
MO: Mosby Elsevier; 2012.
Carlton RR, Adler AM. Principles of Radiographic Imaging: An Art and A Science. 5th ed. Clifton Park,
NY: Thomson Delmar Learning; 2012.
Carroll QB. Radiography in the Digital Age: Physics, Exposure, Radiation Biology. Springfield, IL: Charles
C Thomas; 2011.
Carter CE, Vealé BL. Digital Radiography and PACS. St Louis, MO; Mosby Elsevier; 2009.
Practice Standards for Medical Imaging and Radiation Therapy. Radiography practice standards. June
19, 2011. American Society of Radiologic Technologists website. http://www.asrt.org/main/standards-
regulations/practice-standards/practice-standards. Accessed February 14, 2013.
Seeram E. Digital Radiography: An Introduction for Technologists. Clifton Park, NY: Delmar Cengage
Learning; 2011.
Strategic Document. Version 2012-3, April 11, 2012. Digital Imaging and Communications in Medicine
website. http://medical.nema.org/dicom/geninfo/Strategy.pdf. Accessed February 14, 2013.
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