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charge-coupled devices (CCD)
the oldest indirect conversion digital radiography system used to acquire a digital image
x-ray photons interact with a scintillation material, and the signal is transmitted by lenses or fiberoptics to the CCD
during the transmission process, the lenses reduce the size of the projected visible light image and transfer the image to one or more small capacitors that convert the light into an electrical charge
this charge is stored in a sequential pattern and released line by line and sent to an ADC
structure and function of CCD
made of a photosensitive receptor and electronics embedded in a substrate material in a silicon chip
x-rays strike on scintillator, converted into light
light strike on the chip, converted into electrical signals
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
the detector element (del) contains three electrodes that hold the electrons in an electrical potential well
bucket brigade scheme
when the readout row is reached, data is sent sequentially to the sense amplifier and digitalized
the readout process requires that the movement of electrons is timed
multiple voltage change occur very quickly
overfill of the dels will cause a blooming effect
bucket brigade scheme
the dels are formed by voltage gates that, at readout, are opened and closed like gates to allow flow of electrons
to collect the charge on the silicon chips, the voltage sign is changed on the electrodes with each del, moving the electrons by rows down the columns until the readout row is reached
blooming effect
excess electrons spill out of the del into an adjacent del
overflow drains are built into the array to reduce or prevent this effect
silicon chip
this chip is made up of a polysilicon layer, a silicon dioxide layer, and a silicon substrate
the polysilicon layer is coated with a photosensitive material and contains the electron gates
the silicon dioxide layer is an insulator
the silicon substrate contains the charge storage area
image-related characteristics
size:
it is not practical to manufacture a CCD chip larger than 5 × 5 cm — cost is high
most range from 2 to 4 cm
the image must be matched to the size of the CCD
CCD technology uses lenses or fiberoptics so that the image matches the receptor size
reducing the image size involves several components that contribute to the quality of the image
the scintillator, light collection component, noise
the scintillator and the way it is contructed will determine
how many of the incident x-ray photons are abosrbed
how much light is produced
the wavelength or color of the light
CCD optics are critical contributors to digital image quality
lenses or fiberoptics focus light onto the CCD chip
the efficiency of the transportation of light to the chip is important because of the noise created
the more light that is sent to the chip without creation of noise, the more efficient the system is
the design of optics is also crucial in imaging performance
issues arise with geometric distortion such as light scattering or lens or optic flaws
the amount of electrons produced relative to the incident light from the scintillator is the quantum efficiency of the CCD
scintillator
phosphors are structured or unstructured (turbid)
structured scintillator
CsI — due to its needle-like crystals
CsI needles focus light onto a very narrow area, reducing light spread and allowing the use of thicker scintillators minimizing the loss of spatial resolution
unstructured scintillator
Gd2O2 — due to its powder-like grains
turbid phosphors produce more light spread, resulting in decreased efficiency of the detector
quantum efficiency
represents the absolute efficient of the light collection and signal created in the chip
affects detective quantum efficiency
noises associated with CCD technology
quantum noise (statistical noise)
“dark” or current noise
amplification noise
noise
the random variation of brightness or color information in digital images that creates a grainy, speckled, or mottled texture interference
signal
in medical and digital imaging, refers to the amount of useful, informative data captured by the imaging system
quantum noise
statistical noise
is created by lack of light photons from the scintillator; this is known as quantum mottle
is caused if there is not enough x-ray photons striking the scintillator
if too few light photons are produced by the scintillator, then too few electrons will be generated, and the output signal will be noisy
dark noise
occurs when the CCD chip operates without radiation stimulation
when temperature rises electrons are moving into some areas
at readout, unnecessary information is added to the image
some manufacturers add thermoelectric cooling devices that drop the temperature as much as 40 degrees F, lower than room temperature
can be as much as 10,000 electrons/pixel per second
A 40 degree F drop can reduce by a factor of 100
amplification noise
most commonly referred to as readout noise or read noise
represents the electronic noise generated during the physical process of converting a pixel’s stored electrical charge into a readable analog voltage signal
is common to digital systems, and there are no CCDs without it
the response of each CCD chip will vary across the array
some pixels may not work at all; or work differently
software is used to correct the statistical variation caused by inoperable pixels
the more bad-pixel, the worse the detector efficiency
the cheaper the CCD, the more defects
CCD applications
used in several applications in radiology:
digital fluoroscopy, stereotactic breast biopsy, digital mammography, general radiography, dental, others
advantages/disadvantages of CCD
CCDs are simple and modular
easy to repair, replace, and upgrade
CCDs are relatively cheaper than TFT- based flat-panel systems
demagnification issues reduce DQE
decreases image quality
CMOS
complementary metal oxide semiconductor
systems were developed by NASA
uses a scintillator that converts x-rays into light photons and stores them into capacitors
each pixel has its own amplifier, which is switched on and off by circuitry within the pixel, converting the light photons into electrical charges
voltage from the amplifier is converted by an ADC also located within the pixel
this system is highly efficient and takes up less fill space than CCDs
a semiconductor
when doped, the semiconductor becomes a fill-scale
transistors use little to no power when not needed
image sensors convert light to electrons that are stored in capacitors located within the pixel
during readout, the charge is sent across the chip and read at one corner of the array
at each pixel, several transistors amplify the charge and send it through wires to the array corner
an ADC turns each pixel’s value into a digital value
semiconductors
a solid, chemical element or compound that conducts electricity under some conditions but not others
a good medium for control of electrical current
conduction ability varies according to the amount of current or voltage it receives or on the x-ray intensity
do not conduct electricity well on their own
impurities, or dopants, added to increase conductivity
common dopants added to silicon are:
gallium arsenide, indium antimonide, and oxides of most metals
materials: antimony, arsenic, boron, carbon, germanium, selenium, silicon, sulfur, and tellurium
silicon is the most popular and is the base material of most integrated circuits
comparison of CCD and CMOS technology
CCD sensors are more susceptible to noise
light sensitivity of a CMOS chip is lower than CCD
in a CMOS, the pixel is surrounded with transistors, and many of the light photons hit these rather than the photodiode
CMOS uses very little power
CCDs may use as much as 110x more power
CMOS is very inexpensive to manufacture
CMOS ships tend to have lower quality, lower resolution, and lower sensitivity, but the technology is improving
pixel fill factor is greater with CCDs than CMOS
in digital fluoroscopy
with II:
video system: mirror directing light; video/camera system for delivering image or recording
CCD photodetector is attached to output screen and converts exit light photons into electrical signal and send them to the monitor
without II:
TFT-flat panel uses:
under mag mode, no patient dose increasing
indirect (CsI) is more common — at low mA, better signal
CMOS flat panel detector is catching up (image quality is getting better)