Continuous Phoswich Scintillators
and Detectors
RMD's Imaging
Technology Group has developed a unique, first-of-its-kind,
advanced family of phoswich scintillators and related
detector technology, capable of providing continuous
depth-of-interaction (DOI) information in a monolithic
scintillator for gamma interactions in PET, SPECT
and other gamma-sensing systems used in medical imaging,
security and other applications.
Termed
Continuous Phoswich scintillators (CPS)
and detectors (CPD), this breakthrough
development in radiation detection, measurement and
imaging is applicable in clinical medical imaging,
pre-clinical small animal imaging, security applications
such as baggage and cargo scanning, and industrial
imaging. RMD's CPS material, in addition to its Continuous
Phoswich capability, has been designed and shown to
provide high light output, high speed, excellent energy
resolution, insignificant afterglow and no hysteresis.
Continuous
Phoswich detection adds a third dimension to the localization
of a scintillation event within a scintillator, thereby
enabling the more accurate localization of the origin
of the positron annihilation or gamma emission within
the patient, small animal or other scan subject, in
order to produce images with higher spatial and contrast
resolution, free of radial elongation and parallax
effects that result in degraded image quality, constrain
system design or require greater system complexity
in an effort to reduce these effects.
With its
inherent DOI determination capability, our Continuous
Phoswich scintillator may be made thicker than a conventional
scintillator, in order to increase sensitivity without
compromising spatial resolution. With DOI determination,
the traditional and often difficult imaging tradeoff
between spatial resolution (favoring a thin sensor)
and detection efficiency (favoring a thick sensor)
no longer applies, since DOI determination decouples
the previously fundamental relationship between these
two important considerations. Increased sensitivity
leads to faster imaging (e.g., for improved gated
cardiac imaging or reduced scan time), reduced patient
or subject dose (through greater collection efficiency),
greater collection efficiency for short-lived isotopes,
and/or improved imaging of brief phenomena (e.g.,
bolus passage, tracer washout or tracer decay).
With
CPS and CPD technology, utilizing conventional photodetectors
and straightforward modifications to conventional
front-end electronics, the position of event occurrence
along a selected axis in the Continuous Phoswich scintillator
is determined. This DOI information is then used in
electronics and/or software to adjust X-Y position
information in SPECT and gamma camera imaging and,
in the case of PET, line-of-response (LOR) location
and time-of-flight (TOF) information.
In
PET*, RMD's CPS and CPD technology
eliminates or renders inconsequential the radial elongation
effect of so-called "off-axis" events (that is, event
coincidence detected by scintillators that do not
share a common long axis), improves the timing resolution
for "on-axis" events, and can even yield better off-axis
than on-axis spatial resolution.
(*
Positron Emission Tomography.)
As
seen in an accompanying figure, PET spatial resolution
for on-axis events is determined by scintillator crystal
cross-sectional area and achievable event timing (TOF)
resolution, with both conventional scintillators and
CPS/CPD technology. However, for off-axis events with
conventional scintillators, the radial elongation
effect degrades spatial resolution increasingly with
increasing distance between the event LOR and the
central scan axis (since PET scintillator length is
greater than its width), while event timing resolution
actually improves somewhat with this increased distance.
CPS/CPD
technology determines the DOI of an event in a scintillator,
and allows the straightforward determination, in front-end
detector electronics and/or software, of the event
LOR. As a result, the radial elongation error for
off-axis events is comparable to or even less than
that for on-axis events. CPS/CPD technology also allows
radially longer PET scintillators (with single photodetectors)
for increased overall sensitivity, and allows lines
of response (LORs) that are farther from the central
scan axis for improved utilization of the PET scanner
bore and smaller minimum angles between pairs of coincidence
detectors.
Historically,
most previous attempts to develop useful phoswich
detection technology have been aimed at PET, where
limited improvement over non-DOI coincidence sensing
has been offered by often cumbersome and expensive
solutions, that at best still supply only 1 or 2 bits
of event depth information. Such phoswich detectors
have utilized a variety of designs, including (typically)
discrete combinations of multiple materials, sometimes
double the number of photodetectors otherwise required,
sometimes wavelength-shifting materials, and often
significantly more complex electronics than otherwise
required, to provide only 1 or 2 bits of DOI information.
This often comes at the expense of light loss and
reduced energy resolution, and at considerably greater
system complexity and expense than standard non-phoswich
scintillators and detectors.
In
SPECT* and other pinhole and related gamma imaging,
CPS and CPD technology eliminates or renders inconsequential
the parallax effects encountered in single-photon
imaging with a gamma camera with pinhole, multi-pinhole
or other focused collimation, including many forms
of SPECT and gamma camera imaging.
(*
Single-Photon Emission Computed Tomography.)
As seen
in an accompanying figure, for pinhole, multi-pinhole
and related collimators used in SPECT, and for some
limited-angle tomography and planar imaging, the parallax
effect causes degradation of resolution that increases
radially from the point on the scintillator closest
to the focal point of the radiation source (no parallax),
to the edge of the scintillator (greatest parallax
error).
CPS/CPD
technology allows the straightforward correction,
in front-end detector electronics and/or software,
of interaction event position in the Continuous Phoswich
scintillator to a virtual thin plane, regardless of
the actual scintillator thickness.
RMD's
CPS and CPD materials and devices are undergoing active
test and evaluation, on an ongoing
basis, at RMD and at the Center for Gamma Ray Imaging
(CGRI) at the University of Arizona (Tucson, AZ),
for use in PET, SPECT and other gamma imaging devices
and systems.
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