Synopsis
The aim of this presentation is to
introduce the participant into Time-of-Flight (ToF) Positron Emission
Tomography. General concepts of ToF-PET, fundamental limits and most important
characteristics of the key components scintillator and photo detector will be
discussed. The correlation between timing resolution and image SNR, which is
the main benefit of the timing measurement, will be introduced by means of
examples from real patient examinations and simulations. Special emphasis will
be put on completely new imaging application enabled by ToF-PET and on the
potential of ToF-PET for simultaneous MR/PET imaging.Introduction
The aim of this presentation is to
introduce the participant into Time-of-Flight (ToF) Positron Emission
Tomography and to give an overview on fundamental principles, state of the
technology, fundamental limits, benefits and new approaches enabled by ToF-PET.
Special emphasis will be put on the potential of ToF-PET for simultaneous
MR/PET imaging. The course “Time-of-Flight: Do We Need It in PET/MRI?” will
comprise 4 parts:
Principles and technology of ToF-PET,
General Benefits of ToF-PET, New Approaches
Enabled by Time-of-Flight detection, and
Future Technology Development and Fundamental Limits.
Principles and technology
of ToF-PET
Time-of-Flight PET was first studied
and implemented in the early 1980s. However, these systems were experimental
and were limited by scintillators, photo detectors and electronic components
available at this time. After important technological progress was achieved on
these key components, ToF-PET was readdressed in the 21st century
and found its way into commercial products in 2006. It has become now stat-of-the
art in nuclear imaging. Newly released commercial, clinical PET scanners have
timing resolutions of about 400 picoseconds, which is rather close to the
timing resolutions of 450 to 750 picoseconds achieved with the first
experimental systems based on CsF and BaF2 scintillators. Compared
with other scintillators, CsF and BaF2 have a poor intrinsic gamma
ray detection efficiency (also called stopping power) and low scintillation
light yield, leading to low spatial resolution of the PET systems and also low
system sensitivity. Only the development of new, bright, fast scintillation
crystals with high stopping power made ToF-PET feasible in clinical systems.
With the starting interest in simultaneous MR/PET imaging, the photo multiplier
tube had to be replaced by photo detectors that where insensitive to the strong
electromagnetic fields of MR scanners. This propelled the development of silicon-based
photodetectors and made Silicon Photomultiplier (SiPM) widely available. Apart
from their compactness and MR compatibility, they also have excellent intrinsic
timing resolution, which makes them a promising photodetector for ToF PET
systems. In this part of the presentation, general concepts of ToF-PET and most
important characteristics of the key components scintillator and photo detector
will be discussed.
General Benefits of ToF-PET
ToF-PET
is mainly characterized by an improved trade-off between image contrast and
image noise. But it has also been demonstrated to enable faster convergence of
iterative image reconstruction algorithms, to lead to better lesion detectability,
better image homogeneity and making iterative reconstruction more robust in the
presence of inconsistent data. As a consequence, ToF- PET allows for more
challenging applications, e.g imaging with shorter examination and/or frame times,
imaging with lower counts caused by low uptake, low injected dose or non-standard
radioisotopes and imaging of larger patients. The underlying property that is
responsible for the mentioned advantages is the effect that improving ToF
resolution in PET scanner increases their effective sensitivity. This
correlation between timing resolution and image SNR is often referred to as
Time-of-Flight sensitivity gain will be introduced by means of examples from
real patient examinations and simulations as shown in figure 1.
New Approaches Enabled by
Time-of-Flight detection
Apart from the sensitivity gain achieved
at constant acquired counts, Time-of-Flight measurements provide every detected
temporal coincident event with an additional scalar value that gives the arrival
time difference the both detected gamma photons. This additional parameter
allows for new imaging application as simultaneous acquisition of events
emitted by the object or emitted from a supplementary transmission source for
PET attenuation correction, which is of special interest for highly precise
simultaneous MR/PET imaging. Also it was shown, that bare emission data with
timing information allow joint estimation of activity and attenuation images up
to a global scale factor, that attenuation artefacts due to motion or MR image
segmentation are reduced by ToF reconstruction and that Time-of-Flight also
enables limited angle Positron Emission Tomography.
Future Technology
Development and Fundamental Limits
During the last decade, huge progress
was made in the development of PET detector technology, especially of
silicon-based photodetectors. At the end of the course, a short outlook on expected
future developments and also fundamental limits is given.
Acknowledgements
No acknowledgement found.References
[1] Thoen, et al. "Influence of detector pixel
size, TOF resolution and DOI on image quality in MR-compatible whole-body
PET." PMB 58.18 (2013), 6459