Mark Oehmigen1, Maike E. Lindemann1, Michael Sauer2, Titus Lanz2, and Harald H. Quick1,3
1High Field and Hybrid MR Imaging, University Hospital Essen, Essen, Germany, 2Rapid Biomedical GmbH, Rimpar, Germany, 3Erwin L. Hahn Institute for MR Imaging, University Duisburg-Essen, Essen, Germany
Synopsis
A
dual tuned 13C/1H radiofrequency head coil was evaluated
towards its potential use in integrated PET/MR hybrid imaging. The amount of
PET-signal attenuation due to the head coil was quantified in phantom
experiments. A CT-based 3D template µ-map of the hardware components was
generated and evaluated for attenuation correction (AC). The head coil
homogeneously attenuates the PET signal by 10%. Attenuation correction
homogeneously reduced this attenuation bias to below 1%. These results were
confirmed in PET/MR measurements of six patients. The RF head coil was
successfully integrated into PET/MR hybrid imaging and can now be used for multinucleus
hybrid imaging.Introduction
A dual tuned
13C/
1H radiofrequency
(RF) head coil (Rapid Biomedical GmbH, Rimpar, Germany) is evaluated for its
potential use in PET/MR hybrid imaging. The RF coil features a birdcage design
with 16 rungs that are tuned to the Larmor frequencies of
1H = 123
MHz and
13C = 31 MHz (Fig. 1). When integrated in the setting of
PET/MR hybrid imaging, the RF coil is placed in the field-of-view (FOV) of the
PET-detector during simultaneous PET and MR data acquisition. This causes
attenuation and scattering of the emitted photons and, consequently, leads to
an attenuation bias in PET quantification. The rungs of the birdcage were
extended by 3 cm compared to an MR-only birdcage in order to have the
birdcage rings out of the PET detector ring's area. For attenuation correction
of the remaining rigid and stationary hardware components in the PET-FOV, the
method of a CT-based 3D template µ-map can be applied that corrects for the
quantification bias [1-3]. In this work, the attenuation of a double-tuned RF
head coil was quantified in phantom experiments; a CT-based template µ-map was
generated and applied in AC. The results were then confirmed in PET/MR
measurements of six patients.
Material and Methods
All measurements were performed on an
integrated whole-body PET/MR hybrid system (Biograph mMR, Siemens Healthcare, Erlangen,
Germany). For quantitative PET imaging and evaluation of attenuation a
cylindrical shaped phantom (volume 9.5 l) was used. A phantom holder enabled
the phantom to be positioned a few cm above the patient table with or without
the RF head coil in place (Fig. 2).
Attenuation was determined by difference
measurements. 1) 120 MBq
18F-radiotracer was injected in the water
phantom and the RF coil was placed central in the PET-FOV surrounding the
phantom (Fig. 2A). The PET data were acquired for 30 min in listmode. 2) The RF
coil was removed, and the PET data were decay time corrected (Fig. 2B).
The 3D template AC µ-map of the RF head coil
and of the phantom were acquired using a dual-source CT scanner (SOMATOM
Definition Flash, Siemens Healthcare) with the parameters: tube voltage 140
keV, tube current 400 mA, matrix size of 512 × 512 pixels, voxel size 0.3 × 0.3
× 0.6 mm
3. The CT data attenuation values (140 keV) were adjusted to the PET
energy level of 511 keV, by a bilinear function [2]. All PET data
reconstructions, using the generated AC map of the RF coil and the phantom,
were performed with the reconstruction software (e7 tools, Siemens Molecular
Imaging, Knoxville, USA). The software also provides the hardware AC µ-map of
the PET/MR systems patient table (Fig. 3).
PET/MR hybrid imaging using the
1H
MR-option and
18F-FDG as PET-radiotracer was performed on six
patients (4 male, 2 female; 68 years ± 6 years; 168 cm ± 16 cm; 71 kg ± 11 kg;
285 MBq ± 50 MBq; 3h 16min post injection ± 46min) with the following MR
sequences: Dixon-VIBE for the soft tissue µ-map, T2 TIRM transversal dark fluid
(FLAIR). To measure the attenuation difference in vivo, PET data acquisition on
patients was performed twice: with and without the RF coil in place.
Regions-of-interest were placed in a central slice of the PET images to
determine the tracer activity concentration values (Bq/ml) with and without RF
coil.
Results
In the phantom measurements with and without
the RF head coil in place, an overall global attenuation of true PET events by
8.7% was determined. Attenuation was homogeneously distributed across the
phantom with higher attenuation (up to 25%) along the bottom parts of the coil
(Fig. 4A). Applying the CT-based µ-map of the RF coil successfully reduces the
mean attenuation bias of 10% to below 1% across the phantom volume (Fig.
4B,C). These quantitative results were confirmed in the six patient PET/MR
measurements (Fig. 5). Differences in Bq/ml of 13.5% ± 4.3% were found for
PET images without and with head coil in place. These differences were reduced
to 1.6% ± 1.1% when AC of the coil was applied; indicating accurate
attenuation correction.
Discussion and Conclusion
A dual
tuned
13C/
1H radiofrequency head coil was evaluated
towards its potential use in integrated PET/MR hybrid imaging. Due to its open
and symmetric birdcage design the RF coil attenuates the PET-signal rather
homogeneous. With rigid geometry and a fixed position on the systems patient
table it qualifies for CT-based template AC which was successfully applied. In
conclusion, the RF head coil was successfully integrated into PET/MR hybrid
imaging and can now be used for multinucleus hybrid imaging in further patient
studies.
Acknowledgements
No acknowledgement found.References
[1] Paulus et al. Simultaneous PET/MR imaging:
MR-based attenuation correction of local radiofrequency surface coils. Med
Phys. 2012;39:4306-4315.
[2] Carney et al. Method for transforming CT images for
attenuation correction in PET/CT imaging. Med Phys. 2006;33:976-983.
[3] Paulus et al. Towards improved hardware
component attenuation correction in PET/MR hybrid imaging. Phys Med Biol.
2013;58:8021-8040.