Abstract

Devices aiming at combined Positron Emission Tomography (PET) and Magnetic Resonance Imaging (MRI) to enable simultaneous PET/MR image acquisition have to fulfill demanding requirements to avoid mutual magnetic- as well as electromagnetic-field-related interferences which lead to image quality degradation. Particularly Radio-Frequency (RF)-field-related interferences between PET and MRI may lead to MRI SNR reduction, thereby deteriorating MR image quality. RF shielding of PET electronics is therefore commonly applied to reduce RF emission and lower the potential coupling into MRI RF coil(s). However, shields introduce eddy-current-induced MRI field distortions and should thus be minimized or ideally omitted. Although the MRI noise floor increase caused by a PET system might be acceptable for many MRI applications, some MRI protocols, such as fast or high-resolution MRI scans, typically suffer from low SNR and might need more attention regarding RF silence to preserve the intrinsic MRI SNR. For such cases, we propose RESCUE, an MRI-synchronously-gated PET data acquisition technique: By interrupting the PET acquisition during MR signal receive phases, PET-related RF emission may be minimized, leading to MRI SNR preservation. Our PET insert $Hyperion II^D$ using Philips Digital Photon Counting (DPC) sensors serves as the platform to demonstrate RESCUE. To make the DPC sensor suitable for RESCUE to be applied for many MRI sequences with acquisition time windows in the range of a few milliseconds, we present in this paper a new technique which enables rapid DPC sensor operation interruption by dramatically lowering the overhead time to interrupt and restart the sensor operation. Procedures to enter and leave gated PET data acquisition may imply sensitivity losses which add to the ones occurring during MRI RF acquisition. For the case of our PET insert, the new DPC quick-interruption technique yields a PET sensitivity loss reduction by a factor of 78 when compared to the loss introduced with the standard start/stop procedure. For instance, PET sensitivity losses related to overhead time are 2.9% in addition to the loss related to PET gating being equal to the MRI RF acquisition duty cycle (14.7%) for an exemplary T1-weighted 3D-FFE MRI sequence. MRI SNR measurement results obtained with one $Hyperion II^D$ Singles Detection Module (SDM) using no RF shield demonstrate a noise floor reduction by a factor of 2.1, getting close to the noise floor level of the SNR reference scan (SDM off-powered) when RESCUE was active.

Highlights

  • P OSITRON EMISSION TOMOGRAPHY (PET) is an imaging modality which offers visualization of metabolic processes at molecular level with highest sensitivity and quantification possibilities [1], [2]

  • We presented RESCUE, a PET data acquisition gating technique to be used for simultaneous PET/MR imaging

  • We introduced a new method to quick-stop and -start the Digital Photon Counting (DPC) sensor clocking and performed Magnetic Resonance Imaging (MRI) SNR and noise measurements using a single unshielded Singles Detection Module (SDM)

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Summary

Introduction

P OSITRON EMISSION TOMOGRAPHY (PET) is an imaging modality which offers visualization of metabolic processes at molecular level with highest sensitivity and quantification possibilities [1], [2]. It was successfully combined with Computer Tomography (CT) in the late 1990’s to improve diagnostic accuracy and workflow by co-registering functional PET imaging with anatomical CT images acquired during single scan sessions and reduce the overall scan time by using CT for attenuation and scatter correction instead of PET transmission scans [3], [4]. This promises improved lesion detection using MRI-based motion correction [7], and enables potentially new applications e.g. through the use of simultaneous PET and MR-based spectroscopy [8], [9] or simultaneous PET and functional MRI by temporally correlating their data sets [10]

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