MR-compatibility assessment of the first preclinical PET-MRI insert equipped with digital silicon photomultipliers

被引:50
作者
Wehner, J. [1 ]
Weissler, B. [2 ,3 ]
Dueppenbecker, P. M. [1 ,4 ]
Gebhardt, P. [4 ]
Goldschmidt, B. [1 ]
Schug, D. [1 ]
Kiessling, F. [5 ]
Schulz, V. [1 ,2 ]
机构
[1] Rhein Westfal TH Aachen, Dept Phys Mol Imaging Syst, Inst Expt Mol Imaging Syst, D-52074 Aachen, Germany
[2] Philips Res Europe, Aachen, Germany
[3] Rhein Westfal TH Aachen, Inst Hochfrequenztech, D-52062 Aachen, Germany
[4] Kings Coll London, London WC2R 2LS, England
[5] Rhein Westfal TH Aachen, Inst Expt Mol Imaging, D-52062 Aachen, Germany
基金
英国惠康基金;
关键词
PET; MRI; silicon photo multiplier; multimodality imaging; instrumentation; INTERFERENCE; DETECTOR; SCANNER;
D O I
10.1088/0031-9155/60/6/2231
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
PET (positron emission tomography) with its high sensitivity in combination with MRI (magnetic resonance imaging) providing anatomic information with good soft-tissue contrast is considered to be a promising hybrid imaging modality. However, the integration of a PET detector into an MRI system is a challenging task since the MRI system is a sensitive device for external disturbances and provides a harsh environment for electronic devices. Consequently, the PET detector has to be transparent for the MRI system and insensitive to electromagnetic disturbances. Due to the variety of MRI protocols imposing a wide range of requirements regarding the MR-compatibility, an extensive study is mandatory to reliably assess worst-case interference phenomena between the PET detector and the MRI scanner. We have built the first preclinical PET insert, designed for a clinical 3 T MRI, using digital silicon photomultipliers (digital SiPM, type DPC 3200-22, Philips Digital Photon Counting). Since no thorough interference investigation with this new digital sensor has been reported so far, we present in this work such a comprehensive MR-compatibility study. Acceptable distortion of the B-0 field homogeneity (volume RMS = 0.08 ppm, peak-to-peak value = 0.71 ppm) has been found for the PET detector installed. The signal-to-noise ratio degradation stays between 2-15% for activities up to 21 MBq. Ghosting artifacts were only found for demanding EPI (echo planar imaging) sequences with read-out gradients in Z direction caused by additional eddy currents originated from the PET detector. On the PET side, interference mainly between the gradient system and the PET detector occurred: extreme gradient tests were executed using synthetic sequences with triangular pulse shape and maximum slew rate. Under this condition, a relative degradation of the energy (<= 10%) and timing (<= 15%) resolution was noticed. However, barely measurable performance deterioration occurred when morphological MRI protocols are conducted certifying that the overall PET performance parameters remain unharmed.
引用
收藏
页码:2231 / 2255
页数:25
相关论文
共 42 条
  • [1] Association NEM, 2008, NEMA Standards Publication, NU4-2008, P123
  • [2] Beyer T, 2000, J NUCL MED, V41, P1369
  • [3] CHEMICAL-SHIFT IMAGING - A REVIEW
    BRATEMAN, L
    [J]. AMERICAN JOURNAL OF ROENTGENOLOGY, 1986, 146 (05) : 971 - 980
  • [4] Chen NK, 1999, MAGNET RESON MED, V41, P1206, DOI 10.1002/(SICI)1522-2594(199906)41:6<1206::AID-MRM17>3.0.CO
  • [5] 2-L
  • [6] The Digital Silicon Photomultiplier - A Novel Sensor for the Detection of Scintillation Light
    Degenhardt, Carsten
    Prescher, Gordian
    Frach, Thomas
    Thon, Andreas
    de Gruyter, Rik
    Schmitz, Anja
    Ballizany, Rob
    [J]. 2009 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-5, 2009, : 2383 - 2386
  • [7] Delso G, 2011, J NUCL MED, V52, P1914, DOI 10.2967/jnumed.111.092726
  • [8] Principles of PET/MR Imaging
    Disselhorst, Jonathan A.
    Bezrukov, Ilja
    Kolb, Armin
    Parl, Christoph
    Pichler, Bernd J.
    [J]. JOURNAL OF NUCLEAR MEDICINE, 2014, 55 : 2S - 10S
  • [9] Düppenbecker PM, 2012, IEEE NUCL SCI CONF R, P3478
  • [10] Düppenbecker PM, 2012, IEEE NUCL SCI CONF R, P3481