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PET装置用Zr添加GSO:Ce単結晶

PET装置用Zr添加GSO:Ce単結晶

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U.D.C. 616.07:621.397:681.3.02:546.655:548.55:546.831<br />

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Zr doped GSO:Ce Single Crystal for Positron Emission Tomography<br />

Mitsushi Kamada Naoaki Shimura Kazuhiro Yoshida<br />

Nachimuthu Senguttuvan Shigenori Shimizu<br />

PETPositron Emission Tomography<br />

1998<br />

2002CeGd2SiO5<br />

GSO:CePET<br />

PET<br />

<br />

GSO:Ce<br />

GSO:Ce<br />

Ce 4+ <br />

Zr<br />

ZrGSO:Ce<br />

20%Zr<br />

GSO:Ce<br />

The market of positron emission tomography(PET) equipment for medical imaging is<br />

rapidly expanding with the public health insurance coverage of the PET diagnosis in<br />

USA(1998) and Japan(2003). The Cerium-doped Gd2SiO5 (GSO:Ce) single crystal<br />

produced by Hitachi Chemical is used as a scintillator for detecting rays in the PET.<br />

In order to reduce inspection time and improve image quality in PET diagnosis, the<br />

makers of PET equipment are demanding continuous improvement in the scintillation<br />

performance. The GSO:Ce is especially desired to hold its excellent scintillation light<br />

output even when used in longer size required for improving the efficiency of rays<br />

detection. Therefore, we attempted to grow co-doped GSO single crystals with<br />

additional elements and evaluated their scintillation performance. As a result, we found<br />

that Zr doping is effective in preventing the coloration caused by Ce 4+ . By optimizing the<br />

concentration of Zr at 200 ppm, we have developed a new co-doped GSO:Ce single<br />

crystal with about 20% higher light output and better energy resolution than the<br />

conventional GSO:Ce.<br />

<br />

FDG 18 FPET<br />

Positron Emission Tomography1998<br />

PET<br />

2004400<br />

XCT-ray Computed Tomography<br />

CT-PETPET<br />

<br />

2002<br />

200480<br />

PET<br />

PET<br />

<br />

PET2<br />

511 keV<br />

<br />

PET<br />

<br />

PMT<br />

<br />

<br />

<br />

PET<br />

<br />

1 <br />

PhilipsPETAllegroCT-PETGemini<br />

GSO:Ce<br />

<br />

PETEminence-GGSO:Ce<br />

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13


GSO:Ce<br />

<br />

2, 3 GSO:Ce<br />

Ce<br />

<br />

4 <br />

Ce<br />

<br />

GSO:Ce<br />

Zr<br />

<br />

ZrGSO:Ce<br />

<br />

<br />

GSO:Ce<br />

Gd2O3SiO2Ce<br />

CeO2<br />

<br />

100<br />

ppmIr<br />

<br />

1,950<br />

<br />

Ce<br />

Ce 3+ <br />

Ce 4+ <br />

90120 mm12 mm/hr<br />

1030/min<br />

<br />

<br />

GSO:Ce 5 <br />

GSO:CeCe 3+ <br />

GSO:CeCe 3+ <br />

Ce 3+ 5d4fGSO:Ce<br />

Ce<br />

<br />

PETCe<br />

Ce<br />

Ce 4+ <br />

<br />

<br />

GSO:Ce<br />

<br />

<br />

GSO:Ce<br />

Ce 4+ <br />

6 <br />

GSO:Ce<br />

<br />

4620 mm<br />

<br />

3<br />

137 Cs662 keV<br />

46 mmPMT<br />

R71955PTFE<br />

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100 ppm<br />

GSO:CeZrHfGe<br />

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GSO:Ce<br />

Zr<br />

<br />

Zr<br />

<br />

<br />

GSO:Ce<br />

Zr<br />

<br />

Zr<br />

Zr50100200300500<br />

1,000 ppmGSO:Ce<br />

<br />

ZrGSO:Ce<br />

<br />

Zr200<br />

ppmGSO:Ce<br />

GSO:Ce20%<br />

Zr200 ppm<br />

<br />

ZrGSO:Ce<br />

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15


ZrGSO:CeZr<br />

200 ppm<br />

<br />

ZrHfGe<br />

<br />

GSO:Ce4<br />

4<br />

Zr<br />

GSO:Ce<br />

Ce 4+ <br />

Zr 4+ Gd 3+ <br />

Gd 3+ Zr 4+ 1<br />

Ce 4+ <br />

Ce 3+ Ce 4+ <br />

<br />

ZrGSO:Ce<br />

ZrGSO:Ce<br />

GSO:Ce<br />

Ce1.0 mol%2525100 mm<br />

2525 mm2100 mm<br />

Ce<br />

430 nmZr<br />

GSO:Ce 4 <br />

Ce 4+ Zr<br />

<br />

<br />

<br />

GSO:Ce<br />

20%ZrGSO:Ce<br />

ZrGSO:Ce<br />

PET<br />

PET<br />

<br />

<br />

GSO:Ce<br />

Ce 4+ <br />

<br />

GSO:Ce20%<br />

ZrGSO:Ce<br />

PET<br />

<br />

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1 RADIOISOTOPES53, 179 2004<br />

2 K. Takagi and T. FukazawaAppl. Phys. Lett.42, 46 1983<br />

3 40, 252003-1<br />

4 H. Ishibashi et al.IEEE Trans. Nucl. Sci.45 3, 518 1998<br />

5 28, 251997-1<br />

6 S. Shimizu et al.IEEE Trans. Nucl. Sci.50 4, 778 2003<br />

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