TY - JOUR
T1 - Monitoring of positron using high-energy gamma camera for proton therapy
AU - Yamamoto, Seiichi
AU - Toshito, Toshiyuki
AU - Komori, Masataka
AU - Morishita, Yuki
AU - Okumura, Satoshi
AU - Yamaguchi, Mitsutaka
AU - Saito, Yuichi
AU - Kawachi, Naoki
AU - Fujimaki, Shu
N1 - Publisher Copyright:
© 2014, The Japanese Society of Nuclear Medicine.
PY - 2015/4/1
Y1 - 2015/4/1
N2 - Purpose: In proton therapy, imaging of proton-induced positrons is a useful method to monitor the proton beam distribution after therapy. Usually, a positron emission tomography (PET) system installed in or near the proton beam treatment room is used for this purpose. However, a PET system is sometimes too large and expensive for this purpose. We developed a small field-of-view (FOV) gamma camera for high-energy gamma photons and used it for monitoring the proton-induced positron distribution. Methods: The gamma camera used 0.85 mm × 0.85 mm × 10 mm Ce:Gd3Al2Ga3O12 (GAGG) pixels arranged in 20 × 20 matrix to form a scintillator block, which was optically coupled to a 1-inch-square position-sensitive photomultiplier tube (PSPMT). The GAGG detector was encased in a 20-mm thick container and a pinhole collimator was mounted on its front. The gamma camera was set 1.2 m from the 35 cm × 35 cm × 5 cm plastic phantom in the proton therapy treatment room, and proton beams were irradiated to the phantom with two proton energies. Results: The gamma camera had spatial resolution of ~6.7 cm and sensitivity of 3.2 × 10−7 at 1 m from the collimator surface. For both proton energies, positron distribution in the phantom could be imaged by the gamma camera with 10-min acquisition. The lengths of the range of protons measured from the images were almost identical to the simulation results. Conclusions: These results indicate that the developed high-energy gamma camera is useful for imaging positron distributions in proton therapy.
AB - Purpose: In proton therapy, imaging of proton-induced positrons is a useful method to monitor the proton beam distribution after therapy. Usually, a positron emission tomography (PET) system installed in or near the proton beam treatment room is used for this purpose. However, a PET system is sometimes too large and expensive for this purpose. We developed a small field-of-view (FOV) gamma camera for high-energy gamma photons and used it for monitoring the proton-induced positron distribution. Methods: The gamma camera used 0.85 mm × 0.85 mm × 10 mm Ce:Gd3Al2Ga3O12 (GAGG) pixels arranged in 20 × 20 matrix to form a scintillator block, which was optically coupled to a 1-inch-square position-sensitive photomultiplier tube (PSPMT). The GAGG detector was encased in a 20-mm thick container and a pinhole collimator was mounted on its front. The gamma camera was set 1.2 m from the 35 cm × 35 cm × 5 cm plastic phantom in the proton therapy treatment room, and proton beams were irradiated to the phantom with two proton energies. Results: The gamma camera had spatial resolution of ~6.7 cm and sensitivity of 3.2 × 10−7 at 1 m from the collimator surface. For both proton energies, positron distribution in the phantom could be imaged by the gamma camera with 10-min acquisition. The lengths of the range of protons measured from the images were almost identical to the simulation results. Conclusions: These results indicate that the developed high-energy gamma camera is useful for imaging positron distributions in proton therapy.
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U2 - 10.1007/s12149-014-0936-4
DO - 10.1007/s12149-014-0936-4
M3 - Article
C2 - 25476773
AN - SCOPUS:84939948947
SN - 0914-7187
VL - 29
SP - 268
EP - 275
JO - Annals of Nuclear Medicine
JF - Annals of Nuclear Medicine
IS - 3
ER -