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Development of 1.45-mm resolution four-layer DOI-PET detector for simultaneous measurement in 3T MRI.
https://repo.qst.go.jp/records/47069
https://repo.qst.go.jp/records/4706970e26a00-00f1-43e4-a5b2-1e0a7114b662
Item type | 学術雑誌論文 / Journal Article(1) | |||||
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公開日 | 2015-03-25 | |||||
タイトル | ||||||
タイトル | Development of 1.45-mm resolution four-layer DOI-PET detector for simultaneous measurement in 3T MRI. | |||||
言語 | ||||||
言語 | eng | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||
資源タイプ | journal article | |||||
アクセス権 | ||||||
アクセス権 | metadata only access | |||||
アクセス権URI | http://purl.org/coar/access_right/c_14cb | |||||
著者 |
Nishikido, Fumihiko
× Nishikido, Fumihiko× Tachibana, Atsushi× Obata, Takayuki× Inadama, Naoko× Yoshida, Eiji× Suga, Mikio× Murayama, Hideo× Yamaya, Taiga× 錦戸 文彦× 橘 篤志× 小畠 隆行× 稲玉 直子× 吉田 英治× 菅 幹生× 村山 秀雄× 山谷 泰賀 |
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抄録 | ||||||
内容記述タイプ | Abstract | |||||
内容記述 | Recently, various types of PET-MRI systems have been developed by a number of research groups. However, almost all of the PET detectors used in these PET-MRI systems have no depth-of-interaction (DOI) capability. The DOI detector can reduce the parallax error and lead to improvement of the performance. We are developing a new PET-MRI system which consists of four-layer DOI detectors positioned close to the measured object to achieve high spatial resolution and high scanner sensitivity. As a first step, we are investigating influences the PET detector and the MRI system have on each other using a prototype four-layer DOI-PET detector. This prototype detector consists of a lutetium yttrium orthosilicate crystal block and a 4 × 4 multi-pixel photon counter array. The size of each crystal element is 1.45 mm × 1.45 mm × 4.5 mm, and the crystals are arranged in 6 × 6 elements × 4 layers with reflectors. The detector and some electric components are packaged in an aluminum shielding box. Experiments were carried out with 3.0 T MRI (GE, Signa HDx) and a birdcage-type RF coil. We demonstrated that the DOI-PET detector was normally operated in simultaneous measurements with no influence of the MRI measurement. A slight influence of the PET detector on the static magnetic field of the MRI was observed near the PET detector. The signal-to-noise ratio was decreased by presence of the PET detector due to environmental noise entering the MRI room through the cables, even though the PET detector was not powered up. On the other hand, no influence of electric noise from the PET detector in the simultaneous measurement on the MRI images was observed, even though the PET detector was positioned near the RF coil. | |||||
書誌情報 |
Radiological physics and technology 巻 8, 号 1, p. 111-119, 発行日 2015-01 |
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出版者 | ||||||
出版者 | Springer Japan | |||||
ISSN | ||||||
収録物識別子タイプ | ISSN | |||||
収録物識別子 | 1865-0333 | |||||
PubMed番号 | ||||||
識別子タイプ | PMID | |||||
関連識別子 | 25348721 | |||||
DOI | ||||||
識別子タイプ | DOI | |||||
関連識別子 | 10.1007/s12194-014-0298-6 |