J. Franke, U. Heinen, L. Matthies, V. Niemann, F. Jaspard, M. Heidenreich, T. Buzug
{"title":"首个用于小鼠和大鼠的MPI-MRI混合成像系统集成设计:仪器设置描述","authors":"J. Franke, U. Heinen, L. Matthies, V. Niemann, F. Jaspard, M. Heidenreich, T. Buzug","doi":"10.1109/IWMPI.2013.6528363","DOIUrl":null,"url":null,"abstract":"This hybrid MPI-MRI imaging system (see Fig. 1 RIGHT) is currently under assembly at the research labs of Bruker BioSpin MRI GmbH, whereas single components were already tested. The magnetic field strength and the magnetic field gradient were measured to be up to <sub>Bz</sub>=0.495 T and up to G<sub>z</sub>=2.2 T/m for the PF and the SF, respectively (see Fig. 1 LEFT). The MRI gradient strengths were determined to be G<sub>x</sub>=0.84 mT/A/m, G<sub>y</sub>=0.9 mT/A/m, G<sub>z</sub>=0.87 mT/A/m (I<sub>max</sub>=300 A) and the MRI RF coil was tuned to the Larmor frequency of protons at 0.495 T. The DF resonant circuits were tuned to excitation frequencies of around 25 kHz. With expected maximal DF amplitude of 20 mT and the strongest SF gradient strength a field of view of 18×36×36 mm<sup>3</sup> could be reached.","PeriodicalId":267566,"journal":{"name":"2013 International Workshop on Magnetic Particle Imaging (IWMPI)","volume":"14 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2013-03-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"11","resultStr":"{\"title\":\"First hybrid MPI-MRI imaging system as integrated design for mice and rats: Description of the instrumentation setup\",\"authors\":\"J. Franke, U. Heinen, L. Matthies, V. Niemann, F. Jaspard, M. Heidenreich, T. Buzug\",\"doi\":\"10.1109/IWMPI.2013.6528363\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This hybrid MPI-MRI imaging system (see Fig. 1 RIGHT) is currently under assembly at the research labs of Bruker BioSpin MRI GmbH, whereas single components were already tested. The magnetic field strength and the magnetic field gradient were measured to be up to <sub>Bz</sub>=0.495 T and up to G<sub>z</sub>=2.2 T/m for the PF and the SF, respectively (see Fig. 1 LEFT). The MRI gradient strengths were determined to be G<sub>x</sub>=0.84 mT/A/m, G<sub>y</sub>=0.9 mT/A/m, G<sub>z</sub>=0.87 mT/A/m (I<sub>max</sub>=300 A) and the MRI RF coil was tuned to the Larmor frequency of protons at 0.495 T. The DF resonant circuits were tuned to excitation frequencies of around 25 kHz. With expected maximal DF amplitude of 20 mT and the strongest SF gradient strength a field of view of 18×36×36 mm<sup>3</sup> could be reached.\",\"PeriodicalId\":267566,\"journal\":{\"name\":\"2013 International Workshop on Magnetic Particle Imaging (IWMPI)\",\"volume\":\"14 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2013-03-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"11\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2013 International Workshop on Magnetic Particle Imaging (IWMPI)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/IWMPI.2013.6528363\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2013 International Workshop on Magnetic Particle Imaging (IWMPI)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IWMPI.2013.6528363","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
First hybrid MPI-MRI imaging system as integrated design for mice and rats: Description of the instrumentation setup
This hybrid MPI-MRI imaging system (see Fig. 1 RIGHT) is currently under assembly at the research labs of Bruker BioSpin MRI GmbH, whereas single components were already tested. The magnetic field strength and the magnetic field gradient were measured to be up to Bz=0.495 T and up to Gz=2.2 T/m for the PF and the SF, respectively (see Fig. 1 LEFT). The MRI gradient strengths were determined to be Gx=0.84 mT/A/m, Gy=0.9 mT/A/m, Gz=0.87 mT/A/m (Imax=300 A) and the MRI RF coil was tuned to the Larmor frequency of protons at 0.495 T. The DF resonant circuits were tuned to excitation frequencies of around 25 kHz. With expected maximal DF amplitude of 20 mT and the strongest SF gradient strength a field of view of 18×36×36 mm3 could be reached.