4.7 Article

Error Analysis of Nonconstant Admittivity for MR-Based Electric Property Imaging

期刊

IEEE TRANSACTIONS ON MEDICAL IMAGING
卷 31, 期 2, 页码 430-437

出版社

IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
DOI: 10.1109/TMI.2011.2171000

关键词

B1 map; conductivity; magnetic resonance electrical impedance tomography (MREIT); magnetic resonance electrical property tomography (MREPT); permittivity

资金

  1. WCU through MEST/NRF [R31-2008-000-10049-0]
  2. NRF
  3. Korea government (MEST) [20100018275, 2010-0016421]
  4. KOSEF
  5. Ministry of Education, Science & Technology (MoST), Republic of Korea [R31-2008-000-10049-0] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)
  6. National Research Foundation of Korea [2009-0075774, 2010-0018275, 과06A1304] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

向作者/读者索取更多资源

Magnetic resonance electrical property tomography (MREPT) is a new imaging modality to visualize a distribution of admittivity gamma = sigma + i omega epsilon inside the human body where sigma and denote electrical conductivity and permittivity, respectively. Using B1 maps acquired by an magnetic resonance imaging scanner, it produces cross-sectional images of sigma and epsilon at the Larmor frequency. Since current MREPT methods rely on an assumption of a locally homogeneous admittivity, there occurs a reconstruction error where this assumption fails. Rigorously analyzing the reconstruction error in MREPT, we showed that the error is fundamental and may cause technical difficulties in interpreting MREPT images of a general inhomogeneous object. We performed numerical simulations and phantom experiments to quantitatively support the error analysis. We compared the MREPT image reconstruction problem with that of magnetic resonance electrical impedance tomography (MREIT) to highlight distinct features of both methods to probe the same object in terms of its high- and low-frequency conductivity distributions, respectively. MREPT images showed large errors along boundaries where admittivity values changed whereas MREIT images showed no such boundary effects. Noting that MREIT makes use of the term neglected in MREPT, a novel MREPT admittivity image reconstruction method is proposed to deal with the boundary effects, which requires further investigation on the complex directional derivative in the real Euclidian space R-3.

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