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A single‐scan T mapping method based on two gradient‐echo images with compensation for macroscopic field inhomogeneity
Authors:Yuguang Meng  Hao Lei
Institution:1. State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan 430071, China;2. Graduate School, Chinese Academy of Sciences, Beijing 100049, China
Abstract:Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-3‐weighted imaging (Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-4WI) and quantitative Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-5 mapping with conventional gradient‐echo acquisition are often hindered by severe signal loss induced by macroscopic field inhomogeneity. Various z‐shimming approaches have been developed for Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-6WI/Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-7 mapping in which the effects of macroscopic field inhomogeneity are suppressed while the sensitivity of Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-8‐related signal intensity to alterations in the microscopic susceptibility is maintained. However, this is often done at the cost of significantly increased imaging time. In this work, a fast Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-9 mapping method with compensation for macroscopic field inhomogeneity was developed. A proton density‐weighted image and a composite Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-10‐weighted image, both of which were essentially free from macroscopic field inhomogeneity‐induced signal loss, were used for the Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-11 calculation. The composite Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-12‐weighted image was reconstructed from a number of gradient‐echo images acquired with successively incremented z‐shimming compensation. Because acquisition of the two images and z‐shimming compensation were realized in a single scan, the total acquisition time for obtaining a Turn:x-wiley:07403194:media:MRM21731:tex2gif-stack-13 map with the proposed method is the same as the time taken for a conventional multiecho gradient‐echo imaging sequence without compensation. The performance and efficiency of the proposed method were demonstrated and evaluated at 4.7 T. Magn Reson Med 60:1388–1395, 2008. © 2008 Wiley‐Liss, Inc.
Keywords:magnetic resonance imaging  gradient echo  susceptibility artifact  T  temporal resolution
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