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library:time_to_echo [2025/05/01 01:32] – scott | library:time_to_echo [2025/05/01 01:57] (current) – scott | ||
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==TE for T2* weighting== | ==TE for T2* weighting== | ||
- | Without the strong refocusing pulses of a fast spin echo, transverse magnetization will decay rapidly due to the compounding effect of both T2 and T2* processes. This much shorter decay time means that TE's need to be much shorter, generally less than 30ms, or all the signal will have been lost. | + | Without the strong refocusing pulses of a fast spin echo, transverse magnetization will decay rapidly due to the compounding effect of both T2 and T2* processes. This much shorter decay time means that TE's need to be much shorter, generally less than 30ms, or all the signal will have been lost. The most common method of achieving T2* weighting is to use a 2D gradient echo with a TE of ~20ms. It may be necessary to reduce the receiver bandwidth to recover SNR as well as allow for later TE selections. There are gradient echo sequences with special modifications that allow for enhanced T2* imaging such as Multi-echo GRE and SWAN. Note the T2* weighted image below demonstrating hemorrhage, TE ~18ms. |
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+ | ==In and Out of Phase TE== | ||
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+ | When utilizing fast 3D gradient echo sequences, a TE time may no longer be selectable, and instead the options are limited to an ' | ||
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