T1-weighted image

[Inaki4]

I think I managed to understand what happens.

First of all, I was assuming that TR wasn't long enough to allow the transverse magnetization to fully vanish, but it is supposed to be designed for that purpose. This means that in my last image, after each TR, there is only longitudinal magnetization.

My first question was:

(11-26-2015 07:46 PM)Inaki4 Wrote:  1) According to this, it doesn't make sense to measure after the first 90º pulse right? That way you would measure the whole original longitudinal component (this would make sense for a PD-weighted image).

The answer is that indeed it doesn't make sense to measure after the first pulse. This is because after the first pulse we bring down the whole longitudinal magnetization, so two tissues which only differ in their T1 relaxation time (same proton density) would be indistinguishable. If we wait for a TR short enough not to allow the longitudinal magnetization to fully recover and then use another 90º pulse to bring it to the XY plane, now it makes sense to measure because since both tissues have different T1, each of them would provide a different measurement, so we will get a T1-weighted image.

I verified this in the book Principles of Magnetic Resonance Imaging: A Signal Processing Perspective by Zhi-Pei Liang and Paul C. Lauterbur, where they explain that this first pulse is called preparatory pulse and it is discarded.

My second question was:

(11-26-2015 07:46 PM)Inaki4 Wrote:  2) If you repeat this periodically, the first 90º pulse would put the whole longitudinal Mz into the transverse plane. After a TR, you would apply a second 90º pulse to place a portion of the original longitudinal component (the portion with the highest T1 contrast). But TR after the second pulse, the portion of the longitudinal component you would place in the transverse plane is not the same as before, it would be less. And this would go on pulse after pulse. This image shows what I mean:

As I mentioned, the TR is assumed long enough to allow the transverse magnetization to vanish. TR after the first 90º pulse, just a portion of the longitudinal magnetization would be recovered. But when we bring it down to the XY plane with a second 90º pulse, the situation is exactly the same that after the first 90º pulse in terms of the longitudinal magnetization recovery. In both cases, it starts to recover from 0, so waiting TR after both pulses would allow to recover the exact same portion of longitudinal magnetization.

What matters for the recovery of the longitudinal magnetization is the Z-component density of spins at the time at which the recovery starts, but the two situations described (inmediately after the first and second 90º RF pulses) differ in the Y-component (if the RF pulse is applied in the X-axis) density of spins.