
Mx(t)


















Think of f(w) as the overlap of f(t) with a wave of frequency w .

This is easy to picture by looking at RE part of f(w) only.

Consider f( t ) = cos( 4t ) + cos( 9t ).

| w=1 |
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| w=2 |
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| w=3 |
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| w=4 |
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| w=5 |
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| w=6 |
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| w=7 |
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| w=8 |
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| w=9 |
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| w=10 |
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| f(w) | ![]() |


MX (Real)




MX (Real)





MX (Real)




The phase corrected FIDs:
MX (Real)




MX (Real)




This correction can be done in the frequency domain as well as in the time domain.
Constant phase corrections arise from the inability of the spectrometer to detect the exact
Mxand My.
Linear phase corrections, m, arise from the inability of the spectrometer to detect transverse magnetization starting immediately after the RF pulse.
In MRI, Mx or My signals rarely displayed. Instead a magnitude signal is used. magnitude = square root (Mx2 and My2)