Magnetic Resonance Imaging

Joseph P. Hornak, Ph.D.


Fourier Transforms - I


Fourier Transform

A mathematical technique capable of converting a time domain signal to a frequency domain signal and vice versa.


The + and - Frequency Problem

M, starting at +x, CW rotating about the Z axis,

Mx(t)




FT



 




My(t)




FT



 




Solution: input Mx and My as RE and IM



Signal Detection

Linear Detection
Detecting just Mx or My, the computer discards half of the frequency domain data.



 

Quadrature Detection
Detection of both Mx and My.



The Fourier Transform

An FT is defined by the integral

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 ).


To understand the FT, examine the product of f(t) with cos(w t) for 1 < w < 10,
then the summation of the values of this product between 1 and 10 seconds.

w=1




w=2




w=3




w=4




w=5




w=6




w=7




w=8




w=9




w=10




f(w)


inverse Fourier transform (IFT)




Phase Correction

The FT makes use of RE and IM inputs:
    Mx = RE input
    My = IM input


Consider:   f(t) = e-at e-i2pnt

MX (Real)



MY (Imaginary)


If the inputs are switched... cosine part input as IM, sine part input as RE

MX (Real)



MY (Imaginary)


To obtain an absorption spectrum...



FID with 40o phase shift in the RE and IM

MX (Real)



MY (Imaginary)


The coordinate transformation matrix can be used with f = - 45o.

The phase corrected FIDs:

MX (Real)



MY (Imaginary)


FT phase corrected FIDs gives an absorption spectrum for RE output of the FT.

MX (Real)



MY (Imaginary)

This correction can be done in the frequency domain as well as in the time domain.



Constant (b) and Linear (m) phase corrections.

f = m n + b

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)


Copyright © 2000 J.P. Hornak.
All Rights Reserved.