Digital Signal Processing Reference
In-Depth Information
EXACT RECONSTRUCTION of the TRUE NUMBER of GENUINE FREQUENCIES and AMPLITUDES by FPT (+) : NOISELESS FID
FREQUENCIES in pFPT (+) : ν
+
k,Q = [ −i /(2 πτ )] ln (z +
k,Q ) , zFPT (+) : ν
+
k,P = [ −i /(2 πτ )] ln (z +
k,P ) , INPUT POLES (x) : ν k
AMPLITUDES in FPT (+) : d +
k = P +
K (z +
k,Q ) / [(d/dz +
k,Q )Q +
K (z +
k,Q )] = (p +
K /q +
K
(z +
k,Q −z +
m,P ) / [(z +
k,Q −z +
m,Q )] m k , INPUT (x) : d k
GENUINE FREQUENCIES: POSITIVE IMAGINARY PARTS & CHEMICAL SHIFTS witin 0.985 ppm (Lipid : # 1) − 4.68 ppm (Water : # 25)
FROISSART DOUBLETS ( ν
K ) Π m=1
+
k,Q ; POLES = ZEROS ): NEGATIVE IMAGINARY PARTS & ZERO−VALUED AMPLITUDES
GENUINE & SPURIOUS ( FROISSART ) RESONANCES SEPARATED in 2 DISJOINT REGIONS, Im( ν
+
k,P = ν
+
k ) > 0 and Im( ν
+
k ) < 0
+
k,Q [ pFPT (+) ] , Pade zeros (
+
k,P [ zFPT (+) ] , Input poles (x) :
Argand plot for frequencies ; Pade poles (o) :
ν
) :
ν
ν k
−0.1
−0.05
0
PADE : FPT (+)
TOTAL NUMBER of
FREQUENCIES
K T = K = 128
NUMBER of
FROISSART DOUBLETS
K F = 103
NUMBER of
GENUINE FREQUENCIES
K G = K T − K F = 25
0.05
0.1
25
Water
B 0 = 1.5T
0.15
1
PARTIAL
FID LENGTH USED
N P = 2K T = 256
Lipid
0.2
0.25
CONVERGED
12
11
10
9
8
7
6
5
4
3
2
1
0
−1
−2
−3
+
k ) (ppm)
(i) Re(
ν
Absolute values of amplitudes ; Fast Pade Transform, FPT + (o) : |d +
k | , Input (x) : |d k |
0.18
PADE : FPT (+)
TOTAL NUMBER of
0.16
0.14
AMPLITUDES
K T = K = 128
1
Lipid
0.12
NUMBER of
0.1
ZERO−VALUED
B 0 = 1.5T
0.08
FROISSART AMPLITUDES
K F = 103
25
0.06
Water
PARTIAL
FID LENGTH USED
N P = 2K T = 256
NUMBER of
0.04
GENUINE AMPLITUDES
K G = K T − K F = 25
0.02
CONVERGED
0
12
11
10
9
8
7
6
5
4
3
2
1
0
−1
−2
−3
(ii) Chemical shift (ppm)
FIGURE 6.2
Froissart doublets for unequivocal determination of the exact number K G of
the genuine frequencies and amplitudes from the total number K T
≡K of the
spectral parameters reconstructed by the FPT (+) for the noiseless FID with
input data from Table 3.1. In panel (i), the FPT (+) separates the genuine
from spurious frequencies in the two nonoverlapping regions, Im(ν + ) > 0 and
Im(ν + ) < 0, respectively. In panel (ii), all the spurious (Froissart) amplitudes
are unambiguously identified by their zero values.
Search WWH ::




Custom Search