Fourier correlation analysis of GC-spectra of sheep milk and dairy.
Hilma, Elena ; Mierlita, Dan ; Teusdea, Alin Cristian 等
Abstract: Authors present the discrimination performances of
amplitude and phase-only Fourier correlation over the "twin"
typed GC-spectra of sheep milk and ripened cheese. Therefore are built
up the correlation matrix over the 12 analysed GC-spectra in both the
amplitude and phase domains, in order to assess the most robust Fourier
correlation method for the "twin" GC-spectra discrimination.
Key words: phase-only, Fourier correlation, GC-spectra, sheep milk.
1. INTRODUCTION
One way to measure the discrimination of "twin" type
samples is the Fourier correlation analysis. Such a method is Fourier
correlation (FC) with the classical process in the amplitude domain
(AmC). The amplitude domain Fourier correlation doesn't counts the
variation speed (i.e. the first order derivative) of the analysed
functions and thus for "twin" functions can fail their
discrimination. Phase-only Fourier correlation (POC) (Chien, 2004; Ito
et al., 2004; Miyazawa et al., 2005) as it is named takes into account
the phase or the variation speed of amplitude values of neighbouring
points from the profile data. Theoretically it can discriminate better
the "twin" functions. The present paperwork analyse the
discrimination performances of the (AmC) and (POC) over the
"twin" type spectra. Spectra database used consists of
"twin" gas-chromatogram (GC) spectra. The GC-spectra were
built up in food processing experiment with sheep milk and dairy.
2. PATTERN RECOGNITION CORRELATION METHODS
Fourier correlation process is used for function discrimination.
That means one function is "compared" with several ones.
Comparison criteria concludes if the compared functions are or not
similar each other. The comparison process works basically with two
functions at the same time. In our case the comparison method is the
cross-correlation and the functions are the GC-spectra. In a single
cross-correlation process the two functions are denoted as reference and
non-reference.
The classical amplitude cross-correlation (AmC) considers two
(N-size) GC-spectra: ref(x) as reference GC-spectrum and nref(x) as
non-reference GC-spectrum. The discrete Fourier transforms of these
GC-spectra, denoted as Ref(u) and NRef(u), are given by (Teusdea, 2009)
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (1)
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (2)
e NR(N) N [[NRe (N) x [bar.Ref(u)].sup.[??]] (3)
e f NR(N) = [[NRef(N) x N [bar.NRe(N)].sup.N,N], (4)
where REF Nu) and NREF(N) are the amplitude part,
[[phi].sub.ref](u) and [[phi].sub.nref] (u), are the phase part of the
Fourier transforms.
Classical correlation function, [NRN.sub.RN](x), is the inverse
discrete Fourier transform of classical cross-spectrum, given by
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (5)
where the N[[phi].sub.rn](U) is the phase difference between the
reference and non-reference function. This function presents a highly
wide cross-correlation peak when ref(x) = nref(x). When eNR(N) [not
equal to] nref Nx) then the cross-correlation peak strongly decreases.
The phase-only cross-spectrum is defined by (Ito et al., 2004;
Miyazawa et al., 2006)
RN_CS N REFNu) x N REF ([uNe.sup.i[DELTA]N] [RN.sup.(u)]/[absolute
value of e NR (NNNREF (u) x [e.sup.iNN] [rn.sup.(u)] N
[e.sup.i[DELTA][phi]] [rn.sup.(N) (6)
and thus the phase-only cross-correlation is given by Fourier
transform of the phase-only cross-spectrum (Teusdea, 2009)
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (7)
If ref(N) = e f NR(x) then [NN.sub.RN](N) = N and the phase only
correlation is give by (Teusdea, 2009)
POC(x) N 1/N [[summation].sup.N.sub.u=1] [1 x [e.sup.-2[pi]i/N] ux
x [e.sup.-2[pi]i/N vy] = N(x). (8)
This means that if the two GC-spectra are identical then the POC
gives a highly sharp peak so the matching accuracy is higher than in the
classical method.
Better understanding and symmetry with first order statistical
correlation coefficient, was used the normalized Fourier Correlation
coefficient NFCC given by (Teusdea, 2009)
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (9)
where [N.sup.NN] is the inverse Fourier transform operator, F(u)
and G(u) are the Fourier transform of the N(x) and g(x) functions. If
these Fourier transforms are replaced with the phase-only part of them
then the NFCC becomes PhNFCC, otherwise is denoted as AmNFCC.
3. RESULTS AND DISCUSSION
In the sheep dairy benchmark experiment were considered samples of
fresh sheep milk without (M0) and with 0.05% (M005), 0.10% (M010), 0.15%
(M015) fish oil additive. The fish oil is added to improve the fatty
acid content of the milk and thus mainly to gain the [N.sub.3] and
[[omega].sub.6] content with cardiological and neurogical benefits for
the human body (Soft et al., 2010).
After the milk preparation were processed samples of ripened spun
paste cheese (SPC0, SPC005, SPC010, SPC015) and ripened Teleme cheese
(TC0, TC005, TC010, TC015). The main goal of the experiment was to
analyse the fatty acid profiles from the 12 mentioned samples. Hence
were done the GC-spectra of these samples. The GC-spectra were very
similar or "twin" spectra because, from the fatty acids
profile point of view, the analysed samples were statistically
strong-correlated.
As mentioned above one accurate way to discriminate the "twin
profile" data is the Fourier correlation in the amplitude domain
(eqn. 1-5) and phase domain (eqn. 6-8).
Correlation matrix between the 12 GC-spectra of the milk, spun
paste cheese and Teleme cheese were built for amplitude correlation
coefficient AmNFCC (figure 1) and phase-only correlation coefficient
PhNFCC (figure 2). The correlation values were built up for several
Fourier vector size [N.sup.N],m = [bar.1,20], and then were calculated
theirs [N.sup.P] norm (p = 2.5N.
[FIGURE 1 OMITTED]
[FIGURE 2 OMITTED]
This algorithm increases the accuracy of the correlation process.
The statistical significance of the AmNFCC and PhNFCC is: 0-0.35 strong
discrimination, 0.35-0.70 good discrimination and 0.70-1.00 poor
discrimination.
As it showed in figure 1 the AmNFCC has poor discrimination of
"twin" GC-spectra as the correlation matrix graph is dark
coloured. Figure 2 shows that the PhNFCC has strong discrimination of
"twin" GC-spectra as the correlation matrix graph is light
coloured in the non-diagonal area.
Figure 3 presents the percentage of discrimination values for
AmNFCC and PhNFCC. It is revealed that only in 30.30% cases the
amplitude Fourier correlation do not fail to discriminate the
"twin" type analysed GC-spectra. In the same way the
phase-only Fourier correlation has a 100% of discrimination of
"twin" type analysed GC-spectra.
4. CONCLUSION
In this paper, there are presented the Fourier correlations in
amplitude (AmNFCC) and phase-only (PhNFCC) domain for discrimination the
"twin" type GC-spectra of sheep milk, ripened spun paste
cheese and ripened Teleme cheese. The results in figures 1-3 emphasizes
that just the phase-only Fourier correlation (PhNFCC) has 100%
discrimination performances on "twin" type GC-spectra. The
Fourier correlation in the amplitude domain (AmNFCC) fails in 69.70% to
discriminate the same "twin" GC-spectra.
Our future plan is to work with much larger "twin"
GC-spectra database to ensure higher statistical significance.
5. ACKNOWLEDGEMENTS
This work was supported by CNCSIS-UEFISCSU, Romanian project number
PNII-IDEI, ID-679/2008, number 1082/2009.
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Fig. 3. Comparison of the statistical significance of the
correlation matrix values ("twin" discrimination statistical
threshold is [less than or equal to] 0.7).
<0.7 >0.7
AmNFCC 30.30 69.70
PhNFCC 100.00 0.00
Note: Table made from bar graph.