Submit manuscript...
Journal of
eISSN: 2572-8466

Applied Biotechnology & Bioengineering

Mini Review Volume 7 Issue 1

Functionally-enhanced derivative spectroscopy (FEDS): a powerful tool to increase of spectral resolution in the mid-infrared advanced analysis of complex samples–a mini review

Manuel Palencia,1 Viviana Garcés-Villegas,1,2 Diego F Restrepo,1 Jina M Martínez,1,2 Luis R Anaya–Tatis,2 Enrique M Combatt3

1Department of Chemistry, Universidad del Valle, Colombia
2Mindtech Research Group (Mindtech-RG), Colombia
3Department of Agricultural Engineering and Rural Development, Universidad de Cordoba, Colombia

Correspondence: Manuel Palencia, Department of Chemistry, Universidad del Valle, Campus Melendez, Building E-20, Street 100-00, Cali–Colombia

Received: January 06, 2020 | Published: February 6, 2020

Citation: Palencia M, Garcés-Villegas V, Restrepo DF, et al. Functionally-enhanced derivative spectroscopy (FEDS): a powerful tool to increase of spectral resolution in the mid-infrared advanced analysis of complex samples–a mini review. J Appl Biotechnol Bioeng 2020;7(1):43-46. DOI: 10.15406/jabb.2020.07.00214

Download PDF

Abstract

Functionally-Enhanced Derivative Spectroscopy (FEDS) is a simple, fast and easy to use deconvolution method based on the combination of derivative spectroscopy and simple functional algorithms. As analytical technique has demonstrated to be a powerful tool for analysis of spectral signals of mid-infrared spectra. In specific, FEDS produces the separation of overlapped signals through a transformation of the spectrum that consists of making the signals more acute and intense depending on the signal to noise ratio. The purpose of this review is to provide a theoretical and applied overview of ability of FEDS for the improving spectral analysis of complex samples with importance in materials, food and biomedical engineering, environmental sciences, microbiology, biotechnology and biological, chemical and physical science, among others.

Keywords: derivative spectroscopy, functional transformation, mid-infrared spectrum, deconvolution, signal overlap

Abbreviations

IR, infrared; FEDS, functionally-enhanced derivative spectroscopy; DFT, density functional theory; SNR, signal-noise ratio

Introduction

Background of analytical problem

Infrared spectroscopy (IR spectroscopy) is a well-known technique based on the interaction of IR radiation with the matter. By this interaction, changes of vibrational state of functional groups are produced.1–5 These changes are visualized in the IR spectra as signals associated with the wavelength of vibration, or as usually is done in chemistry, with the wavenumber, but also, with the intensity of absorbed radiation (absorbance).2,3 Thus, each molecule has associated a characteristic vibrational patter which gives qualitative and quantitative information about molecular structure. The component quantitative is resulting of Beer-Lambert Law which describes a linear relationship between the absorbance and the concentration.2,3 However, as the number of components in the analytic sample increases, the vibrational patter is increased in complexity. The reason of the above is that each component into the sample has its own vibrational patter and, in consequence, overlap of signals is produced. In addition, the molecular vibration is affected by the chemical environment, or being the same, by the intra- and intermolecular interactions, and therefore, as a result of the above, the signal broadening is produced and overlap is increased. But also, fluctuations of signals, displacements and the presence of noise are factors which are usually identified in the typical IR spectra.1–5

Many applications of IR spectroscopy have been described, and these have been focused in the positive aspects of technique being generally omitted their limitations. Some applications for the study of complex and dynamic systems in microbiology and biotechnology are: to characterize molecular composition and stress response in foodborne pathogenic bacteria,6 analysis of microbial cell,7 identification and discrimination of bacteria,8 real-time monitoring of nitrile biotransformations,9 microbial biodegradation pathways,10 monitoring of bacterial biofilm formation on implantable devices,11 characterization of structural properties of fungal-bacterial biofilms.12 Applications in other fields also have been described and these are easily localized in specialized publications.1–5 From analytical overview, the quality analysis is directly related with the quality of information obtained. Thus, in a typical IR analysis, overlap and broadening of signals is not desired. However, in many cases this cannot be avoided and the analysis is strongly restricted. The above is a major problem when complexity of sample is increased (e.g., blood, biofilms, soils, animal and plant tissues, polymeric composites, among others), and therefore, the IR technique has seen limited their applications to relatively simple systems (e.g., individual molecules, binary systems) or to the identification of characteristic signals of one or more components in a mixture (e.g., identification of carbonyl groups of esters in a matrix of polypropylene).6-11 In order to resolve these problems different strategies have been used, being the theoretical and computational approach, and the mathematical approach, the more generalized, including Fourier transform, Derivative spectroscopy and Functionally-Enhanced Derivative Spectroscopy (FEDS). The purpose of this review is to provide a theoretical and applied overview about the ability of FEDS for the improving spectral analysis of complex samples with importance in materials, food and biomedical engineering, environmental sciences, microbiology, biotechnology, and biological, chemical and physical sciences, among others.

Previous approaches to FEDS

Theoretical and computational approach is based in theoretical modeling of vibrational patters of molecules by advanced procedures, as Density Functional Theory or DFT, thus, theorical spectrum of molecules is obtained by the combination of theory and calculations. However, its application requires specialized knowledge in quantum and computational chemistry, specialized software (e.g., Gaussian software), and a relatively high computational cost depending of complexity of target problem. But also, the use of this approach is limited to simple molecules and systems, where the predicted spectrum is depending of computational code used, in consequence, it not rare that theoretical spectrum differs of experimental spectrum. Many examples for the study of simple molecules have been published, by instance, vibrational analysis of nucleic acids,13,14 amino acids as glycine and cysteine,15,16 or biological components as N-Acetyl-D-glucosamine and D-Glucuronic Acid.17 On the other hand, mathematical approach is based on to consider the spectrum as a continuous mathematical function and, therefore, several mathematical strategies can be used. The most common technique is the Fourier deconvolution or Fourier self-deconvolution algorithm.18–21 However, though from a conceptual approach the Fourier self-deconvolution is simple, its application is limited by the complexity of computation, the appearing of negative intensities from calculations, the highly sensitive to the noise and the appearing of 'false' signals resulting of mathematical arguments without physical meaning.18

Other strategy is the derivative spectroscopy, mainly, the second-order derivate. The derivation process yields helpful features associated with the spectrum such as maximum and minimum points (first-order derivative) and points of inflection (second-order derivative). Thus, the first-order derivative is the slope of the “spectrum function” in function of wavenumber, or wavelength. Whereas the first-order derivative has a value of zero at the same wavelengths where the original spectrum has a maximum or minimum, the second-order derivative has a value equal to zero where the first-order derivative reaches a minimum or maximum absorbance; but also, these points correspond to points of inflection in the original spectrum. In this way, the first and second order derivatives facilitate the extracting of features specifically associated with the spectra; however, upper derivatives are hardly rationalized since these don't show a direct relation with original function.22,23 In addition, the most important effect of the derivative method is that broad bands are suppressed in comparison with sharp bands and, in consequence, this suppression increases with the increase of derivative order.22–27 An unwished effect of the derivative spectroscopy is that the signal-noise ratio (SNR) decreases as derivatives with higher orders are used; therefore, for the derivative process, it is important the control of the degree of smoothing that is applied in order to adapt the procedure to different analytical problems.22,23

FEDS spectroscopy: fundaments

In contrast with the strategies previously described, FEDS is a simple method for the deconvolution and the increase of spectral resolution of signals, based on the transformation of spectrum by the use of derivative algorithm enhanced by functional transformations. In addition, it has the following advantages: easy use, no require high computational capacity, adaptability according to objective, no requires advanced software, and produces the deconvolution of spectrum coherently with original IR spectrum.28 FEDS algorithm is based on the application of functional transformations of spectrum and first-order differentiation. By FEDS, the spectrum is considered a collection of data which correspond to points of function where for each value of wavenumber (v) is obtained one absorbance value (a). In consequence, a is function of v, and therefore it can be written to be w, where w denotes a function w:(v) which describes the IR spectrum. After, it is defined a new function y which is obtained by the calculation of inverse of respective absorbance. Thus, if a is the absorbance of w(v) then a-1 will be the absorbance of y(v). Later, first-order derivate of y(v) is calculated with a ‘small’ consideration.

Since the difference between two adjacent values of v is constant, the function w is given by the difference between absorbances instead of quotient between the difference of absorbance (i.e., aj+1aj where j denotes the j-th position in the spectrum) and the difference between respective v (i.e., vj+1vj). The above defines the auxiliary function p (the notation p comes from the Spanish word 'primera' alluding to the use of the first derivative). The following step consists in to use the mathematical operator 1/(|x|)0.5 where x denotes any mathematical argument, and it is used to define the working function called Function P. Note that this operator is equal to scale factor defined under the wavelet concept, which is used to define the general expression of ‘mother wavelet’. Function P is defined for each vj as

P j = 1+ a j | p j | MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsaqaaaaa aaaaWdbiaadcfajuaGpaWaaSbaaSqaaKqzadWdbiaadQgaaSWdaeqa aKqzGeWdbiabg2da9Kqbaoaalaaak8aabaqcLbsapeGaaGymaiabgU caRiaadggajuaGpaWaaSbaaSqaaKqzadWdbiaadQgaaSWdaeqaaaGc baqcfa4dbmaakaaak8aabaqcfa4dbmaaemaak8aabaqcLbsapeGaam iCaKqba+aadaWgaaWcbaqcLbmapeGaamOAaaWcpaqabaaak8qacaGL hWUaayjcSdaaleqaaaaaaaa@4C8C@ (1)

where (1 + aj) is an amplification factor for the assignation of a weight congruent with absorbance intensity (i.e., small values of absorbance in the experimental spectrum will be amplified using small values of aj since 1+ aj will be a small factor, contrary to the expected for large values of aj). It is important avoid confusions with the notation used, and therefore it is suggested the use of the same terms in order to achieve a language uniformity. Details description is given by Palencia.28

An important aspect for the correct application of FEDS is the pre-treatment of data. For each region of spectrum being analyzed, data must be auto-scaled with respect to the values of minimum and maximum absorbances (amin and amax, respectively).

b j = a j a min a max a min MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGIb qcfa4aaSbaaeaajugWaiaadQgaaKqbagqaaKqzGeGaeyypa0tcfa4a aSaaaOqaaKqzGeGaamyyaKqbaoaaBaaabaqcLbmacaWGQbaajuaGbe aajugibiabgkHiTiaadggajuaGdaWgaaqaaKqzadGaamyBaiaadMga caWGUbaajuaGbeaaaOqaaKqzGeGaamyyaKqbaoaaBaaabaqcLbmaca WGTbGaamyyaiaadIhaaKqbagqaaKqzGeGaeyOeI0IaamyyaKqbaoaa BaaabaqcLbmacaWGTbGaamyAaiaad6gaaKqbagqaaaaaaaa@57D1@ (2)

where aj and bj are the experimental absorbance and the corresponding auto-scaled absorbance, respectively. In order to avoid calculation mistakes resulting to scaling from 0 to 1 during the application of FEDS algorithm, the zero absorbance was approximated by the calculation of average value between two adjacent values of absorbance satisfying that bj-1 < bj < bj+1 with bj = 0 (deterministic approximation). Since derivative spectrum is strongly sensitive to the noise in the original signal, the smoothing of spectral noise must be decreased by the use of average-based spectral filter (ABSF).28 ABSF is given by

ABSF( b i ;N=20)= 1 3   j j+2 ( b j )| N=1 N=20 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsaqaaaaa aaaaWdbiaadgeacaWGcbGaam4uaiaadAeacaGGOaGaamOyaKqba+aa daWgaaWcbaqcLbmapeGaamyAaaWcpaqabaqcLbsapeGaai4oaiaad6 eacqGH9aqpcaaIYaGaaGimaiaacMcacqGH9aqpjuaGdaabcaGcpaqa aKqba+qadaWcaaGcpaqaaKqzGeWdbiaaigdaaOWdaeaajugib8qaca aIZaaaaiaacckajuaGdaGfWbGcbeWcpaqaaKqzadWdbiaadQgaaSWd aeaajugWa8qacaWGQbGaey4kaSIaaGOmaaqdpaqaaKqzajWdbiabgg HiLdaajuaGdaqadaGcpaqaaKqzGeWdbiaadkgajuaGpaWaaSbaaSqa aKqzadWdbiaadQgaaSWdaeqaaaGcpeGaayjkaiaawMcaaaGaayjcSd qcfa4damaaDaaaleaajugWa8qacaWGobGaeyypa0JaaGymaaWcpaqa aKqzadWdbiaad6eacqGH9aqpcaaIYaGaaGimaaaaaaa@65C4@ (3)

ABSF is the moving average with a data window of 3 and 20 cycles (N = 20). Thus, for each bj, bj+1 and bj+2 the corresponding average value is calculated, and subsequently, this procedure is repeated N times. However, as the spectrum line function in the absorbance domain is modified by the use of Equation 3, the same transformation of data is performed on values of wavenumber (v) in order to correct the displacements respect to original spectrum (i.e., maximum points in original spectrum should be the same in the original and smoothed spectra).28

FEDS applications

FEDS has been used for the structural study of humin and its interaction with humic acids by Fourier-transform mid-infrared spectroscopy permitting to identify the wavenumbers of hydroxyl groups of humic acids in extracted of humified organic matter.29 In a similar context, during edaphology studies, FEDS has been used for the study, by attenuated total reflectance spectroscopy, structural changes of humified organic matter by chemical perturbations via alkaline dissolution. Results showed that FEDS can be used to increase the differentiation between soil spectra, and possibility the identification of signals highly overlapped.30 In addition, FEDS have been used to determine weak signals in spectra of nitrogen-fixing bacterial biofilms.31 On the other hand, FEDS was used to explore the deconvolution of surface plasmon of inorganic nanoparticles. Though contraction of signal was obtained, results permits conclude that FEDS technique can be used for the building of mixture models of spectral signals in order to achieve a correlation with their components.32 The mid-infrared spectral characterization of fish scales: “Bocachico” (Prochilodus magdalenae) was performed by FEDS permitting the characterization of collagen and identification of hydroxyapatite.33 In the study of binary mixture, FEDS was used for the solve the problem of the overlap of spectral signals in mixtures of triethylamine-acetone demonstrating its capability to extract signals from small fluctuations of line function of IR spectra.34

Conclusion

FEDS is an analytical tool which enormous potential in the analysis of complex systems. It has as advantage its easy implementation and interpretation. In addition, it is adaptable to much types of problems and maximize the potential use of IR spectroscopy. Though the most of researches has been centered to the use of IR spectra, it is concluded from review of fundaments that FEDS can be implemented in any functional relationship of physical variables. On the other hand, FEDS transform of IR spectra permits the building of new and more specific spectral libraries, of target substances in many multicomponent systems with importance in biotechnology and bioengineering. In addition, it eases the comparison of spectra and the study of spectral signals with very low intensities permitting to extract analytical information from signal-noise mixtures, and the deconvolution of overlapped signals.

Acknowledgments

Authors thanks to Universidad del Valle, Mindtech s.a.s., and Universidad de Cordoba.

Conflicts of interest

Authors declare that there is no conflict of interest.

Funding

None.

References

  1. Haas J, Mizaikoff B. Advances in Mid-Infrared Spectroscopy for Chemical Analysis. Ann Rev Anal Chem. 2016;9:45–68.
  2. Monnier GF. A review of infrared spectroscopy in microarchaeology: Methods, applications, and recent trends. J Archaeol Sci Reports. 2018;18:806–823.
  3. Prieto N, Pawluczyc O, Dugan M, et al. A Review of the Principles and Applications of Near-Infrared Spectroscopy to Characterize Meat, Fat, and Meat Products. Appl Spectr. 2017;71:3702817709299.
  4. Tinti AT, Tugnoli V, Bonora S, et al. Recent applications of vibrational mid-Infrared (IR) spectroscopy for studying soil components: a review. J Central Eur Agricul. 2015;16:1–22.
  5. Pasquini C. Near Infrared Spectroscopy: fundamentals, practical aspects and analytical applications. J Brazilian Che Soc. 2003. 14 p.
  6. Alvarez-Ordoñez A, Mouwen D, Lopez M, et al. Fourier transform infrared spectroscopy as a tool to characterize molecular composition and stress response in foodborne pathogenic bacteria. J Microbiol Met. 2011;84:369–378.
  7. Ojeda J, Dittrich M. Fourier transform infrared spectroscopy for molecular analysis of microbial cells. Chapter 8. In Navid A. Microbial systems biology: Methods and Protocols, Methods in Molecular Biology. Microbial Systems Biology. 2012. p. 187–211.
  8. Prakash J, Kar S, Lin C, et al. Identification and discrimination of bacteria using Fourier transform infrared spectroscopy. Spectrochim. Act Part A: Mol Biomol Spectr. 2013;116:478–484.
  9. Dadd M, Sharp D, Pettman A, et al. Real-time monitoring of nitrile biotransformations by mid-infrared spectroscopy. J Microbiol Met. 2000;41:69–75.
  10. Huang W, Hopper D, Goodacre R, et al. Rapid characterization of microbial biodegradation pathways by FT-IR spectroscopy. J Microbiol Met. 2006;67:273–280.
  11. Khatoon Z, McTiernan C, Suuronen E, et al. Bacterial biofilm formation on implantable devices and approaches to its treatment and prevention. Heliyon. 2018;4:e01067.
  12. Singhalage D, Seneviratne G, Madawala S, et al. Characterization of structural properties of fungal-bacterial biofilms by Fourier Transform Infrared Spectroscopy. Ceylon J Sci. 2018;47:77–83.
  13. Guan Y, Wurrey CJ, Thomas GJ. Vibrational analysis of nucleic acids I. The phosphodiester group in dimethyl phosphate model compounds: (CH3O2)PO2-, (CD3O)2PO2- and (13CH3O)2PO2. Biophys J. 1994;66:225–235.
  14. Guan Y, Thomas GJ. Vibrational analysis of nucleic acids IV. Normal modes of the DNA phosphodiester structure modeled by diethyl phosphate. Biopolym. 1994;66:813–835.
  15. Kumar S, Rai AK, Singh VB, et al. Vibrational spectrum of glycine molecule. Spectrochim Act Part A: Mol Biomol Spectr. 2005;61(11–12):2741–2746.
  16. Parker, S. Assignment of the vibrational spectrum of L-cysteine. Chem Phys. 2013;424:75–79.
  17. Kovacs A, Nyerges B, Izvekov V. Vibrational Analysis of N-Acetyl- D-glucosamine and D-Glucuronic Acid. J Phys Chem. 2008;112(18):5728–5735.
  18. Friesen W, Michaelian K. Deconvolution and Curve-Fitting in the Analysis of Complex Spectra: The CH Stretching Region in Infrared Spectra of Coal. Appl Spectr. 1991;45:50–56.  
  19. Vazhnova T, Lukyanov D. Fourier Self-Deconvolution of the IR Spectra as a Tool for Investigation of Distinct Functional Groups in Porous Materials: Brønsted Acid Sites in Zeolites. Anal Chem. 2013;85:11291–1296.
  20. Yooke PB. Fourier self-deconvolution in IR spectroscopy. TrAC Trends in Analytical Chemistry. 1988;7:130–136.
  21. Brangule A, Agris K. Importance of FTIR Spectra Deconvolution for the Analysis of Amorphous Calcium Phosphates. IOP Conf Series: Mat Sci Eng. 2015;77:012027.
  22. Nishikida K, Nishio E, Hannah R. Selected Applications of Modern FT-IR Techniques. Tokio. Gordon and Breah Publishers; 1995. 281 p.
  23. Stuart B. Infrared spectroscopy: Fundaments and applications. Wiley; 2004. 221 p.
  24. Rieppo L, Saarakkala S, Narhi T, et al. Application of second derivative spectroscopy for increasing molecular specificity of fourier transform infrared spectroscopic imaging of articular cartilage. Osteoarthritis and Cartilage. 2012;20:451–459.
  25. Gallignani M, Rondón RA, Ovalles JF, et al. Transmission FTIR derivative spectroscopy for estimation of furosemide in raw material and tablet dosage form. Acta Pharm Sin B. 2014;4:376–383.
  26.  Fetterman MR. Fourier-transform infrared derivative spectroscopy with an improved signal-to-noise ratio. Optics Letters. 2005;30:2311–2313.
  27. Palencia VJ, Martinez JM. Spectral data transformation analysis by simple mathematical functions: Fourier transform infrared spectrum. J Sci Technol Appl. 2017;3:44–55.
  28. Palencia M. Functional transformation of Fourier-transform mid-infrared spectrum for improving spectral specificity by simple algorithm based on wavelet-like functions. J Adv Res. 2018;14:53–62.
  29. Garcia A, Combatt E, Palencia M. Structural study of humin and its interaction with humic acids by Fourier-transform mid-infrared spectroscopy. J Sci Technol Appl. 2018;4:28–39.
  30. Restrepo DF, Palencia M, Palencia VJ. Study by attenuated total reflectance spectroscopy of structural changes of humified organic matter by chemical perturbations via alkaline dissolution. J Sci Technol Appl. 2018;4:49–59.
  31. Berrio ME, Palencia SL, Lerma TA, et al. Bacterial colonization modelling on soil particles: Effect of humic acids on the formation of nitrogen-fixing bacteria biofilms. J Sci Technol Appl. 2018;5:33–44.
  32. Sanchez Y, Garcia A, Palencia M. Determination and distribution of size of inorganic particles by spectral deconvolution of surface plasmon resonance. J Sci Technol Appl. 2018;5:45–54
  33. Anaya-Tatis LR, Libreros KH, Palencia VJ, et al. Mid-infrared spectral characterization of fish scales: "Bocachico" (Prochilodus magdalenae) by functionally-enhanced derivative spectroscopy (FEDS) - A methodological approach. J Sci Technol Appl. 2019;6:28–39.
  34. Otalora A. Palencia M. Application of functionally-enhanced derivative spectroscopy (FEDS) to the problem of the overlap of spectral signals in binary mixtures: Triethylamine-acetone. J Sci Technol Appl. 2019;6:96–107.
Creative Commons Attribution License

©2020 Palencia, et al. This is an open access article distributed under the terms of the, which permits unrestricted use, distribution, and build upon your work non-commercially.