Organelle specific simultaneous Raman/green fluorescence protein microspectroscopy for living cell physicochemical studies

We demonstrate a novel bio‐spectroscopic technique, “simultaneous Raman/GFP microspectroscopy”. It enables organelle specific Raman microspectroscopy of living cells. Fission yeast, Schizosaccharomyces pombe, whose mitochondria are green fluorescence protein (GFP) labeled, is used as a test model system. Raman excitation laser and GFP excitation light irradiate the sample yeast cells simultaneously. GFP signal is monitored in the anti‐Stokes region where interference from Raman scattering is negligibly small. Of note, 13 568 Raman spectra measured from different points of 19 living yeast cells are categorized according to their GFP fluorescence intensities, with the use of a two‐component multivariate curve resolution with alternate least squares (MCR‐ALS) analysis in the anti‐Stokes region. This categorization allows us to know whether or not Raman spectra are taken from mitochondria. Raman spectra specific to mitochondria are obtained by an MCR‐ALS analysis in the Stokes region of 1389 strongly GFP positive spectra. Two mitochondria specific Raman spectra have been obtained. The first one is dominated by protein Raman bands and the second by lipid Raman bands, being consistent with the known molecular composition of mitochondria. In addition, the second spectrum shows a strong band of ergosterol at 1602 cm^?1, previously reported as “Raman spectroscopic signature of life of yeast.”     

Simultaneous fingerprint and high‐wavenumber fiber‐optic Raman spectroscopy enhances real‐time in vivo diagnosis of adenomatous polyps during colonoscopy

Colorectal cancer can be prevented if detected early (e.g., precancerous polyps‐adenoma). Endoscopic differential diagnosis of hyperplastic polyps (that have little or no risk of malignant transformation) and adenomas (that have prominent malignant latency) remains an unambiguous clinical challenge. Raman spectroscopy is an optical vibrational technique capable of probing biomolecular changes of tissue associated with neoplastic transformation. This work aims to apply a fiber‐optic simultaneous fingerprint (FP) and high wavenumber (HW) Raman spectroscopy technique for real‐time in vivo assessment of adenomatous polyps during clinical colonoscopy. We have developed a fiber‐optic Raman endoscopic technique capable of simultaneously acquiring both the FP (i.e., 800–1800 cm^–1) and HW (i.e., 2800–3600 cm^–1) Raman spectra from colorectal tissue subsurface (<200 µm) for real‐time assessment of colorectal carcinogenesis. In vivo FP/HW Raman spectra were acquired from 50 patients with 17 colorectal polyps during clinical colonoscopy. Prominent Raman spectral differences (p < 0.001) were found between hyperplastic (n = 118 spectra), adenoma (n = 184 spectra) that could be attributed to changes in inter‐ and intra‐cellular proteins, lipids, DNA and water structures and conformations. Simultaneous FP/HW Raman endoscopy provides a diagnostic sensitivity of 90.9% and specificity of 83.3% for differentiating adenoma from hyperplastic polyps, which is superior to either the FP or HW Raman technique alone. This study shows that simultaneous FP/HW Raman spectroscopy technique has the potential to be a clinically powerful tool for improving early diagnosis of adenomatous polyps in vivo during colonoscopic examination.

     

Raman spectroscopy for the non‐contact and non‐destructive monitoring of collagen damage within tissues

The non‐destructive and label‐free monitoring of extracellular matrix (ECM) remodeling and degradation processes is a great challenge. Raman spectroscopy is a non‐contact method that offers the possibility to analyze ECM in situ without the need for tissue processing. Here, we employed Raman spectroscopy for the detection of heart valve ECM, focusing on collagen fibers. We screened the leaflets of porcine aortic valves either directly after dissection or after treatment with collagenase. By comparing the fingerprint region of the Raman spectra of control and treated tissues (400–1800 cm^–1), we detected no significant differences based on Raman shifts; however, we found that increasing collagen degradation translated into decreasing Raman signal intensities. After these proof‐of‐principal experiments, we compared Raman spectra of native and cryopreserved valve tissues and revealed that the signal intensities of the frozen samples were significantly lower compared to those of native tissues, similar to the data seen in the enzymatically‐degraded tissues. In conclusion, our data demonstrate that Raman microscopy is a promising, non‐destructive and non‐contact tool to probe ECM state in situ. (© 2012 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

The structural analysis of three‐dimensional fibrous collagen hydrogels by raman microspectroscopy

To investigate molecular effects of 1‐Ethyl‐3‐(3‐dimethylaminopropyl) carbodiimide (EDC), EDC/N‐hydroxysuccinimide (NHS), glyceraldehyde cross‐linking as well as polymerization temperature and concentration on the three‐dimensional (3D) collagen hydrogels, we analyzed the structures in situ by Raman microspectroscopy. The increased intensity of the 814 and 936 cm^?1 Raman bands corresponding to the C—C stretch of a protein backbone and a shift in the amide III bands from 1241 cm^?1/1268 cm^?1 in controls to 1247 cm^?1/1283 cm^?1 in glyceraldehyde‐treated gels indicated changes to the alignment of the collagen molecules, fibrils/fibers and/or changes to the secondary structure on glyceraldehyde treatment. The increased intensity of 1450 cm^?1 band and the appearance of a strong peak at 1468 cm^?1 reflected a change in the motion of lysine/arginine CH₂ groups. For the EDC‐treated collagen hydrogels, the increased intensity of 823 cm^?1 peak corresponding to the C—C stretch of the protein backbone indicated that EDC also changed the packing of collagen molecules. The 23% decrease in the ratio of 1238 cm^?1 to 1271 cm^?1 amide III band intensities in the EDC‐modified samples compared with the controls indicated changes to the alignment of the collagen molecules/fibrils and/or the secondary structure. A change in the motion of lysine/arginine CH₂ groups was detected as well. The addition of NHS did not induce additional Raman shifts compared to the effect of EDC alone with the exception of a 1416 cm^?1 band corresponding to a COO^? stretch. Overall, the Raman spectra suggest that glyceraldehyde affects the collagen states within 3D hydrogels to a greater extent compared to EDC and the effects of temperature and concentration are minimal and/or not detectable. © 2012 Wiley Periodicals, Inc. Biopolymers 99: 349–356, 2013.     

Cell classification with low‐resolution Raman spectroscopy (LRRS)

The identification of individual eukaryotic and prokaryotic cells is the backbone of clinical pathology and provides crucial information about the genesis and progression of a disease. While most commonly fluorescent‐label based methods are applied, label‐free methods, such as Raman spectroscopy, are elegant alternatives. A major disadvantage of Raman spectroscopy is the low signal yield resulting in long acquisition times, making it impractical for high‐throughput clinical analysis. As a rule, Raman‐based cell identification relies on high‐resolution Raman spectra. This comes at a cost of detected Raman photons. In this letter we show that while the proper biochemical characterization of cells requires high‐resolution Raman spectra, the proper classification of cells does not. By varying the slit‐width between 50 µm and 500 µm it is possible to show that detected Raman signal from eukaryotic cells increased up to seven‐fold. Raman‐based cell classification was performed on three cancer cell lines: Jurkat, MiaPaca2, and Capan1, at three different resolutions 8 cm^–1, 24 cm^–1, and 48 cm^–1. Moreover, we have simulated the resolution decrease due to low‐diffraction gratings by binning neighboring pixels together. In both cases the cells were well classifiable using support vectors machine (SVM).

For anyone working in the field of Raman spectroscopy this picture of Sir C.V. Raman is recognizable, even with reduced spatial resolution. Raman spectra of eukaryotic cells can also be recognized even with six fold reduced spectral resolution.     

Polarized Raman spectrum of single crystal uridylyl (3′–5′) adenosine: Local Raman tensors of some functional groups

Polarized Raman scattering measurements have been made of a single crystal of uridylyl(3′–5′)adenosine (UpA) by the use of a Raman microscope with 488.0 nm excitation. The UpA crystal belongs to space group P2₁ (monoclinic), and Raman intensities I_aa, I_bb, and I_c′c′, have been determined for each Raman band. These intensities correspond to the aa, bb, and c′c′ components of the crystal Raman tensor, where c′ is defined as an axis perpendicular to the crystallographic a axis in the ac plane. From these experimental data, and by taking the known crystal structure into account, anisotropic and isotropic molecular Raman tensors have been calculated for the following 11 normal modes: ring stretching modes of the adenine residue (protonated) at 1560, 1516, 1330, and 715 cm⁻¹; ring stretching modes of the uracil residue at 1696, 1657, 1615, 1228, and 790 cm⁻¹; PO⁻₂ symmetric stretching mode at 1080 cm⁻¹; P(—)O single bond stretching mode at 801 cm₋₁. These pieces of information of the Raman tensors are considered to be useful for estimating the orientations of the DNA and RNA strands in a biological complex from a polarized Raman spectroscopic measurement of such a complex. © 1998 John Wiley & Sons, Inc. Biopoly 45: 135–147, 1998     

Real‐time monitoring of high‐gravity corn mash fermentation using in situ raman spectroscopy

In situ Raman spectroscopy was employed for real‐time monitoring of simultaneous saccharification and fermentation (SSF) of corn mash by an industrial strain of Saccharomyces cerevisiae. An accurate univariate calibration model for ethanol was developed based on the very strong 883 cm^?1 C–C stretching band. Multivariate partial least squares (PLS) calibration models for total starch, dextrins, maltotriose, maltose, glucose, and ethanol were developed using data from eight batch fermentations and validated using predictions for a separate batch. The starch, ethanol, and dextrins models showed significant prediction improvement when the calibration data were divided into separate high‐ and low‐concentration sets. Collinearity between the ethanol and starch models was avoided by excluding regions containing strong ethanol peaks from the starch model and, conversely, excluding regions containing strong saccharide peaks from the ethanol model. The two‐set calibration models for starch (R² = 0.998, percent error = 2.5%) and ethanol (R² = 0.999, percent error = 2.1%) provide more accurate predictions than any previously published spectroscopic models. Glucose, maltose, and maltotriose are modeled to accuracy comparable to previous work on less complex fermentation processes. Our results demonstrate that Raman spectroscopy is capable of real time in situ monitoring of a complex industrial biomass fermentation. To our knowledge, this is the first PLS‐based chemometric modeling of corn mash fermentation under typical industrial conditions, and the first Raman‐based monitoring of a fermentation process with glucose, oligosaccharides and polysaccharides present. Biotechnol. Bioeng. 2013; 110: 1654–1662. © 2013 Wiley Periodicals, Inc.     

Fourier transform infrared and Raman‐based biochemical profiling of different grades of pure foetal‐type hepatoblastoma

The biomolecular events resulting from the progression of hepatoblastoma remain to be elucidated. Fourier‐transform infrared (FTIR) and Raman spectroscopies are capable of noninvasively and accurately capturing the biochemical properties of biological tissue from its pathological status. Our aim was to probe critial biomolecular changes of liver accompanying the progression of pure foetal hepatoblastoma (PFH) by FTIR and Raman spectroscopies. Herein, biochemical alterations were both evident in the FTIR spectra (regions of 3100‐2800 cm^?1 and 1800‐900 cm^?1) and the Raman spectra (region of 1800‐400 cm^?1) among normal, borderline and malignant liver tissues. Compared with normal tissues, the ratios of protein‐to‐lipid, α‐helix‐to‐β‐sheet, RNA‐to‐DNA, CH3 methyl‐to‐CH2 methylene, glucose‐to‐phospholipids, and unsaturated‐to‐saturated lipids intensities were significantly higher in malignant tissues, while the ratios of RNA‐to‐Amide II, DNA‐to‐Amide II, glycogen‐to‐cholesterol and Amide I‐to‐Amide II intensities were remarkably lower. These biochemical alterations in the transition from normal to malignant have profound implications not only for cyto‐pathological classification but also for molecular understanding of PFH progression. The successive changes of the spectral characteristics have been shown to be consistent with the development of PFH, indicating that FTIR and Raman spectroscopies are excellent tools to interrogate the biochemical features of different grades of PFH.      

A quantitative bioapatite/collagen calibration method using Raman spectroscopy of bone

Numerous calibration models were developed and tested for the quantitative analysis of collagen and bioapatite in bone using Raman spectroscopy. The ν₁ phosphate vibration at 960 cm^–1 was used as indicator of the content of bioapatite while for collagen three markers were used: the C–H₂ band at 2940 cm^–1, the amide I band at 1667 cm^–1 and the vibrations of proline and hydroxyproline at 855 and 878 cm^–1, respectively. Also a calibration model based on the PLS algorithm was developed, too. Validation of the derived calibration models indicated that the model that makes use of the height ratio of the peaks 960/(855+878) exhibits the best accuracy. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Spectroscopic detection of β ‐sheet structure in nascent Aβ oligomers

Deep‐UV resonance Raman (UVRR) spectroscopy and circular dichroism (CD) were employed to study the secondary structure of Aβ(1–42) in fresh samples with increasing fractions of oligomeric peptide. A feature with a minimum at ～217 nm appeared in CD spectra of samples containing oligomeric Aβ(1–42). UVRR spectra more closely resembled those of disordered proteins. The primary difference between UVRR spectra was the ratio of the 1236 cm^–1 to 1260 cm^–1 amide III peak intensities, which shifted in favor of the 1236 cm^–1 band as the fraction of oligomeric peptide increased. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

The molecular interaction of a protein in highly concentrated solution investigated by Raman spectroscopy

We used Raman spectroscopy to investigate the structure and interactions of lysozyme molecules in solution over a wide range of concentrations (2.5–300 mg ml^?1). No changes in the amide‐I band were observed as the concentration was increased, but the width of the Trp band at 1555 cm^?1 and the ratios of the intensities of the Tyr bands at 856 and 837 cm^?1, the Trp bands at 870 and 877 cm^?1, and the bands at 2940 (CH stretching) and 3420 cm^?1 (OH stretching) changed as the concentration was changed. These results reveal that although the distance between lysozyme molecules changed by more than an order of magnitude over the tested concentration range, the secondary structure of the protein did not change. The changes in the molecular interactions occurred in a stepwise process as the order of magnitude of the distance between molecules changed. These results suggest that Raman bands can be used as markers to investigate the behavior of high‐concentration solutions of proteins and that the use of Raman spectroscopy will lead to progress in our understanding not only of the basic science of protein behavior under concentrated (i.e., crowded) conditions but also of practical processes involving proteins, such as in the field of biopharmaceuticals. © 2014 Wiley Periodicals, Inc. Biopolymers 103: 237–246, 2015.     

Characterisation of DNA methylation status using spectroscopy (mid‐IR versus Raman) with multivariate analysis

Methylation status plays important roles in the regulation of gene expression and significantly influences the dynamics, bending and flexibility of DNA. The aim of this study was to determine whether attenuated total reflection Fourier‐transform infrared (ATR‐FTIR) or Raman spectroscopy with subsequent multivariate analysis could determine methylation patterning in oligonucleotides variously containing 5‐methylcytosine, cytosine and guanine bases. Applied to Low‐E reflective glass slides, 10 independent spectral acquisitions were acquired per oligonucleotide sample. Resultant spectra were baseline‐corrected and vector normalised over the 1750 cm^–1–760 cm^–1 (for ATR‐FTIR spectroscopy) or the 1750 cm^–1–600 cm^–1 (for Raman spectroscopy) regions. Data were then analysed using principal component analysis (PCA) coupled with linear discriminant analysis (LDA). Exploiting this approach, biomolecular signatures enabling sensitive and specific discrimination of methylation patterning were derived. For DNA sequence and methylation analysis, this approach has the potential to be an important tool, especially when material is scarce. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Hen egg white lysozyme fibrillation: a deep‐UV resonance Raman spectroscopic study

Amyloid fibrils are associated with numerous degenerative diseases. The molecular mechanism of the structural transformation of native protein to the highly ordered cross‐β structure, the key feature of amyloid fibrils, is under active investigation. Conventional biophysical methods have limited application in addressing the problem because of the heterogeneous nature of the system. In this study, we demonstrated that deep‐UV resonance Raman (DUVRR) spectroscopy in combination with circular dichroism (CD) and intrinsic tryptophan fluorescence allowed for quantitative characterization of protein structural evolution at all stages of hen egg white lysozyme fibrillation in vitro. DUVRR spectroscopy was found to be complimentary to the far‐UV CD because it is (i) more sensitive to β ‐sheet than to α ‐helix, and (ii) capable of characterizing quantitatively inhomogeneous and highly light‐scattering samples. In addition, phenylalanine, a natural DUVRR spectroscopic biomarker of protein structural rearrangements, exhibited substantial changes in the Raman cross section of the 1000‐cm^–1 band at various stages of fibrillation. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

DFT study of structure and vibrational spectra of ceramide 3: comparison to experimental data

The Fourier transform Raman and infrared (IR) spectra of the Ceramide 3 (CER3) have been recorded in the regions 200–3500 cm^? 1 and 680–4000 cm^? 1, respectively. We have calculated the equilibrium geometry, harmonic vibrational wavenumbers, electrostatic potential surfaces, absolute Raman scattering activities and IR absorption intensities by the density functional theory with B3LYP functionals having extended basis set 6-311G. This work is undertaken to study the vibrational spectra of CER3 completely and to identify the various normal modes with better wavenumber accuracy. Good consistency is found between the calculated results and experimental data for the IR and Raman spectra.     

Towards the design of an optimal strategy for the production of ergosterol from Saccharomyces cerevisiae yeasts

The total yield of ergosterol produced by the fermentation of the yeast Saccharomyces cerevisiae depends on the final amount of yeast biomass and the ergosterol content in the cells. At the same time ergosterol purity—defined as percentage of ergosterol in the total sterols in the yeast—is equally important for efficient downstream processing. This study investigated the development of both the ergosterol content and ergosterol purity in different physiological (metabolic) states of the microorganism S. cerevisiae with the aim of reaching maximal ergosterol productivity. To expose the yeast culture to different physiological states during fermentation an on‐line inference of the current physiological state of the culture was used. The results achieved made it possible to design a new production strategy, which consists of two preferable metabolic states, oxidative‐fermentative growth on glucose followed by oxidative growth on glucose and ethanol simultaneously. Experimental application of this strategy achieved a value of the total efficiency of ergosterol production (defined as product of ergosterol yield coefficient and volumetric productivity), 103.84 × 10^?6 g L^?1h^?1, more than three times higher than with standard baker's yeast fed‐batch cultivations, which attained in average 32.14 × 10^?6 g L^?1h^?1. At the same time the final content of ergosterol in dry biomass was 2.43%, with a purity 86%. These results make the product obtained by the proposed control strategy suitable for effective down‐stream processing. © 2017 American Institute of Chemical Engineers Biotechnol. Prog., 33:838–848, 2017     

Understanding tissue specific compositions of bioenergy feedstocks through hyperspectral Raman imaging

Hyperspectral Raman imaging was used to study the tissue/cell type specific distribution of lignin and cellulose polymers within the plant cell walls. Distinct differences in cell wall compositions were identified between two potential bioenergy feedstocks: corn stover and Eucalyptus globulus. Characteristic bands of 627, 1,175, 1,206, and 1,428 cm⁻¹ were only observed for corn stover and 1,381 cm⁻¹ was only present in E. globulus. One‐dimensional and two‐dimensional chemical maps of lignin and cellulose were generated for the stem of corn stover, ranging from the epidermis to the pith area and revealed that lignin and cellulose abundance varies significantly among different cell types in the following order: sclerenchyma cells and tracheids (∼5 times) > epidermal cells (∼3 times) > bundle sheath cells > parenchyma cells. The Raman mapping methods developed on corn stover were also validated on E. globulus and clearly highlighted their difference in lignin composition. Biotechnol. Bioeng. 2011;108: 286–295. © 2010 Wiley Periodicals, Inc.     

A comparative Raman and CARS imaging study of colon tissue

An experimental evaluation of the information content of two complimentary techniques, linear Raman and coherent anti‐Stokes Raman scattering (CARS) microscopy, is presented. CARS is a nonlinear variant of Raman spectroscopy that enables rapid acquisition of images within seconds in combination with laser scanning microscopes. CARS images were recorded from thin colon tissue sections at 2850, 1660, 1450 and 1000 cm^–1 and compared with Raman images. Raman images were obtained from univariate and multivariate (k‐means clustering) methods, whereas all CARS images represent univariate results. Variances within tissue sections could be visualized in chemical maps of CARS and Raman images. However, identification of tissue types and characterization of variances between different tissue sections were only possible by analysis of cluster mean spectra, obtained from k‐means cluster analysis. This first comparison establishes the foundation for further development of the CARS technology to assess tissue. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Atomic Fe‐Doped MOF‐Derived Carbon Polyhedrons with High Active‐Center Density and Ultra‐High Performance toward PEM Fuel Cells

A metalorganic gaseous doping approach for constructing nitrogen‐doped carbon polyhedron catalysts embedded with single Fe atoms is reported. The resulting catalysts are characterized using scanning transmission electron microscopy, X‐ray photoelectron spectroscopy, and X‐ray absorption spectroscopy; for the optimal sample, calculated densities of Fe–N_x sites and active N sites reach 1.75812 × 10¹³ and 1.93693 × 10¹⁴ sites cm^‐2, respectively. Its oxygen reduction reaction half‐wave potential (0.864 V) is 50 mV higher than that of 20 wt% Pt/C catalyst in an alkaline medium and comparable to the latter (0.78 V vs 0.84 V) in an acidic medium, along with outstanding durability. More importantly, when used as a hydrogen–oxygen polymer electrolyte membrane fuel cell (PEMFC) cathode catalyst with a catalyst loading as low as 1 mg cm^‐2 (compared with a conventional loading of 4 mg cm^‐2), it exhibits a current density of 1100 mA cm^‐2 at 0.6 V and 637 mA cm^‐2 at 0.7 V, with a power density of 775 mW cm^‐2, or 0.775 kW g^–1 of catalyst. In a hydrogen–air PEMFC, current density reaches 650 mA cm^‐2 at 0.6 V and 350 mA cm^‐2 at 0.7 V, and the maximum power density is 463 mW cm^‐2, which makes it a promising candidate for cathode catalyst toward high‐performance PEMFCs.     

Photodamage to Pigment in the Photosystem Ⅱ Reaction Center D1/D2/Cytochrome b559 Complex

Strong light （800μmol photons/m^2 per s）-induced bleaching of the pigment in the isolated photosystem Ⅱ reaction center （PSII RC） under aerobic conditions （in the absence of electron donors or acceptors） was studied using high-pressure liquid chromatography （HPLC）, absorption spectra, 77K fluorescence spectra and resonance Raman spectra. Changes in pigment composition of the PSII RC as determined by HPLC after light treatment were as follows： with Increasing illumination time chlorophyll （Chl） a and β-carotene （β-car） content decreased. However, decreases in pheophytin （Pheo） could not be observed because of the mixture of the Pheo formed by degraded chlorophyll possibly. On the basis of absorption spectra, it was determined that, with a short time of illuminatlon, the initial bleaching occurred maximally at 680 nm but that with Increasing Illumination time there was a blue shift to 678 nm. It was suggested that P680 was destroyed Initially, followed by the accessory chlorophyll. The activity of P680 was almost lost after 10 mln light treatment. Moreover, the bleaching of Pheo and β-car was observed at the beginning of illumination. After Illumination, the fluorescence emission Intensity changed and the fluorescence maximum blue shifted, showing that energy transfer was disturbed. Resonance Raman spectra of the PSII RC excited at 488.0 and 514.5 nm showed four main bands, peaking at 1 527 cm^-1 （υ101）, 1 159 cm^-1 （υ2）, 1 006 cm^-1 （υ3）, 966 cm^-1 （υ4） for 488.0 nm excitation and 1 525 cm^-1 （υ1）, 1 159 cm^-1 （υ2）, 1 007 cm^-1 （υ3）, 968 cm^-1 （υ4） for 514.5 nm excitation. It was confirmed that two spectroscopically different β-car molecules exist In the PSII RC. After light treatment for 20 mln, band positions and bandwidths were unchanged. This indicates that carotenoid configuration Is not the parameter that regulates photoprotectlon in the PSII RC.     

Quantitative conformational analysis of cytochromec bound to phospholipid vesicles studied by resonance Raman spectroscopy

Resonance Raman spectra have been recorded from ferri-cytochromec bound to phospholipid vesicles composed of dimyristoyl phosphatidylglycerol (DMPG), dioleoyl phosphatidylglycerol (DOPG) or dioleoyl phosphatidylglycerol-dioleoyl phasphatidylcholine (DOPG-OPC) (70 : 30 mole/mole). Lipid binding induces very significant conformational changes in the protein molecule. The resonance Raman spectra differ in their content of bands originating from two different conformational species, I and II, of the protein, and from two different spin and coordination states of the heme in conformation II. Data of sufficiently high precision were obtained that the spectra of the individual species could be quantitated by a constraint interative fitting routine using single Lorentzian profiles. In the high frequency, or marker band region (1200 to 1700 cm⁻¹), the frequencies, half widths and relative intensities of the individual bands could be estimated from previous surface enhanced resonance Raman measurements on cytochromec adsorbed on a silver electrode. These were then further optimized to yield both the spectral parameters and relative contents of the different species. In the low frequency, or finger-print, region (200 to 800 cm⁻¹), the spectral parameters of the individual species were obtained from difference spectra derived by sequential subtraction between the spectra of ferri-cytochromec in the three different lipid systems, using the relative proportions of the species derived from the marker band region. These parameters were then subsequently refined by iterative optimization. The optimized spectral parameters in both frequency regions for the six-coordinated low spin states I and II, and for the five-coordinated high spin state II are presented. The proportion of state II, in which hence the heme crevice assumes an open structure, and of the five-coordinated high spin configuration, is found to increase on binding ferri cytochromec to negatively charged lipid vesicles. The extent of this conformational change increases in the order: DOPG-DOPC<DOPG<DMPG, with a parallel decrease of the proportion of the conformational state I, whose structure is similar to that of the uncomplexed ferri-cytochrome c in solution. Similar conformational changes are found for ferro-cytochromec compared to those obtained with the oxidized species on binding to lipids. The present work is essential for studies which seek to analyze, in any detailed fashion, the conformational transitions in the heme protein which take place in response to changes in the lipid environment.