Raman Spectroscopy Analysis of the Biochemical Characteristics of Molecules Associated with the Malignant Transformation of Gastric Mucosa

Objective

The purpose of this study was to comparatively analyze the signature Raman spectra of genomic DNA, nuclei, and tissue of normal gastric mucosa and gastric cancer and to investigate the biochemical transformation of molecules associated with gastric mucosa malignancy.

Method

Genomic DNA, nuclei, and tissue from normal gastric mucosa and gastric cancer were analyzed by Raman spectroscopy.

Results

1) The Raman spectrum of gastric cancer genomic DNA showed that two peaks appeared, one at approximately 1090 cm^-1 with a higher intensity than the peak at 1050 cm^-1 in the spectrum. Characteristic peaks appeared at 950 cm^-1, 1010 cm^-1, and 1100-1600 cm^-1. 2) Using a hematoxylin and eosin (H&E)-stained section, the intensity of the characteristic peak of nucleic acids at 1085 cm^-1 was increased and shifted to 1088 cm^-1 in cancer cells. The relative intensity of the characteristic peaks of nucleoproteins at 755 cm^-1 and 1607 cm^-1 was significantly increased in cancer cells compared with normal cells. 3) Compared with normal tissues, the peak representing PO^2- symmetric stretching vibration shifted from 1088 cm^-1 to 1083 cm^-1 in cancer tissue, and the characteristic peak for collagen at 938 cm^-1 shifted to 944 cm^-1. In addition, an extra characteristic peak indicating C = C stretching vibration appeared at 1379 cm^-1 in the lipid spectrum in cancer tissue.

Conclusions

The position, intensity, and shape of peaks in the Raman spectra of DNA, nuclei, and tissue from gastric cancer were significantly different compared with those of normal cells. These results indicate that the DNA phosphate backbone becomes unstable in cancer cells and might be broken; the relative content of histones is increased and stable; the relative collagen content is reduced, facilitating cancer cell metastasis; and the relative content of unsaturated fatty acids is increased, increasing the mobility of the plasma membrane of cancer cells.     

Infrared absorption and raman scattering of sulfate groups of heparin and related glycosaminoglycans in aqueous solution

The i.r. spectra for aqueous solutions of sulfated glycosaminoglycans and model compounds in the transmittance “window” region of the solvent (1400-950 cm^?1) are dominated by the strong and complex absorption centered at ～1230 cm^?1 and associated with the antisymmetric stretching vibrations of the SO groups. Primary and secondary O-sulfate groups absorb at somewhat higher frequencies (1260-1200 cm^?1) than N-sulfates (～1185 cm^?1). Each sulfate band lends itself to quantitative applications, especially within a given class of sulfated polysaccharide. Laser-Raman spectra of heparin and model compounds have been obtained in aqueous solution and in the solid state. The most-prominent Raman peak (at ～1060 cm^?1) is attributable to the symmetrical vibration of the SO groups, with N-sulfates emitting at somewhat lower frequencies (～1040 cm^?1) than O-sulfates. The Raman pattern in the 950-800 cm^?1 region (currently used in the i.r. for distinguishing between types of sulfate groups) also involves vibrations that are not localized only in the COS bonds.     

A Raman spectroscopic study on 5′-rGMP gel and self-aggregate

In order to analyze the melting behavior of 5′-rGMP gel at acidic pH and self-aggregate near neutral pH we have obtained Raman spectra of aqueous solutions of 5′-rGMP at various temperatures. At low temperature the intensities of Raman peaks at 502, 585, 1083, 1179, 1322, 1366, 1487, and 1578 cm^?1 decrease due to the formation of ordered structure (Raman hypochromism). In contrast, the peaks at 671, 725, 813, and 1338 cm^?1 become stronger at low temperature (Raman hyperchromism). The Raman hyperchromism of the 671- and 813-cm^?1 peaks have been explained in terms of detailed structural models. Recently, the 668- and 682-cm^?1 peaks in the Raman spectrum of aqueous 5′-rGMP solution have been attributed to the guanine ring breathing vibrations in C3′- and C2′-endo conformers [Benevides, J. B., Lemur, D. & Thomas, G. J., Jr. (1984) Biopolymers 23 , 1011–1024]. On the basis of this information our Raman data can be interpreted to suggest that the continuous helix model of 5′-rGMP gel is right-handed. The 1487-cm^?1 peak intensity has been used to monitor the melting profies at several pHs. Near neutral pH the melting profile shows a single transition, whereas at acidic pH it shows two transitions. From these observations we propose possible pathways for the melting of 5′-rGMP gel formed at acidic pH and self-aggregate formed near neutral pH.     

Intensity Changes of Base and Backbone Raman Modes in the B to Z Transition of poly(dG-dm5C)

Abstract

Raman spectroscopy was employed to investigate the temperature-induced B to Z transition of poly(dG-dm-⁵C). The transition midpoint was about 37°C for a solvent containing 20 mM Mg²⁺. A 10-fold change in Mg²⁺ concentration altered the transition midpoint by at least 60°C. Raman spectra of the B and Z forms of poly(dG-dm⁵C) exhibited characteristics similar to those observed with poly(dG-dC). The 682 cm^?1 guanine mode and 835 cm^?1 backbone mode were present in the B conformation. In the Z form the intensities of these two bands decrease substantially and new peaks were observed at 621 cm^?1, 805 and 819 cm¹. Several bands unique to poly(dG-dm⁵C) were also observed. Transition profiles of band intensity vs. temperature were determined for fourteen Raman bands. The curves of all of the base vibrations and one backbone mode had the same slope and midpoint. This indicates that conformational changes in the guanine and methycytosine bases occur concurrently.     

Raman spectral changes induced by side-chain interactions in racemic poly-gamma-benzyl glutamate

Laser Raman spectra are reported for solid films cast from a series of solutions containing mixtures of right- and left-handed α-helices of poly-γ-benzyl-L - and D -glutamate. Procedures were established for producing spectra that were reproducible in position to ±0.3 cm^?1 and in relative intensity to a few percent for features of interest. Spectra for the pure L and pure D polymers were identical, as expected. Several small but definite spectral changes appear in the mixtures, reaching a maximum for the racemic 50:50 mixture. The changes are a shift of ?1.4 cm^?1 in the amide I peak at 1650.5 cm^?1; a shift of about ?5 cm^?1 in the partially resolved amide III peak at 1291 cm^?1; a shift of +2.5 cm^?1 in the benzyl peak at 3062.5 cm^?1; changes in relative intensity of as much as 50% in several regions; and the marked enhancement of several peaks, particularly that at 254 cm^?1. These changes are discussed in terms of side-chain interactions in the packing of right- and left-handed helices.     

Direct discrimination of different plant populations and study on temperature effects by Fourier transform infrared spectroscopy

Fourier transform infrared spectroscopy was used to characterise highland and lowland populations of Polygonum minus Huds. grown in different controlled environments. A thermal perturbation technique of two-dimensional correlation infrared spectroscopy (2D-IR) correlation spectra was applied to establish differences between the populations. The absorption peaks at 3,480 cm^?1 (hydroxyl group), 2,927 cm^?1 (methyl group), 1,623 cm^?1 (carbonyl group), and 1,068 cm^?1 (C–O group) were particularly powerful in separating the populations. These peaks, which indicate the presence of carbohydrate, terpenes, amide and flavonoids were more intense for the highland populations than lowland populations, and increased in environments with a higher temperature. Wavenumbers (1,634, 669 cm^?1) and (1,634, 1,555 cm^?1) in the 2D-IR correlation spectra provided fingerprint signals to differentiate plants grown at different temperatures. This study demonstrates that IR fingerprinting, which combines mid-IR spectra and 2D-IR correlation spectra, can directly discriminate different populations of P. minus and the effects of temperature.     

Studies on determining conformational order in n-alkanes and phospholipids from the 1130 cm−1 raman band

Conformational disorder in lipid bilayer systems is commonly measured with reference to the intensity of the 1130 cm^?1 Raman band. However, estimates of the concentration of gauche bonds may vary by a factor of six according to the model used to relate intensity and concentration. In an effort to narrow the wide range in these estimates, we have measured the intensity of the 1130 cm^?1 band of crystalline n-C₂₁H₄₄ in its orthorhombic and hexagonal phases. On transition to the hexagonal phase, the intensity of the 1130 cm^?1 band is much reduced. It is assumed that the observed intensity reduction results from the introduction of gauche bonds whose number can be independently estimated from other features in the Raman and infrared spectra. From these measurements we conclude that the intensity of the 1130 cm^?1 band is not linearly related to the concentration of gauche bonds and that a disproportionately large decrease in the 1130 cm^?1 band intensity results from the introduction of a low concentration of gauche bonds. Thus previous estimates of gauche bond concentrations based on the assumption of a linear relation have tended to greatly overestimate the gauche bond concentration. These results derived from experiment are in accord with those of Pink et al. (Pink, D.A., Green, T.J. and Chapman, D. (1980) Biochemistry 19, 349–356) derived from theory.     

Infrared and raman studies of the methyl cis undecenoates and of the methyl undecynoates

The infrared spectra (of CCl₄ solutions) and the Raman spectra (of the neat liquids) of the eight isomeric methyl cis-undecenoates, of methyl undec-10-enoate, and of the nine isomeric methyl undecynoates have been obtained. Conjugation of the double bond with the carbonyl group lowers the wavenumber value of ν(CC) by 8 cm^?1 from the mean value of 1657 cm^?1. Conjugation of the triple bond with the carbonyl group gives rise to a single Raman band due to ν(CC) at 2241 cm^?1 whereas the non-conjugated, non-terminal triple bond gives a Fermi resonance doublet at 2234 and 2293 cm^?1.     

Resonance raman spectroscopy of iron (3)--ovotransferrin and iron (3)--human serum transferrin

We report the resonance Raman spectra in the frequency range 300–1800 cm^?1 of Fe (III)-ovotransferrin and Fe (III)-human serum transferrin in aqueous solution at about 10^?4M protein concentration. This is the first observation of resonance Raman scattering ascribable to amino acid ligand vibrational modes of a nonheme iron protein. The resonance Raman spectra of the transferrins are similar except that the resonance band near 1270 cm^?1 is shifted to a higher frequency for Fe(III)-human serum transferrin than that for Fe(III)-ovotransferrin. The resonance Raman bands observed near 1170, 1270, 1500 and 1600 cm^?1 may reflect resonance enhancement of p-hydroxy-phenyl frequencies of tyrosine residues and/or imidazolium frequencies of histidine residues.     

Laser Raman scattering of cobramine B, a basic protein from cobra venom

Cobramine B, a small basic protein from cobra venom, is selected as a model for studying the scattering intensity of tyrosyl ring vibrations in the Raman spectra of proteins. All three tyrosines in this protein appear to be “buried” in the interior of the molecule and probably involved in interactions which are similar to those of the three “buried” tyrosines in RNase A when it is dissolved in water. Spectral evidence is presented and discussed. The Raman spectra in the 300–1800 cm^?1 region of cobramine B in the solid and solution are compared quantitatively. Several differences exist between the two spectra and may be interpreted in terms of difference in conformation. In the amide I region, a strong single line was observed at 1672 cm^?1 both in the solid and solution spectra, suggesting that this protein may contain a large fraction of antiparallel-β structure. This is supported by the presence of a line at 1235 cm^?1 in the amide III region, which is also characteristic of β-structure. The resolved peaks at 1254 and 1270 cm^?1 indicate the coexistence of some hydrogen-bonded random-coil and some α-helix with the β-structure.     

Dichroism of the Infrared Spectrum of Nerve

Infrared spectra were obtained from the sciatic and optic nerves of the frog (Rana sp.) and the trigeminal and olfactory nerves of the garfish (Lepisosteus osseus). The myelinated nerves showed dichroism at several absorption peaks, particularly 1,220-1,230 cm^-1, but the nonmyelinated nerves showed little or no dichroism. The dichroic peaks indicate that in myelinated nerve, there is an ordered arrangement of protein and lipid molecules which was not found in nonmyelinated nerve.     

Raman intensities of carbon-carbon stretching modes in a model membrane

Laser-Raman spectra of L-α-dimyristoylphosphatidylcholine (DMPC) liposomes in the spectral range 1000–1200 cm^?1 were obtained as a function of temperature from ?80 to +50°C. The triplet found in this spectral region was resolved into Lorentzian components by means of an iterative computer program. The peak intensities, band widths, and band areas of the resolved 1062 cm^?1 and 1130 cm^?1 bands, assigned to CC stretching vibrations of trans segments, were evaluated as a function of temperature. While the peak intensities of the bands decrease substantially with temperature, the band widths show a considerable increase. The change in band areas is therefore smaller than the change in peak heights. Experiments with all trans carboxylic acids showed that in these compounds the area of the Raman bands at 1062 cm^?1 and 1130 cm^?1 is proportional to the number of trans bonds. The variation with temperature of the number of trans and gauche bonds in the studied phospholipid is reflected by the change of the area of the 1130 cm^?1 Raman band.     

Exploration of polyacrylamide microplastics and evaluation of their toxicity on multiple parameters of Oreochromis niloticus

Due to the increased production of polyacrylamide microplastics in the environment impacting the adverse effects on aquatic organisms have become a global concern. The present study aimed to evaluate the toxicity of different concentrations (0.018, 0.03 0.09 g/1) of polyacrylamide microplastics on Oreochromis niloticus. Polyacrylamide microplastics were characterized by Fourier transform infrared and Raman spectroscopy. The FTIR technique revealed the spherical morphology and size range of polyacrylamide (0.1–0.4 mm) with 99 % purity. Raman Spectroscopy results showed peaks around (1100 cm^?1 and 1650 cm^?1) in gills, these peaks confirmed the presence of polyacrylamide microplastics in the gills of Oreochromis niloticus. Polyacrylamide microplastics significantly shortened the antioxidant enzymes (Catalase and Reduced glutathione) proceedings and the increase was observed in Malondialdehyde and Lipid peroxide levels in high-dose treated groups. Moreover, total protein contents were expressively increased, while other blood parameters (AST, ALP, ALT) were significantly decreased. Hemoglobin (g/dl), Erythrocyte (106/µl) and TLC (1x10⁹/l) levels were reduced significantly (p < 0.05) in high concentrations. The administration of polyacrylamide microplastics induced different histological changes in the gills, liver and intestine of O. niloticus. It was concluded that polyacrylamide microplastics are toxic agents having harmful effects on fish health.     

Determination of Glucose Concentration in Whole Blood using Fourier-Transform Infrared Spectroscopy

Fourier-transform infrared(FTIR) transmission spectroscopy has beenused for the determination of glucoseconcentrations in whole blood samples fromtwenty-eight patients. A four-vectorpartial least squares calibration model,using the spectral range 950–1200 cm^-1,yielded a standard error of prediction of0.59 mM for an independent test set. Forblood samples from a single patient, wefound that the glucose concentration wasproportional to the difference between thevalues of the second derivative spectrum at1082 cm^-1 and 1093 cm^-1, suggestingthat these two specific wavelengths can beused for determining glucose concentrationsin blood.     

Internal DNA Modes Below 25 cm−1: A Resonance Raman Spectroscopy Observation

Abstract

The first resonance Raman scattering observation of the low-frequency (LF) region (below 40 up to 12 cm^?1) of DNA motions is presented. Since the concentration of the studied DNA solution was very low (1 mg/ml), the spectra features reflect internal vibrations of the macro-molecule. The decomposition of the spectra into Lorentzians clearly indicate three intrahelical DNA modes: the corresponding peaks are located at the frequencies 16,19, and 23 (±1) cm^?1. This result is in agreement with our quasi-continuity model of the LF B-form DNA dynamics (V. Lisy, P. Miskovsky and P. Schreiber, J. Biomol. Struct. Dyn. 13, 707 (1996)). The fit of the experimental frequencies to the theory, using the Genetic Algorithms approach, allowed us to make some conclusions about the model force constants which could be found by independent conformational energy calculations. Possible positions of five lowest-frequency DNA peaks, predicted by the model, are discussed.     

Laser-raman spectroscopic study of carbohydrates: 1-thio-β-d-hexopyranosides

Some β-d-hexopyranosides of 1-thio-d-glucose, 2-acetamido-2-deoxy-1-thio-d-glucose, and 1-thio-d-galactose were examined by laser-Raman spectroscopy. An anomeric CH bending vibration was found at 891 ± 7 cm^-1 for all compounds investigated; thus, the anomers of these sugars can be differentiated by Raman spectroscopy. The N-acetyl group and carboxyl group can also be detected by Raman spectroscopy. Unlike protein samples, the carbohydrates in aqueous solution yield less useful information from Raman spectra than in the solid state; this is due to the extensive overlapping of carbohydrate OH bands with water OH bands.     

Application of "in vivo cryotechnique" to detect erythrocyte oxygen saturation in frozen mouse tissues with confocal Raman cryomicroscopy

To measure oxygen saturation (SO₂) of flowing erythrocytes in blood vessels of living animals, our “in vivo cryotechnique” (IVCT) was combined with confocal Raman microscopy at low temperature (−150 °C), referred to as cryomicroscopy. We evaluated two resonance Raman (RR) shifts around 1355 and 1378 cm⁻¹, reflecting de-oxygenated and oxygenated hemoglobin molecular structures, respectively. Judging from the calibration analyses of quickly frozen human whole blood for the control experiment in vitro, the two RR shifts were well retained at the low temperature, and their calculated ratios mostly reflected the relative SO₂ measured with a blood-gas analyzer. In blood vessels of living mouse organs prepared with the IVCT, their RR spectral peaks were also detected at the same RR shifts obtained in human blood. In the blood vessels of living mouse small intestines, some arterioles and venules were clearly distinguishable by monitoring different peak patterns of their RR shifts. The different ratios of the RR shift-areas were calculated even in the arterial vessels. In blood vessels of mouse livers, the Raman spectra showed a lower peak shift of 1378 cm⁻¹ compared to that of 1355 cm⁻¹, indicating an SO₂ decrease in hepatic blood circulation. Thus, the new cryopreparation technique will enable us to directly analyze the in vivo SO₂ in various tissues of a whole animal body prepared with the IVCT, reflecting their living states.     

Raman Spectroscopy Analysis of Botryococcene Hydrocarbons from the Green Microalga Botryococcus braunii

Botryococcus braunii, B race is a unique green microalga that produces large amounts of liquid hydrocarbons known as botryococcenes that can be used as a fuel for internal combustion engines. The simplest botryococcene (C₃₀) is metabolized by methylation to give intermediates of C₃₁, C₃₂, C₃₃, and C₃₄, with C₃₄ being the predominant botryococcene in some strains. In the present work we have used Raman spectroscopy to characterize the structure of botryococcenes in an attempt to identify and localize botryococcenes within B. braunii cells. The spectral region from 1600–1700 cm⁻¹ showed ν(C=C) stretching bands specific for botryococcenes. Distinct botryococcene Raman bands at 1640 and 1647 cm⁻¹ were assigned to the stretching of the C=C bond in the botryococcene branch and the exomethylene C=C bonds produced by the methylations, respectively. A Raman band at 1670 cm⁻¹ was assigned to the backbone C=C bond stretching. Density function theory calculations were used to determine the Raman spectra of all botryococcenes to compare computed theoretical values with those observed. The analysis showed that the ν(C=C) stretching bands at 1647 and 1670 cm⁻¹ are actually composed of several closely spaced bands arising from the six individual C=C bonds in the molecule. We also used confocal Raman microspectroscopy to map the presence and location of methylated botryococcenes within a colony of B. braunii cells based on the methylation-specific 1647 cm⁻¹ botryococcene Raman shift.     

Raman resonance studies of functional fragments of helix pomatia βC-haemocyanin

Resonance Raman spectra were recorded for tenth molecules of β_C-haemocyanin of Helix pomatia, for a limited tryptic hydrolysate, and for the five isolated fragments.On excitation at 514.5 nm the intensity of the peroxide stretching vibration was preserved in the fragments. Domain h showed a frequency of 741 cm^?1 in contrast to 745–747 cm^?1 for the other fragments.On excitation at 457.9 nm the intensity of the Cu-N vibration at 270 cm^?1 was lowered on partial trypsinolysis, suggesting a less symmetrical arrangement of the ligands of Cu in the fragments.     

Preparation and characterization of oxochromium(IV) and nickel(II) complexes with 5,14-dihydro-7,16-diethyl-(E)- or -(Z)-dipyrido[b,i][1,4,8,11]tetraazacyclotetradecine

The reaction of 5,14-dihydro-7,16-diethyl-(E) or -(Z)-dipyrido[b,i][1,4,8,11]tetraazacyclotetradecine with chromium hexacarbonyl produced the corresponding oxochromium(IV) complexes. These compounds had intense bands in the infrared region at 985 cm⁻¹, which are attributed to the CrO stretching modes. The two complexes gave mass spectra with prominent parent and parent-O peaks. On the other hand the mass spectra for the nickel(II) complexes showed parent and parent-CH₃ peaks. The absorption bands appearing in the energy range greater than 19 000 cm⁻¹ were attributable to the π→π* and CT transitions. Consistent with their diamagnetism, the oxochromium complexes gave well-resolved proton NMR and carbon-13 NMR spectra. The magnitude of downfield shifts for the oxochromium(IV) complex is much larger than that observed for the corresponding nickel(II) complex. This is due to the fact that the positive charge provided by chromium(IV) is greater in magnitude than that by nickel(II).