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Raman microprobe

Raman Microspectroscopy. Raman spectra of small soflds or small regions of soflds can be obtained at a spatial resolution of about 1 p.m usiag a Raman microprobe. A widespread appHcation is ia the characterization of materials. For example, the Raman microprobe is used to measure lattice strain ia semiconductors (30) and polymers (31,32), and to identify graphitic regions ia diamond films (33). The microprobe has long been employed to identify fluid iaclusions ia minerals (34), and is iacreasiagly popular for identification of iaclusions ia glass (qv) (35). [Pg.212]

Fig. 6. Schematic diagram of a Raman microprobe where BS = beam splitter, L = lens, and MI = mirror, (a) The illumination pathway (b) the collection... Fig. 6. Schematic diagram of a Raman microprobe where BS = beam splitter, L = lens, and MI = mirror, (a) The illumination pathway (b) the collection...
A principal advantage of the Raman microprobe is that the optics are those of a conventional light microscope a wide variety of special-purpose objectives developed for materials and biological microscopy are available. The Raman microprobe also offers the advantage of fluorescence reduction owing to the high spatial resolution of the microscope if a region of low fluorescence can be chosen for observation. [Pg.213]

The spatial resolution of the Raman microprobe is about an order of magnitude better than that obtainable using an infrared microscope. Measurement times, typically of a few seconds, are the same as for other Raman spectrographs. To avoid burning samples, low (5—50-mW) power lasers are employed. [Pg.213]

Fig. 7. Raman microprobe spectra of (a) polystyrene [9003-33-6], (b) low density polyethylene, and (c) polycarbonate [24936-68-3]. Fig. 7. Raman microprobe spectra of (a) polystyrene [9003-33-6], (b) low density polyethylene, and (c) polycarbonate [24936-68-3].
Laser Raman Microprobe. A more sophisticated microscope is the Laser Raman Microprobe, sometimes referred to as MOLE (the molecular orbital laser examiner). This instmment is designed around a light microscope to yield a Raman spectmm (45) on selected areas or particles, often <1 ia volume. The data are related, at least distantly, to iafrared absorption, siace the difference between the frequency of the exciting laser and the observed Raman frequency is the frequency of one of the IR absorption peaks. Both, however, result from rotational and vibrational states. Unfortunately, strong IR absorption bands are weak Raman scatterers and vice versa hence there is no exact correspondence between the two. [Pg.335]

Sample preparation is straightforward for a scattering process such as Raman spectroscopy. Sample containers can be of glass or quartz, which are weak Raman scatterers, and aqueous solutions pose no problems. Raman microprobes have a spatial resolution of - 1 //m, much better than the diffraction limit imposed on ir microscopes (213). Eiber-optic probes can be used in process monitoring (214). [Pg.318]

We will confine ourselves to those applications concerned with chemical analysis, although the Raman microprobe also enables the stress and strain imposed in a sample to be examined. Externally applied stress-induced changes in intramolecular distances of the lattice structures are reflected in changes in the Raman spectrum, so that the technique may be used, for example, to study the local stresses and strains in polymer fibre and ceramic fibre composite materials. [Pg.54]

Inorganic Compounds. The Raman microprobe has been used by Berg and Kerridge (2000) to obtain computer mappings of the structures of salt eutectics solidified from their melts. In contrast to metallic eutectics, which commonly occur... [Pg.54]

Guineau, B. (1989), Nondestructive analysis of organic pigments and dyes using raman microprobe, microfluorimeter and absorption microspectrophotometer, Stud. Conserv. 34, 38-AA. [Pg.581]

Optical examination of etched polished surfaces or small particles can often identify compounds or different minerals hy shape, color, optical properties, and the response to various etching attempts. A semi-quantitative elemental analysis can he used for elements with atomic number greater than four by SEM equipped with X-ray fluorescence and various electron detectors. The electron probe microanalyzer and Auer microprobe also provide elemental analysis of small areas. The secondary ion mass spectroscope, laser microprobe mass analyzer, and Raman microprobe analyzer can identify elements, compounds, and molecules. Electron diffraction patterns can be obtained with the TEM to determine which crystalline compounds are present. Ferrography is used for the identification of wear particles in lubricating oils. [Pg.169]

Thomas R. (2000) Determination of water contents of granite melt inclusions by confocal laser Raman microprobe spectroscopy. Am. Mineral. 85, 868-872. [Pg.616]

There are also several papers describing adsorption of quinoline. Sawamoto [143] have studied adsorption and reorientation of quinoline molecules at Hg electrodes by recording differential capacity-potential and differential capacity-time plots using the flow-injection method. Adsorption of quinoline was found reversible at any potential, with the possibility of reorientation of the molecules at the interface. Ozeld etal. [144] have studied adsorption, condensation, orientation, and reduction of quinoline molecules at pure Hg electrode from neutral and alkaline solutions, applying electrochemistry and Raman microprobe spectroscopy. The adsorbed quinoline molecules changed their orientation from the flat at —0.1 V > E > —0.3 V, to the upright at < —0.5 V. At potentials —0.3 V > > —0.5 V, both orientations were observed. Later, Ozeld et al. [145] have extended the studies on reorientation of quinolinium ions at the Hglacidic aqueous solution interface. For these conditions, the specific adsorption of quinoline was not observed. [Pg.978]

The dentin-adhesive interface has been studied using a Raman microprobe technique [199], which shows the formation of resin-reinforced dentin and the penetration of resin into dentin substrate to a depth of 5-6 microns. Further study of the interface showed that only small molecules such as MMA, 4-MET (hydrolyzed 4-META) or oligomers infiltrated the dentin, and that all of the resin in the dentin originated from the monomer solution [200]. SEM and TEM studies of the ultrastructure of the resin-dentin interdiffusion zone showed a 2 micron zone with closely packed collagen fibrils running parallel to the interface [201]. [Pg.20]

Raman Spectroscopy Detecting forged medieval manuscripts (Anal. Chem. 2002, 74, 3658-3661. "Analysis of Pigmentary Materials on the Vinland Map and Tartar Relation by Raman Microprobe Spectroscopy")... [Pg.261]

Aerosol Heterogeneity. The variation of the chemical composition from particle to particle within an aerosol size class has been probed in a number of ways. Single-particle chemical analysis has been achieved by using the laser Raman microprobe (25) and analytical scanning electron microscopy (26). With the electron microscope techniques, the particle can be sized as well as analyzed chemically, so the need for classification prior to sample collection is reduced. Analyzing hundreds to thousands of particles provides the information necessary to track the particles back to their different sources but is extremely time consuming. [Pg.205]

Since its development by Delhaye and Dhamelincourt in 1975 [1] the epi-illumination Raman microprobe has become one of the most important input systems in Raman spectroscopy and is the instrument around which most Raman imaging systems are constructed. Epi-illumination instruments are almost always constructed around research-grade commercially available fluorescence microscope frames, with input optics modified to accept an exciting laser and with output optics modified to direct backscattered Raman signal to a spectrograph. [Pg.98]

It should be noted that the transmission of the acousto-optic filter is only about 50%, while the transmission of the liquid crystal filter is about 20-40%. By contrast, a dielectric filter passes 80-90% of the incident light. The differences arise because both the AOTF and LCTF operate on linearly polarized light. In most Raman microprobes, both polarization components of the Raman scatter are collected, even when the exciting laser is linearly polarized. [Pg.100]

The effect of highly localized loading on the surface of yttria-stabilized zirconia ceramic was investigated by polarized Raman microprobe spectroscopy. Figure 17.2a-d shows a micrograph of an indentation print, a map of... [Pg.409]

Two retrieved cross-linked UHMWPE acetabular cups were preliminary investigated by Raman microprobe spectroscopy with respect to their oxidation... [Pg.410]

The Laser Raman microprobe constitutes a physical method of microanalysis based on the vibration spectra characteristic of polyatomic structures. A focused laser beam excites the sample. The light diffused by the Raman effect is used for identification and localisation of the molecular constituents present in the sample. An optical microscope allows a survey of the interesting structures and the placing of the laser beam. The spectra obtained from fossil organic particles generally match well the corresponding IR-spectra, but the features in particular yield additional information, which will be discussed below with the given examples (Fig. 23, p. 36). [Pg.13]

A few wood sections were delignified using the acid chlorite method [14] (sample 2). In order to obtain sample 3, a 1.6-jxm spot in the S2 cell wall of a cross section was laser-delignified (514.5-nm line) by exposing it in a Raman microprobe experiment [15]. In our laboratory, it has been observed that the... [Pg.28]


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Applications of the Raman Microprobe

Laser Raman microprobe

Microprobe

Microprobes

Raman Laser Microprobe Microscopy

Raman Microprobe and Microscopy

Raman microprobe analysis

Raman microprobe characterization

Raman microprobe contamination

Raman microprobe experiments

Raman microprobe fibers

Raman microprobe purpose

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