Vibrational characterization of C60 solid films using Raman spectroscopy.
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Vibrational characterization of C60 solid films using Raman spectroscopy. by Kelly Lynn Akers

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Published .
Written in English


Book details:

The Physical Object
Pagination140 leaves.
Number of Pages140
ID Numbers
Open LibraryOL16934631M
ISBN 100315971541
OCLC/WorldCa221216409

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Using an improved DFT calculation of the vibrational frequencies based on the B3-LYP functional and the G* basis set, the infrared, Raman, neutron inelastic and luminescence spectra of C60 are rediscussed, and a revised assignment of all the silent modes is obtained and compared with the most recent by:   Abstract Vibrational Raman spectra have been obtained at 1 cm−1 resolution, for C60 and C For C60 the positions of the bands were in good agreement with theoretical predictions. For C70 . Raman spectroscopy is a widely used characterization technique in material science. It is a non-destructive tool with relatively simple instrumentation, and provides intrinsic qualitative information of analytes by probing their vibrational modes. In many cases, Raman enhancement is essential for detecting low-intensity signals in high-noise environments, spectrally unresolved features, and Author: Vinayaka H. Damle, Miri Sinwani, Hagit Aviv, Yaakov R. Tischler. Raman spectroscopy is a scattering technique, and can readily be used on opaque and solid samples, unlike IR absorbance spectroscopy. The exact intensity of Raman scattering from a particular vibrational mode is a complex matter, but, generally, will increase as the number of Figure 3. Ratiometric calibration curve.

Vibrational spectroscopy has been used to characterize the three uncommon complex iron sulfates clairite, (NH 4) 2 Fe 3 (SO 4) 4 (OH) 3 3H 2 O, metavoltine, Na 6 K 2 Fe 2+ Fe 3+ 6 (SO 4) 12 O 2 18H 2 O, and voltaite, K 2 Fe 2+ 5 Fe 3+ 3 Al(SO 4) 12 18H 2 O. The investigated specimens were formed at the burning coal dump Anna I (Alsdorf, Germany) due to alteration processes connected with the.   The Raman scattering of multi-walled carbon nanotubes (MWNTs) has also been discussed in Sect. Section presents the discussion on phonon properties and Raman scattering of graphene. In Sect. , the basic mechanism of surface-enhanced Raman spectroscopy (SERS) and its application to probe individual molecules are given. Raman spectroscopy is another vibrational technique, currently gaining popularity because recent technological advances have made the instrumentation more accessible. Figure 5 shows a basic schematic of the Raman spectrometer you will use in the lab. Raman spectroscopy uses a single wavelength laser source to excite the electrons in a sample. Vibrational Spectroscopy (IR, Raman) Vibrational spectroscopy. In order to describe the 3N-6 or 3N-5 different possibilities how non-linear and linear molecules containing N atoms can vibrate, the models of the harmonic and anharmonic oscillators are used. These modes of vibration (normal modes) give rise to • absorption bands (IR).

Photoinduced Polymerization of Solid C60 Films Article (PDF Available) in Science () February with Reads How we measure 'reads'. Abstract. Experimental studies of the vibrational modes of pristine and photopolymerized solid C 60 films are presented. A modest flux of visible or ultraviolet light is shown in the temperature range > T > K to transform C 60 into a second solid phase which is identified with a polymeric form. A photochemical “2+2 cycloaddition” reaction mechanism is proposed to form the C 60 polymer. Raman spectroscopy is the standard characterization technique for nanotubes. Raman spectrum of C 60 @SWBNNT have been reported in the literature at different laser energies (, and nm) [].All fundamental Raman lines of the encapsulated C 60 peas are observed and a structured peak at , , and cm − 1 is measured and assigned to the reaction products of the carbon.   Raman spectroscopy was used to characterize the residual stress and defect density of AlN thin films reactively sputtered on silicon (). The authors studied the correlation between the shift of the E 2 (high) phonon of AlN at cm − 1 and the film biaxial stress and obtained a biaxial piezospectroscopic coefficient of GPa ∕ cm − 1.A correlation was found between the width of the.