Characterization of DNA structures by laser Raman spectroscopy

Biopolymers ◽  
1984 ◽  
Vol 23 (2) ◽  
pp. 235-256 ◽  
Author(s):  
B. Prescott ◽  
W. Steinmetz ◽  
G. J. Thomas
Keyword(s):  
Raman Spectroscopy ◽  
Laser Raman Spectroscopy ◽  
Dna Structures ◽  
Laser Raman

Characterization of the coke formed on reforming catalysts by laser raman spectroscopy

1985 ◽  
Vol 16 (3) ◽  
pp. 343-354 ◽  
Author(s):  
D. Espinat ◽  
H. Dexpert ◽  
E. Freund ◽  
G. Martino ◽  
M. Couzi ◽  
...  
Keyword(s):  
Raman Spectroscopy ◽  
Laser Raman Spectroscopy ◽  
Laser Raman ◽  
Reforming Catalysts

Characterization of Humic Substances by Laser Raman Spectroscopy

1994 ◽  
Vol 27 (5) ◽  
pp. 649-660 ◽  
Author(s):  
Yu-hui YANG ◽  
Bo-nian Li ◽  
Zu-yi Tao
Keyword(s):  
Raman Spectroscopy ◽  
Humic Substances ◽  
Laser Raman Spectroscopy ◽  
Laser Raman

Characterization of GaAsAlAs superlattices by laser-Raman spectroscopy

1984 ◽  
Vol 49 (2) ◽  
pp. 157-159 ◽  
Author(s):  
K. Kubota ◽  
M. Nakayama ◽  
H. Katoh ◽  
N. Sano
Keyword(s):  
Raman Spectroscopy ◽  
Laser Raman Spectroscopy ◽  
Laser Raman

scholarly journals Characterization of Metal/Carbon Multilayers by Raman Spectroscopy

1989 ◽  
Vol 160 ◽  
Author(s):  
David D. Allred ◽  
Qi Wang ◽  
Jesus Gonzalez-Hernandez
Keyword(s):  
Raman Spectroscopy ◽  
Amorphous Semiconductor ◽  
Laser Raman Spectroscopy ◽  
Plasma Confinement ◽  
Ray Optics ◽  
X Ray ◽  
Laser Raman ◽  
Line Shapes ◽  
Two Peaks

AbstractLaser Raman spectroscopy has been found to be useful for characterizing amorphous semiconductor multilayers, especially the interfaces of multilayers. Recently, we have extended this technique to the characterization of magnetron sputtered multilayers commonly used as reflectors in soft x-ray optics. Unlike the multilayers previously studied which contained only semiconductors and dielectrics, these are generally semiconductor/metal multilayers. We report here on the Raman characterization of the most common class of multilayers used in soft x-ray optics, those that contain a high density metal like tungsten interspersed with layers of carbon. In all of the metal/carbon multilayers the dominate feature in the Raman spectra is due to a-C. The a-C spectra consists of a broad peak at about 1560 cm-1 (G-peak) and a shoulder at about 1400 cm-1 (D-peak). This can be deconvoluted with Gaussian line shapes to yield two peaks (one at about 1560 to 1570 cm-1 and the other at about 1380 to 1420 cm-1). Among the W/C multilayer samples peak positions and relative magnitudes changed little with carbon thickness over the range of 1 to 12 nm. Significant differences are, however, seen as the identity of the metal component is altered or, especially, as the preparations are varied. For example, the intensity ratio of the D-peak to G-peak was much larger for multilayer samples prepared under conditions of good plasma confinement.

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