scholarly journals Electron-phonon and phonon-phonon anharmonic interactions in 2H−MoX2 ( X=S,Te ): A comprehensive resonant Raman study

2021 ◽  
Vol 104 (7) ◽  
Author(s):  
Suvodeep Paul ◽  
Saheb Karak ◽  
Annie Mathew ◽  
Ankita Ram ◽  
Surajit Saha
1978 ◽  
Vol 25 (4) ◽  
pp. 209-211 ◽  
Author(s):  
Peter Y. Yu ◽  
Benjamin Welber

Author(s):  
F. Demangeot ◽  
J. Frandon ◽  
M. A. Renucci ◽  
H. Sands ◽  
D. Batchelder ◽  
...  

The photoluminescence and Raman spectra of several Ga1−xAlxN layers (0 ≤ x ≤ 0.86) grown on sapphire substrates by metal-organic vapor phase epitaxy have been recorded at room temperature, under an excitation at 244 nm. Using the photoluminescence spectra, the variation of the band gap of these alloys can be followed only up to x = 0.5. From resonant Raman scattering, it can be deduced that the band gap energy of the solid solution for x very close to 0.7 corresponds to the incident photon energy (5.08 eV). This result is confirmed by a detailed comparison of the present work with previous experimental data on the A1(LO) phonon peak position, obtained under visible excitation.


1987 ◽  
Vol 48 (C9) ◽  
pp. C9-827-C9-830
Author(s):  
S. MANNINEN ◽  
P. SUORTTI ◽  
M. J. COOPER ◽  
J. CHOMILIER ◽  
G. LOUPIAS
Keyword(s):  
X Ray ◽  

2000 ◽  
Vol 633 ◽  
Author(s):  
Sandra D. Brown ◽  
Ado Jorio ◽  
Paola Corio ◽  
Mildred Dresselhaus ◽  
Gene Dresselhaus ◽  
...  

AbstractWe present a resonant Raman study of the tangential G-band in metallic SWNTs. By measuring the Raman spectra for isolated SWNTs, we show that the two different lineshapes observed for semiconducting and metallic SWNTs in bundles also occur for isolated SWNTs. A lineshape analysis of the tangential G-band feature for metallic SWNT bundles is presented, showing that only two components are present, the higher frequency component having a Lorentzian lineshape, and the lower one having a Breit–Wigner–Fano (BWF) line-shape. Through comparisons of the Raman tangential G-band spectra from three different diameter distributions of carbon nanotubes, we find that both the frequency and linewidth of the BWF component are diameter dependent.


1990 ◽  
Vol 41 (14) ◽  
pp. 10138-10145 ◽  
Author(s):  
Hilde Fleurent ◽  
Dirk Schoemaker ◽  
Wim Joosen
Keyword(s):  

Small ◽  
2009 ◽  
Vol 5 (23) ◽  
pp. 2698-2702 ◽  
Author(s):  
J. Campos-Delgado ◽  
H. Farhat ◽  
Y. A. Kim ◽  
A. Reina ◽  
J. Kong ◽  
...  
Keyword(s):  

1987 ◽  
Vol 35 (6) ◽  
pp. 2892-2895 ◽  
Author(s):  
J. E. Zucker ◽  
A. Pinczuk ◽  
D. S. Chemla ◽  
A. C. Gossard

2005 ◽  
Vol 87 (7) ◽  
pp. 071902 ◽  
Author(s):  
I. L. Li ◽  
S. C. Ruan ◽  
Z. M. Li ◽  
J. P. Zhai ◽  
Z. K. Tang

1999 ◽  
Vol 14 (3) ◽  
pp. 1124-1131 ◽  
Author(s):  
A. Marucci ◽  
S. D. M. Brown ◽  
M. A. Pimenta ◽  
M. J. Matthews ◽  
M. S. Dresselhaus ◽  
...  

A resonant Raman study of polyparaphenylene (PPP) prepared by the Kovacic and the Yamamoto methods and heat-treated at temperatures THT between 650 and 750°C has been performed using different laser excitation energies Elaser between 1.92 and 3.05 eV. For samples treated at low THT, the Raman spectra change with Elaser, and this behavior is ascribed to the coexistence of two forms of the PPP polymer (benzenoid and quinoid) as well as a disordered carbon material. For higher THT samples, only a dispersion of the position of the Raman band as a function of Elaser is observed, and this is explained as due to the carbonization of the original polymer. The transition temperature between these two regions of resonance behavior is lower for the Yamamoto-PPP samples than for the Kovacic-PPP samples.


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