Theory of resonant Raman scattering from low-energy collective excitations of interacting electrons in quantum wires

1998 ◽  
Vol 4 (3) ◽  
pp. 357-367 ◽  
Author(s):  
M. Sassetti ◽  
B. Kramer
2013 ◽  
Vol 410 ◽  
pp. 126-130 ◽  
Author(s):  
Re. Betancourt-Riera ◽  
Ri. Betancourt-Riera ◽  
J.M. Nieto Jalil ◽  
R. Riera

2000 ◽  
Vol 49 (2) ◽  
pp. 224-230 ◽  
Author(s):  
E Mariani ◽  
M Sassetti ◽  
B Kramer

2007 ◽  
Vol 21 (17) ◽  
pp. 2989-3000
Author(s):  
XIANG-FU ZHAO ◽  
CUI-HONG LIU

The scattering intensity (SI) for an electron resonant Raman scattering (ERRS) process in a free-standing semiconductor quantum wire of cylindrical geometry associated with bulk longitudinal optical (LO) phonon modes or the surface optical (SO) phonon modes is calculated for T=0 K . The Fröhlich interaction is considered to illustrate the theory for a GaAs system. Electron states are confined within a free-standing quantum wire (FSW). Single parabolic conduction and valence bands are assumed. The selection rules are studied. Numerical results and a discussion are also presented for various radii of the cylindrical quantum wires.


1990 ◽  
Vol 101 (1-4) ◽  
pp. 940-943 ◽  
Author(s):  
D. Scalbert ◽  
J.A. Gaj ◽  
A. Mauger ◽  
J. Cernogora ◽  
C. Benoit ÁLa Guillaume ◽  
...  

2001 ◽  
Vol 15 (22) ◽  
pp. 3031-3038
Author(s):  
HYUN C. LEE

Resonant Raman scattering of degenerate interacting two-channel quantum wire is studied. All collective excitations of two-channel quantum wire are shown to give rise to peaks in the polarized Raman spectra near resonance. If there exist certain symmetries among interactions, a resonant peak can also appear in the depolarized Raman spectra, in contrast to the single-channel case studied by Sassetti and Kramer. We also calculate the explicit form of the scattering cross-section away from the peaks. The above features may be experimentally verified in armchair carbon nanotube systems.


1989 ◽  
Vol 69 (5) ◽  
pp. 453-456 ◽  
Author(s):  
D. Scalbert ◽  
J. Cernogora ◽  
A. Mauger ◽  
C.Benoit àla Guillaume ◽  
A. Mycielski

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