Confined Acoustic Vibration Modes in CuBr Quantum Dots

2005 ◽  
Vol 74 (11) ◽  
pp. 3082-3087 ◽  
Author(s):  
Michio Ikezawa ◽  
Jialong Zhao ◽  
Atsushi Kanno ◽  
Yasuaki Masumoto
Author(s):  
Victor Farm-Guoo Tseng ◽  
Daniel Diamond ◽  
Sarah Goodrich ◽  
Joshua J. Radice ◽  
Nathan Lazarus ◽  
...  

2006 ◽  
Vol 132 ◽  
pp. 307-310
Author(s):  
J. Geurts ◽  
U. Bass ◽  
S. Mahapatra ◽  
K. Brunner ◽  
T. Muck ◽  
...  

Nano Letters ◽  
2008 ◽  
Vol 8 (5) ◽  
pp. 1296-1302 ◽  
Author(s):  
J. Burgin ◽  
P. Langot ◽  
A. Arbouet ◽  
J. Margueritat ◽  
J. Gonzalo ◽  
...  

1993 ◽  
Vol 36 (5) ◽  
pp. 1423-1429 ◽  
Author(s):  
L. Huarng ◽  
P. Chen ◽  
S. Upadhyaya

2002 ◽  
Vol 44 (10) ◽  
pp. 1976-1980 ◽  
Author(s):  
A. G. Milekhin ◽  
L. L. Sveshnikova ◽  
S. M. Repinskii ◽  
A. K. Gutakovskii ◽  
M. Friedrich ◽  
...  

2013 ◽  
Vol 27 (18) ◽  
pp. 1350134 ◽  
Author(s):  
Y. XING ◽  
X. X. LIANG ◽  
Z. P. WANG

Using a dielectric continuum approach, the optical vibration modes in a spherical core-shell quantum dots (QDs) imbedded in a host nonpolar material are studied. The dispersion relation and the corresponding electron–phonon interaction Hamiltonian are derived. The numerical calculations for the CdSe/ZnS system are performed. The results reveal that there are three branches frequencies of interface/surface optical phonon in the system. A detailed discussion of the combined effects of the spatial confinement and dielectric mismatch between the dot and the host medium is given.


Author(s):  
M.J. Kim ◽  
L.C. Liu ◽  
S.H. Risbud ◽  
R.W. Carpenter

When the size of a semiconductor is reduced by an appropriate materials processing technique to a dimension less than about twice the radius of an exciton in the bulk crystal, the band like structure of the semiconductor gives way to discrete molecular orbital electronic states. Clusters of semiconductors in a size regime lower than 2R {where R is the exciton Bohr radius; e.g. 3 nm for CdS and 7.3 nm for CdTe) are called Quantum Dots (QD) because they confine optically excited electron- hole pairs (excitons) in all three spatial dimensions. Structures based on QD are of great interest because of fast response times and non-linearity in optical switching applications.In this paper we report the first HREM analysis of the size and structure of CdTe and CdS QD formed by precipitation from a modified borosilicate glass matrix. The glass melts were quenched by pouring on brass plates, and then annealed to relieve internal stresses. QD precipitate particles were formed during subsequent "striking" heat treatments above the glass crystallization temperature, which was determined by differential thermal analysis.


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