scholarly journals Nature of red luminescence band in research-grade ZnO single crystals: A “self-activated” configurational transition

2014 ◽  
Vol 105 (4) ◽  
pp. 041912 ◽  
Author(s):  
Y. N. Chen ◽  
S. J. Xu ◽  
C. C. Zheng ◽  
J. Q. Ning ◽  
F. C. C. Ling ◽  
...  
2007 ◽  
Vol 90 (6) ◽  
pp. 063103 ◽  
Author(s):  
U. Philipose ◽  
S. Yang ◽  
T. Xu ◽  
Harry E. Ruda

2001 ◽  
Vol 15 (28n30) ◽  
pp. 3753-3756 ◽  
Author(s):  
T. AOKI-MATSUMOTO ◽  
K. FURUTA ◽  
T. YAMADA ◽  
H. MORIYA ◽  
K. MIZUNO ◽  
...  

Photoluminescence of pentacene single crystals is studied in the temperature range of 7 K to 200 K under excitation with He-Ne laser light. Photoluminescence spectra consist of four broad bands, L1 to L4. The highest energy band, L1, located close to the lowest exciton absorption band mainly appears for //b-polarization. The intensity of the second one, L2, with Stokes-shift of about 1500 cm -1, decreases as temperature rises above 30 K and disappears at 100 K. The bands, L3 and L4, which are located at lower energy, are observed at higher temperatures up to 200 K. Based on their energy positions, the band L2 is assigned to a shallow self-trapped exciton luminescence band, and the bands L3 and L4 to deep self-trapped exciton luminescence bands. By comparing this result with reported result on tetracene crystals, self-trapped excitons are considered to be more stable in pentacene.


2012 ◽  
Vol 111 (5) ◽  
pp. 054311 ◽  
Author(s):  
P. R. Coxon ◽  
M. Newman ◽  
M. R. C. Hunt ◽  
N. O’Farrell ◽  
B. R. Horrocks ◽  
...  

2017 ◽  
Vol 419 ◽  
pp. 476-483 ◽  
Author(s):  
I. Fraj ◽  
L. Favre ◽  
T. David ◽  
M. Abbarchi ◽  
K. Liu ◽  
...  

2009 ◽  
Vol 95 (22) ◽  
pp. 221904 ◽  
Author(s):  
Pan Gao ◽  
Mu Gu ◽  
Xiao-Lin Liu ◽  
Bo Liu ◽  
Shi-Ming Huang

2014 ◽  
Vol 104 (3) ◽  
pp. 032103 ◽  
Author(s):  
M. A. Reshchikov ◽  
A. Usikov ◽  
H. Helava ◽  
Yu. Makarov

Author(s):  
Lucien F. Trueb

A new type of synthetic industrial diamond formed by an explosive shock process has been recently developed by the Du Pont Company. This material consists of a mixture of two basically different forms, as shown in Figure 1: relatively flat and compact aggregates of acicular crystallites, and single crystals in the form of irregular polyhedra with straight edges.Figure 2 is a high magnification micrograph typical for the fibrous aggregates; it shows that they are composed of bundles of crystallites 0.05-0.3 μ long and 0.02 μ. wide. The selected area diffraction diagram (insert in Figure 2) consists of a weak polycrystalline ring pattern and a strong texture pattern with arc reflections. The latter results from crystals having preferred orientation, which shows that in a given particle most fibrils have a similar orientation.


Author(s):  
E. L. Thomas ◽  
S. L. Sass

In polyethylene single crystals pairs of black and white lines spaced 700-3,000Å apart, parallel to the [100] and [010] directions, have been identified as microsector boundaries. A microsector is formed when the plane of chain folding changes over a small distance within a polymer crystal. In order for the different types of folds to accommodate at the boundary between the 2 fold domains, a staggering along the chain direction and a rotation of the chains in the plane of the boundary occurs. The black-white contrast from a microsector boundary can be explained in terms of these chain rotations. We demonstrate that microsectors can terminate within the crystal and interpret the observed terminal strain contrast in terms of a screw dislocation dipole model.


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