Real-time band structure changes of GaAs during continuous dynamic compression to 5 GPa

2009 ◽  
Vol 95 (15) ◽  
pp. 152108 ◽  
Author(s):  
P. Grivickas ◽  
M. D. McCluskey ◽  
Y. M. Gupta
Keyword(s):  
Band Structure ◽  
Real Time ◽  
Dynamic Compression ◽  
Structure Changes ◽  
Continuous Dynamic ◽  
Time Band

Lattice and electronic band structure changes across the surface ferroelectric transition

1998 ◽  
Vol 249 (5-6) ◽  
pp. 505-511 ◽  
Author(s):  
Jaewu Choi ◽  
P.A. Dowben ◽  
Stephen Ducharme ◽  
V.M. Fridkin ◽  
S.P. Palto ◽  
...  
Keyword(s):  
Band Structure ◽  
Electronic Band Structure ◽  
Electronic Band ◽  
Ferroelectric Transition ◽  
Structure Changes

Uniaxial stress induced band structure changes in h-SiB

2018 ◽  
Author(s):  
M. S. Manju ◽  
K. M. Ajith ◽  
M. C. Valsakumar
Keyword(s):  
Band Structure ◽  
Uniaxial Stress ◽  
Structure Changes

scholarly journals 52 REAL-TIME PCR USING MOLECULAR BEACONS TO DETECT INOS AND COX-2 EXPRESSION IN CHONDROCYTE/AGAROSE CONSTRUCTS SUBJECTED TO IL-1β AND DYNAMIC COMPRESSION

2007 ◽  
Vol 15 ◽  
pp. C42-C43
Author(s):  
T.T. Chowdhury ◽  
O.O. Akanji ◽  
S. Arghandawi ◽  
D.M. Salter ◽  
D.L. Bader ◽  
...  
Keyword(s):  
Real Time ◽  
Real Time Pcr ◽  
Dynamic Compression ◽  
Molecular Beacons ◽  
Cox 2

Band Structure Changes in Interealates of Niobium Diselenide

1976 ◽  
Vol 76 (2) ◽  
pp. 599-604 ◽  
Author(s):  
A. R. Birks ◽  
S. P. Hind ◽  
P. M. Lee
Keyword(s):  
Band Structure ◽  
Niobium Diselenide ◽  
Structure Changes

Grain Refinement in Magnesium Alloy AZ31 during Hot Deformation

2004 ◽  
Vol 467-470 ◽  
pp. 531-536 ◽  
Author(s):  
Xu Yue Yang ◽  
Hiromi Miura ◽  
Taku Sakai
Keyword(s):  
Magnesium Alloy ◽  
Kink Bands ◽  
Alloy Az31 ◽  
Continuous Dynamic Recrystallization ◽  
Magnesium Alloy Az31 ◽  
Structure Changes ◽  
Coarse Grains ◽  
Grain Fragmentation ◽  
Continuous Reaction ◽  
Continuous Dynamic

The deformation behavior and structure changes of magnesium alloy AZ31 were studied in compression at temperatures ranging from 523K to 673K and at a strain rate of 3 x 10-3 s-1. They depend sensitively on deformation temperature. At high temperatures, grain fragmentation takes place due to frequent formation of kink bands initially at corrugated grain boundaries and then in grain interiors, followed by full development of new grains in high strain. At lower temperatures, in contrast, twinning takes place in rather coarse grains and kink bands are formed mainly in finer original ones in low strain. It is concluded that new grain evolution can be controlled by a deformation-induced continuous reaction resulting in grain fragmentation by kink bands, i.e. continuous dynamic recrystallization (cDRX). The latter is discussed comparing with conventional, i.e. discontinuous, DRX.

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