Optical charge state manipulation of divacancy spins in silicon carbide under resonant excitation

2021 ◽  
Author(s):  
Junfeng Wang ◽  
Jiyang Zhou ◽  
qiang li ◽  
Feifei Yan ◽  
Mu Yang ◽  
...  
2017 ◽  
Vol 8 (1) ◽  
Author(s):  
Gary Wolfowicz ◽  
Christopher P. Anderson ◽  
Andrew L. Yeats ◽  
Samuel J. Whiteley ◽  
Jens Niklas ◽  
...  

2007 ◽  
Vol 401-402 ◽  
pp. 631-634 ◽  
Author(s):  
H.N. Bani-Salameh ◽  
A.G. Meyer ◽  
B.R. Carroll ◽  
R.L. Lichti ◽  
Y.G. Celebi ◽  
...  

Nano Letters ◽  
2019 ◽  
Vol 19 (10) ◽  
pp. 7173-7180 ◽  
Author(s):  
Matthias Widmann ◽  
Matthias Niethammer ◽  
Dmitry Yu. Fedyanin ◽  
Igor A. Khramtsov ◽  
Torsten Rendler ◽  
...  

Nano Letters ◽  
2020 ◽  
Vol 20 (8) ◽  
pp. 6142-6147
Author(s):  
Zhao Mu ◽  
Soroush Abbasi Zargaleh ◽  
Hans Jürgen von Bardeleben ◽  
Johannes E. Fröch ◽  
Milad Nonahal ◽  
...  

2017 ◽  
Vol 111 (26) ◽  
pp. 262403 ◽  
Author(s):  
Charles F. de las Casas ◽  
David J. Christle ◽  
Jawad Ul Hassan ◽  
Takeshi Ohshima ◽  
Nguyen T. Son ◽  
...  

2008 ◽  
Vol 600-603 ◽  
pp. 537-540
Author(s):  
Alexander A. Lebedev ◽  
M. Lemmer ◽  
B. Hilling ◽  
M. Wohlecke ◽  
Mirco Imlau ◽  
...  

Resonant excitation of space charge waves (SCW) by means of an oscillating light pattern has been investigated in hexagonal silicon carbide with 4H and 6H stacking sequence. The experimental data can be explained by the existence of trap recharging waves in the 4H-SiC sample and damped forced charge-density waves in the 6H-SiC sample.


2021 ◽  
Vol 129 (21) ◽  
pp. 215702
Author(s):  
Nguyen T. Son ◽  
Ivan G. Ivanov

Author(s):  
R. J. Lauf

Fuel particles for the High-Temperature Gas-Cooled Reactor (HTGR) contain a layer of pyrolytic silicon carbide to act as a miniature pressure vessel and primary fission product barrier. Optimization of the SiC with respect to fuel performance involves four areas of study: (a) characterization of as-deposited SiC coatings; (b) thermodynamics and kinetics of chemical reactions between SiC and fission products; (c) irradiation behavior of SiC in the absence of fission products; and (d) combined effects of irradiation and fission products. This paper reports the behavior of SiC deposited on inert microspheres and irradiated to fast neutron fluences typical of HTGR fuel at end-of-life.


Author(s):  
K. B. Alexander ◽  
P. F. Becher

The presence of interfacial films at the whisker-matrix interface can significantly influence the fracture toughness of ceramic composites. The film may alter the interface debonding process though changes in either the interfacial fracture energy or the residual stress at the interface. In addition, the films may affect the whisker pullout process through the frictional sliding coefficients or the extent of mechanical interlocking of the interface due to the whisker surface topography.Composites containing ACMC silicon carbide whiskers (SiCw) which had been coated with 5-10 nm of carbon and Tokai whiskers coated with 2 nm of carbon have been examined. High resolution electron microscopy (HREM) images of the interface were obtained with a JEOL 4000EX electron microscope. The whisker geometry used for HREM imaging is described in Reference 2. High spatial resolution (< 2-nm-diameter probe) parallel-collection electron energy loss spectroscopy (PEELS) measurements were obtained with a Philips EM400T/FEG microscope equipped with a Gatan Model 666 spectrometer.


Author(s):  
L. A. Giannuzzi ◽  
C. A. Lewinsohn ◽  
C. E. Bakis ◽  
R. E. Tressler

The SCS-6 SiC fiber is a 142 μm diameter fiber consisting of four distinct regions of βSiC. These SiC regions vary in excess carbon content ranging from 10 a/o down to 5 a/o in the SiC1 through SiC3 region. The SiC4 region is stoichiometric. The SiC sub-grains in all regions grow radially outward from the carbon core of the fiber during the chemical vapor deposition processing of these fibers. In general, the sub-grain width changes from 50nm to 250nm while maintaining an aspect ratio of ~10:1 from the SiC1 through the SiC4 regions. In addition, the SiC shows a <110> texture, i.e., the {111} planes lie ±15° along the fiber axes. Previous has shown that the SCS-6 fiber (as well as the SCS-9 and the developmental SCS-50 μm fiber) undergoes primary creep (i.e., the creep rate constantly decreases as a function of time) throughout the lifetime of the creep test.


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