Controlled p-type Sb doping in LPE-grown Hg1−x Cdx Te epilayers

1993 ◽  
Vol 22 (9) ◽  
pp. 1165-1172 ◽  
Author(s):  
Theodore C. Harman
Keyword(s):  
2022 ◽  
pp. 131365
Author(s):  
Guanyu Yao ◽  
Jun Yu ◽  
Hao Wu ◽  
Zhongzhou Li ◽  
Wenjing Zou ◽  
...  

1991 ◽  
Vol 220 ◽  
Author(s):  
Richard Kubiak ◽  
Carl Parry

ABSTRACTThis paper reviews the diverse methods used to achieve doping during MBE of Si and SiGe, and the incorporation processes involved. The optimum choice of dopant and methodology depends on the most appropriate growth conditions for a given structure. At growth temperatures exceeding 750°C, Potential Enhanced n-type doping of coevaporated Sb is capable of achieving high resolution structures, at doping levels up to mid-1019 cm−3. At lower temperatures, such as those most suited to SiGe growth, Sb-doping becomes a formidable challenge, due to the high accumulated equilibrium coverages required. Low energy ion implantation appears to be the favoured route for good control, p-type B-doping can readily be achieved by coevaporation of compounds or, to avoid oxygen incorporation at low temperatures, the element. A “designer” chart for B-doping of Si is presented.


RSC Advances ◽  
2018 ◽  
Vol 8 (61) ◽  
pp. 35023-35030 ◽  
Author(s):  
Linlin Shi ◽  
Luchao Du ◽  
Yingtian Xu ◽  
Liang Jin ◽  
He Zhang ◽  
...  

Sb-doped microwires which have a zigzag rough surface demonstrate p-type conduction and enhanced rectifying behavior with increasing Sb doping concentration.


2010 ◽  
Vol 1256 ◽  
Author(s):  
Joe Briscoe ◽  
Diego E. Gallardo ◽  
Steve Dunn

AbstractThe in-situ aqueous synthesis of ZnO nanorods doped with Sb is presented. To control the inclusion of Sb into the ZnO nanorods structure ethylene glycol (EG) is added to the reaction solution. The addition of EG reduces the rate at which Sb is included in the ZnO rods and produces nanorods with a morphology that is similar to the undoped rods. This is contrary to the rods produced with Sb in the absence of EG which produce a less well ordered structure. An I/V curve taken from individual rods indicates a change in the diode behaviour. The change in I/V behaviour is associated with a change from the natural n-type behaviour of ZnO to a p-type behaviour due to the Sb doping.


2006 ◽  
Author(s):  
J. L. Liu ◽  
F. X. Xiu ◽  
L. J. Mandalapu ◽  
Z. Yang
Keyword(s):  

2011 ◽  
Vol 98 (13) ◽  
pp. 131902 ◽  
Author(s):  
F. Friedrich ◽  
I. Sieber ◽  
C. Klimm ◽  
M. Klaus ◽  
Ch. Genzel ◽  
...  
Keyword(s):  

2006 ◽  
Vol 89 (20) ◽  
pp. 202102 ◽  
Author(s):  
Peng Wang ◽  
Nuofu Chen ◽  
Zhigang Yin ◽  
Ruixuan Dai ◽  
Yiming Bai

2007 ◽  
Vol 40 (14) ◽  
pp. 4241-4244 ◽  
Author(s):  
X H Pan ◽  
Z Z Ye ◽  
Y J Zeng ◽  
X Q Gu ◽  
J S Li ◽  
...  
Keyword(s):  

Author(s):  
H. Yen ◽  
E. P. Kvam ◽  
R. Bashir ◽  
S. Venkatesan ◽  
G. W. Neudeck

Polycrystalline silicon, when highly doped, is commonly used in microelectronics applications such as gates and interconnects. The packing density of integrated circuits can be enhanced by fabricating multilevel polycrystalline silicon films separated by insulating SiO2 layers. It has been found that device performance and electrical properties are strongly affected by the interface morphology between polycrystalline silicon and SiO2. As a thermal oxide layer is grown, the poly silicon is consumed, and there is a volume expansion of the oxide relative to the atomic silicon. Roughness at the poly silicon/thermal oxide interface can be severely deleterious due to stresses induced by the volume change during oxidation. Further, grain orientations and grain boundaries may alter oxidation kinetics, which will also affect roughness, and thus stress.Three groups of polycrystalline silicon films were deposited by LPCVD after growing thermal oxide on p-type wafers. The films were doped with phosphorus or arsenic by three different methods.


Author(s):  
Y. Kikuchi ◽  
N. Hashikawa ◽  
F. Uesugi ◽  
E. Wakai ◽  
K. Watanabe ◽  
...  

In order to measure the concentration of arsenic atoms in nanometer regions of arsenic doped silicon, the HOLZ analysis is carried out underthe exact [011] zone axis observation. In previous papers, it is revealed that the position of two bright lines in the outer SOLZ structures on the[011] zone axis is little influenced by the crystal thickness and the background intensity caused by inelastic scattering electrons, but is sensitive to the concentration of As atoms substitutbnal for Siatomic site.As the result, it becomes possible to determine the concentration of electrically activated As atoms in silicon within an observed area by means of the simple fitting between experimental result and dynamical simulatioan. In the present work, in order to investigate the distribution of electrically activated As in silicon, the outer HOLZ analysis is applied using a nanometer sized probe of TEM equipped with a FEG.Czodiralsld-gown<100>orientated p-type Si wafers with a resistivity of 10 Ώ cm are used for the experiments.TheAs+ implantation is performed at a dose of 5.0X1015cm-2at 25keV.


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