Transient Dose Loss of Phosphorus during Postimplantation Annealing at 800 °C

2007 ◽  
Vol 46 (7A) ◽  
pp. 4035-4037 ◽  
Author(s):  
Jung-Ruey Tsai ◽  
Li-Wei Ho ◽  
Ruey-Dar Chang
2005 ◽  
Vol 864 ◽  
Author(s):  
T. Cesca ◽  
A. Gasparotto ◽  
G. Mattei ◽  
A. Verna ◽  
B. Fraboni ◽  
...  

AbstractWe have investigated the structural and electrical behavior of Fe centers introduced in InP by high temperature ion implantation. The lattice location of the Fe atoms and the effect of postimplantation annealing treatments have been studied by PIXE-channeling measurements. I-V, CV and DLTS analyses have been used to characterize the electrical properties related to the presence Fe2+/3+ deep traps. The results show that the background n-doping density play a crucial role in controlling the annealing behavior and the electrical activation of the Fe centers. The same effect has been observed in samples containing Fe concentrations both above and below the Fe solubility threshold in InP.


1996 ◽  
Vol 11 (10) ◽  
pp. 2463-2469 ◽  
Author(s):  
M. K. Puchert ◽  
A. Hartmann ◽  
R. N. Lamb ◽  
J. W. Martin

Polycrystalline (0001)-oriented thin films of ZnO (thickness 120 nm) were deposited by rf magnetron sputtering and post-deposition annealed at 500 °C in oxygen (1 atm). The films were subsequently implanted with copper at doses over the range 1016 to 1017 ions/cm2. X-ray diffraction (XRD) indicates the compressive intrinsic film stress is largely relieved by the preimplantation anneal, and does not change when implanted or when further annealed after implantation, suggesting that the dominant cause of intrinsic stress is the atomic packing density rather than the crystallographic defect density. Resistivity measurements indicate that annealing of pure ZnO films causes the perpendicular resistivity to increase from 1.3 × 105 Ω · cm to 5 × 1010 Ω · cm. Copper implantation results in a lower resistivity of the order of 107 Ω · cm, but subsequent annealing actually increases resistivity beyond that of annealed nonimplanted ZnO to 3 × 1012 Ω · cm. It is proposed that copper increases the resistivity of those annealed films by trapping free electrons with the Cu 3d hole state occurring in CuO (formed predominantly during annealing). In order to check this, the oxidation state of the implanted copper was studied before and after annealing by x-ray photoelectron spectroscopy (XPS) and extended x-ray absorption fine structure (EXAFS). Three oxidation states of copper (Cu0, Cu1+, Cu2+) are detected in the implanted films, and postimplantation annealing results in oxidation of copper to the Cu2+ state, confirming that the presence of CuO in ZnO is associated with increased resistivity.


2002 ◽  
Vol 41 (Part 1, No. 3A) ◽  
pp. 1220-1223 ◽  
Author(s):  
Ruey-Dar Chang ◽  
Philip S. Choi ◽  
Dim-Lee Kwong ◽  
Mark Gardner ◽  
Paul K. Chu

1994 ◽  
Vol 212-215 ◽  
pp. 375-381 ◽  
Author(s):  
V.N. Chernikov ◽  
Ju.V. Lakhotkin ◽  
H. Ullmaier ◽  
H. Trinkaus ◽  
P. Jung ◽  
...  

1996 ◽  
Vol 442 ◽  
Author(s):  
N.A. Sobolev ◽  
O.V. Aleksandrov ◽  
E.I. Shek

AbstractDependence of the donor center concentration, the Er activation coefficient and the nlayer thickness on the implantation and subsequent annealing conditions was studied. A model of formation of donor centers has been developed. The model is based on the interaction of Er atoms with self-interstitials. It describes the dependence of electrical parameters of Er-doped layers on temperature and time of postimplantation annealing.


2007 ◽  
Vol 556-557 ◽  
pp. 611-614 ◽  
Author(s):  
Erwan Oliviero ◽  
Mihai Lazar ◽  
Heu Vang ◽  
Christiane Dubois ◽  
Pierre Cremillieu ◽  
...  

6H and 4H–SiC epilayers were Al-implanted at room temperature with multiple energies (ranging from 25 to 300 keV) in order to form p-type layers with an Al plateau concentration of 4.5×1019 cm-3 and 9×1019 cm-3. Post-implantation annealing were performed at 1700 or 1800 °C up to 30 min in Ar ambient. During this process, some samples were encapsulated with a graphite (C) cap obtained by thermal conversion of a spin-coated AZ5214E photoresist. From Atomic Force Microscope measurements, the roughness is found to increase drastically with annealing temperature for unprotected samples while the C capped samples show a preservation of their surface states even for the highest annealing temperature. After 1800°C/30 min annealing, the RMS roughness is 0.46 nm for the lower fluence implanted samples, slightly higher than for unimplanted samples (0.31 nm). Secondary Ion Mass Spectroscopy measurements confirm that the C cap was totally removed from the SiC surface. The total Al-implanted fluence is preserved during postimplantation annealing. A redistribution of the Al dopants is observed at the surface which might be attributed to Si vacancy-enhanced diffusion. An accumulation peak is also observed after annealing at 0.29 9m, depth corresponding to the amorphous/crystalline interface that was determined on the as-implanted samples by Rutherford Backscattering Spectroscopy in channeling mode. The redistribution of the dopants has an impact on their electrical activation. A lower sheet resistance (Rsh= 8 k) is obtained for samples annealed without capping than for samples annealed with C capping (Rsh= 15 k ).


2020 ◽  
Vol 67 (10) ◽  
pp. 4360-4365
Author(s):  
Johanna Muting ◽  
Viktor Bobal ◽  
Marc Georg Willinger ◽  
Ali Baghi Zadeh ◽  
Steffen Reidt ◽  
...  

1999 ◽  
Vol 74 (26) ◽  
pp. 3996-3998 ◽  
Author(s):  
E. Schroer ◽  
V. Privitera ◽  
F. Priolo ◽  
E. Napolitani ◽  
A. Carnera

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