Formation energies and relative stability of perfect and faulted dislocation loops in silicon
Formation energies and relative stability of perfect and faulted dislocation loops in silicon
A study of the relative thermal stability of perfect and faulted dislocation loops formed during annealing of preamorphized silicon wafers has been carried out. A series of transmission electron microscopy experiments has been designed to study the influence of the ion dose, the annealing ambient and the proximity of a free surface on the evolution of both types of loops. Samples were implanted with either 150 keV Ge+ or 50 keV Si+ ions to a dose of 2×1015 cm–2 and annealed at 900 °C in N2, N2O, and O2. The calculations of formation energy of both types of dislocation loops show that, for defects of the same size, faulted dislocation loops (FDLs) are more energetically stable than perfect dislocation loops (PDLs) if their diameter is smaller than 80 nm and vice versa. The experimental results have been analyzed within the framework of the Ostwald ripening of two existing populations of interstitial defects. It is found that the defect ripening is nonconservative if the surface is close to the end of range defect layer or if the sample is oxidized during annealing. In both cases, the knowledge of the formation energy of both types of dislocation loops allows a realistic estimate of the interstitial flux towards and from the surface, respectively, during annealing, in agreement with the experimental results. During a conservative ripening process, a direct correspondence exists between the formation energy of the two defect families and the number of atoms bound to them. In this case, the relative stability of FDLs and PDLs depends on the initial supersaturation of Si interstitial atoms created during implantation
8420-8428
Cristiano, F.
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Grisolia, J.
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Colombeau, B.
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Omri, M.
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De Mauduit, B.
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Claverie, A.
8a62fe63-c992-4c62-872b-5cce1ecf397c
Giles, F.
8896c267-238d-494b-90bf-c4e9eefffee8
Cowern, N.E.B.
d5f2073f-03d8-42bc-bf2d-e9024c7b15bf
2000
Cristiano, F.
7410e8d7-50f3-452f-90f7-110d4303edfb
Grisolia, J.
30fc73f3-f935-4e0a-962c-f3d6757e0f26
Colombeau, B.
3cd2d3b9-12d6-41bc-b9e2-064fa8414bb4
Omri, M.
8fed2fbe-eba8-4efa-8bc9-b3f980370530
De Mauduit, B.
613ef413-dd2f-4be6-bc1d-81eb1a2bad17
Claverie, A.
8a62fe63-c992-4c62-872b-5cce1ecf397c
Giles, F.
8896c267-238d-494b-90bf-c4e9eefffee8
Cowern, N.E.B.
d5f2073f-03d8-42bc-bf2d-e9024c7b15bf
Cristiano, F., Grisolia, J., Colombeau, B., Omri, M., De Mauduit, B., Claverie, A., Giles, F. and Cowern, N.E.B.
(2000)
Formation energies and relative stability of perfect and faulted dislocation loops in silicon.
Journal of Applied Physics, 87 (12), .
(doi:10.1063/1.373557).
Abstract
A study of the relative thermal stability of perfect and faulted dislocation loops formed during annealing of preamorphized silicon wafers has been carried out. A series of transmission electron microscopy experiments has been designed to study the influence of the ion dose, the annealing ambient and the proximity of a free surface on the evolution of both types of loops. Samples were implanted with either 150 keV Ge+ or 50 keV Si+ ions to a dose of 2×1015 cm–2 and annealed at 900 °C in N2, N2O, and O2. The calculations of formation energy of both types of dislocation loops show that, for defects of the same size, faulted dislocation loops (FDLs) are more energetically stable than perfect dislocation loops (PDLs) if their diameter is smaller than 80 nm and vice versa. The experimental results have been analyzed within the framework of the Ostwald ripening of two existing populations of interstitial defects. It is found that the defect ripening is nonconservative if the surface is close to the end of range defect layer or if the sample is oxidized during annealing. In both cases, the knowledge of the formation energy of both types of dislocation loops allows a realistic estimate of the interstitial flux towards and from the surface, respectively, during annealing, in agreement with the experimental results. During a conservative ripening process, a direct correspondence exists between the formation energy of the two defect families and the number of atoms bound to them. In this case, the relative stability of FDLs and PDLs depends on the initial supersaturation of Si interstitial atoms created during implantation
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Published date: 2000
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Local EPrints ID: 21519
URI: http://eprints.soton.ac.uk/id/eprint/21519
ISSN: 0021-8979
PURE UUID: 673db104-ffbe-4617-8ee6-6a369563b8fe
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Date deposited: 06 Feb 2007
Last modified: 15 Mar 2024 06:31
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Author:
F. Cristiano
Author:
J. Grisolia
Author:
B. Colombeau
Author:
M. Omri
Author:
B. De Mauduit
Author:
A. Claverie
Author:
F. Giles
Author:
N.E.B. Cowern
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