2009
DOI: 10.1063/1.3268472
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Defect kinetics and dopant activation in submicrosecond laser thermal processes

Abstract: Defect evolution in ion implanted c-Si at the submicrosecond time scales during a laser thermal annealing process is investigated by means of kinetic simulations. Nonmelting, melting, and partial melting regimes are simulated. Our modeling considers irradiation, heat diffusion, and phase transition together with defect diffusion, annihilation, and clustering. The reduction in the implantation damage and its reorganization in defect aggregates are studied as a function of the process conditions. The approach is… Show more

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Cited by 26 publications
(18 citation statements)
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“…Hence, along with KMC methodologies, great interest has developed in the past decades in continuous models, which deal with the same issues previously reported [14][15][16].…”
Section: Fully Continuous Modelingmentioning
confidence: 99%
“…Hence, along with KMC methodologies, great interest has developed in the past decades in continuous models, which deal with the same issues previously reported [14][15][16].…”
Section: Fully Continuous Modelingmentioning
confidence: 99%
“…1.5 J/cm 2 ) at a temperature just below the melting threshold. The calculation was made coupling the phase-field methodology 36 for the simulation of the temperature T and phase fields  with the thermo-elastic theory, where the constitutive relations…”
Section: Large Loops Lying On (001) Planes With Burgers Vector Parallmentioning
confidence: 99%
“…As a consequence, the damage initialization corresponds to a space dependent cluster size distributions of I and V type aggregates, where the total defects dose stored in cluster of size N ≥ 2 is reduced to the ∼10% of the total dose estimated by means of TRIM simulation due to the dynamic annealing [15]. However, we note that the simulation results shown here are not qualitatively affected by the particular initial choice of the cluster size distribution [13]. The SIMS as implanted P profile is used to initialize the impurity in the simulation.…”
Section: S(xt)=e Las P(t)(1-r)αexp(-αx)mentioning
confidence: 85%