Transient Scanning Electron Beam Annealing Methods Used to Study Diffusion and Defects in Implanted Silicon

1986 ◽  
Vol 71 ◽  
Author(s):  
Michael J. Hart ◽  
Alan G. R. Evans ◽  
Gehan A. J. Amaratunga

AbstractRapid thermal annealing of arsenic and boron difluoride implants, such as those used for source/drain regions in CMOS, has been carried out using a scanning electron beam annealer, as part of a study of transient diffusion effects. Three types of e-beam anneal have been performed, with peak temperatures in the range 900-1200°C; the normal isothermal e-beam anneals, together with sub-second fast anneals and ‘dual-pulse’ anneals, in which the sample undergoes an isothermal pre-anneal followed by rapid heating to the required anneal temperature in less than O.5s.The diffusion occuring during these anneal cycles has been modelled using SPS−1D, an implant and diffusion modelling program developed by one of the authors. This has been modified to incorporate simulated temperature vs. time cycles for the anneals. Results are presented applying the usual equilibrium clustering model, a transient point-defect enhancement to the diffusivity proposed recently by Fair and a new dynamic clustering model for arsenic. Good agreement with SIMS measurements is obtained using the dynamic clustering model, without recourse to a transient defect model.Defects remaining in diodes fabricated with the forementioned implants after these anneal cycles have been studied using DLTS techniques. Trap densities for the three types of e-beam anneal are comparable to those for furnace annealed diodes, as are the reverse leakage currents measured (typically 2–5nA for a 0.85mm2 diode at -5V).

1987 ◽  
Vol 92 ◽  
Author(s):  
Michael J. Hart ◽  
Alan G.R. Evans ◽  
Gehan A.J. Amaratunga ◽  
John L. Altrip

ABSTRACTScanning electron beam annealing techniques have been applied to the study of diffusion of implanted arsenic and boron difluoride. Electron beam anneals over the time range 0-180s (at Tmax), with peak temperatures in the range 1100-1200°C have been performed on uniformly implanted samples. Controlled slow cooling has been performed for some samples. Direct sample temperature measurements were made using a dual-colour pyrometer under control of a microcomputer, which provided data-logging and feedback control of temperature. The accurate temperature control achieved using this system is important for realistic diffusion modelling.Measurement of the resulting chemical and electrical dopant profiles, using SIMS, RBS and spreading resistance methodshas shown the presence of non-equilibrium diffusion at short times [6]. Channelling RBS studies used to investigate the activation and clustering behaviour of arsenic during the first stages of these very rapid anneals is reported.Modelling of the arsenic diffusion occuring for a range of implant doses subjected to these anneals has been performed,applying avariety of models, including a dynamic clustering model. This dynamic clustering model, based upon an equilibrium cluster model and a measured de-clustering rate, has been shown previously to give good agreementwith experiment. Forthese experiments, a modified de-clustering coefficient was needed to model the diffusion occuring for a wider range of arsenic implants. A solution of the Poisson equation for the internal electric field has also been incorporated.DLTS techniques have been used to study the defects remaining in diodes fabricated using these implagts andanneals. Trap densities of <5×1010cm−3 and leakages of <2×10−9 A.cm2 at −5V have been measured for the best devices, similar tothose observed for control furnace anneals.


1970 ◽  
Vol 17 (6) ◽  
pp. 450-457 ◽  
Author(s):  
S. Miyauchi ◽  
K. Tanaka ◽  
J.C. Russ

Optik ◽  
2016 ◽  
Vol 127 (17) ◽  
pp. 6978-6981 ◽  
Author(s):  
Hassan N. Al-Obaidi ◽  
Musatfa M. Abid ◽  
Wasan J. Kadhem

1987 ◽  
Vol 20 (7) ◽  
pp. 901-905 ◽  
Author(s):  
M J Hart ◽  
A G R Evans ◽  
N K Bartlett

2016 ◽  
Vol 7 (1) ◽  
Author(s):  
Atsufumi Hirohata ◽  
Yasuaki Yamamoto ◽  
Benedict A. Murphy ◽  
Andrew J. Vick

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