1986
DOI: 10.1002/pssa.2210970132
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Optical beam induced minority carrier distribution in semiconductors

Abstract: The three‐dimensional distribution of minority carriers is calculated in a semi‐infinite semiconductor with arbitrary surface recombination. The optical probe is modelled as an exponentially decaying Gaussian so that the effects of a finite probe width may be considered. The reliability of the infinite diffusion length limit is shown to depend on the surface recombination velocity.

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Cited by 20 publications
(5 citation statements)
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“…Optical coordinates have also been introduced, given by where sin ϑ is the numerical aperture of the objective lens. The time-resolved PMC signals will now be found to be proportional to a volume integral over the minority carrier concentration, say N , given by The symmetry of the problem suggests that we may use the Fourier−Bessel transform of n ( r , z ) to solve the problem. , Accordingly The continuity equation now bocomes, in terms of ñ , where κ 2 = D n ν 2 + 1/τ. It is important to note that the boundary conditions that applied to n of eq 29 viz…”
Section: Model and Analysis Of The Effects Of Focusingmentioning
confidence: 99%
See 1 more Smart Citation
“…Optical coordinates have also been introduced, given by where sin ϑ is the numerical aperture of the objective lens. The time-resolved PMC signals will now be found to be proportional to a volume integral over the minority carrier concentration, say N , given by The symmetry of the problem suggests that we may use the Fourier−Bessel transform of n ( r , z ) to solve the problem. , Accordingly The continuity equation now bocomes, in terms of ñ , where κ 2 = D n ν 2 + 1/τ. It is important to note that the boundary conditions that applied to n of eq 29 viz…”
Section: Model and Analysis Of The Effects Of Focusingmentioning
confidence: 99%
“…The time-resolved PMC signals will now be found to be proportional to a volume integral over the minority carrier concentration, say N, given by The symmetry of the problem suggests that we may use the Fourier-Bessel transform of n(r,z) to solve the problem. 12,13 Accordingly…”
Section: Model and Analysis Of The Effects Of Focusingmentioning
confidence: 99%
“…The symmetry of our problem suggests that the solution is most easily obtained in a cylindrical coordinate system [19]. It will be useful to introduce the Fourier-Bessel…”
Section: The Photoluminescence Image Of a Defectmentioning
confidence: 99%
“…It has already been shown [20] that the presence of a point like defect may be taken into account, to the first Born approximation, by modifying the generation term to where the defect of strengthy is located a t (yo, a ) and po(r, z ) is the solution of (7) in the absence of the defect. An appropriate form for the optical generation function is [19] where go is a constant which takes into account the surface reflectivity, 01 is the intensity absorption coefficient and c is the half-width of the probe beam. We may find p(0, z ) most easily by taking the Fourier-Bessel transform of ( 7 ) with g(r, z ) replaced by g'(r, 2).…”
Section: The Photoluminescence Image Of a Defectmentioning
confidence: 99%
“…Schematic diagram of Schottky barrier 'ohmic coniaciThe cyclindrical symmetry[5,9] of the problem suggests that it may be most easily solved by introducing the Fourier-Bessel (or Hankel) transform of n(r, z , t ) defined as m G(v, z, t ) = J n(r, z, t ) Jo(vr) r dr ,…”
mentioning
confidence: 99%