2022
DOI: 10.24214/jcbps.c.12.4.25165
|View full text |Cite
|
Sign up to set email alerts
|

Optimization of the thickness of the doping rate base (Nb) of the (n+/p/p+) silicon solar cell with vertical multi-junctions connected in series and placed under monochromatic illumination in frequency modulation

Abstract: The silicon solar cell with vertical multi-junctions (MJV) connected in series, is studied under monochromatic illumination in frequency modulation, for different cases of doping rate of its base. The diffusion equation relating to the density of minority charge carriers in the base of the solar cell is solved, taking into account the dynamic coefficient of diffusion (D(ω,N_b)) related to the doping rate (Nb) and to the frequency (ω) of modulation, as well as recombination speeds (Sf) at the junction and (Sb) … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
5
0

Year Published

2022
2022
2023
2023

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 5 publications
(5 citation statements)
references
References 20 publications
(40 reference statements)
0
5
0
Order By: Relevance
“…In this interval of low frequencies, the relaxation time of the minority carriers is important (large values of D in Equation ( 5)), allowing a large distance of travel (Einstein relation). A large optimum thickness of the base is then obtained [43] [57] [58] (Figure 9). On the other hand, at high frequency values, the relaxation time (ωτ  1) of minority carriers is reduced, as well as the coefficient (Equation ( 5)) and the scattering length (Equation ( 9)) of minorities corresponding to a short travel distance, then the optimum thickness [57] [58] of the base needed to collect the charge carriers is small, regardless of the temperature.…”
Section: Discussionmentioning
confidence: 99%
“…In this interval of low frequencies, the relaxation time of the minority carriers is important (large values of D in Equation ( 5)), allowing a large distance of travel (Einstein relation). A large optimum thickness of the base is then obtained [43] [57] [58] (Figure 9). On the other hand, at high frequency values, the relaxation time (ωτ  1) of minority carriers is reduced, as well as the coefficient (Equation ( 5)) and the scattering length (Equation ( 9)) of minorities corresponding to a short travel distance, then the optimum thickness [57] [58] of the base needed to collect the charge carriers is small, regardless of the temperature.…”
Section: Discussionmentioning
confidence: 99%
“…Previous works have plotted dynamic diffusion coefficient [14,15,[38][39][40][41][42] of minority carriers in the base of the solar cell (Eq. 7).…”
Section: Ac Diffusion Coefficient and Frequency Domainsmentioning
confidence: 99%
“…In figure 6 the optimum thickness of the base increases versus the diffusion coefficient D(ω, T) whatever the zones of modulation frequency [17,18,42] , as expressed in (Eq. 7).…”
Section: Ac Photocurrent Density and Ac Back Surface Recombinationmentioning
confidence: 99%
“…[36][37][38][39] of graphical determination of the optimum base thickness (Hopt) of solar cells. Solar cells are, either horizontally illuminated by (n+), or vertically illuminated over all the different regions of the solar cell [40,41] . Expressions of (Sb1V), (Sb2 recombination velocity (Sb2H) gives the optimum thickness (Hopt) for the conventional solar cell.…”
Section: Composite Ac Back Surface Recombination Velocity Determinationmentioning
confidence: 99%
“…The use of light frequency modulation [37][38][39][40] makes it possible to influence minority charge carriers' recombination parameters in the bulk (diffusion length L(ω) and diffusion coefficient D(ω) ) and on the back surface. Then several cases of solar cells are observed according to the conditions of regimes, static (ωτ <<1) and dynamic (ωτ >>1).…”
Section: (I)for Low Frequencymentioning
confidence: 99%