Silicon Junction Diode: Charge Density and Potential Analysis

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SUMMARY

The discussion focuses on the analysis of charge density and electric potential in a silicon junction diode, specifically between n-type and p-type semiconductors. The potential difference between the two regions is established as 0.3 V, with charge slabs of thickness 10^-4 m. The relationship between potential and charge density is defined using the equation involving the second derivative of potential, σ/ε. The user successfully derived expressions for the potential in both regions and determined that B equals 0.15 through substitution and boundary conditions.

PREREQUISITES
  • Understanding of semiconductor physics, specifically n-type and p-type materials.
  • Familiarity with electric potential and electric field concepts.
  • Knowledge of differential equations and boundary value problems.
  • Proficiency in using the relationship between charge density and electric potential (σ/ε).
NEXT STEPS
  • Explore the derivation of electric field strength in semiconductor junctions.
  • Study the impact of varying charge densities on potential distribution in diodes.
  • Learn about the graphical representation of electric potential and electric field in semiconductor devices.
  • Investigate the role of boundary conditions in solving differential equations in physics.
USEFUL FOR

Students and professionals in electrical engineering, semiconductor physics, and anyone involved in the design and analysis of diode circuits.

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Homework Statement



In a silicon junction diode, the region of the planar junction between n-type and p-type
semiconductors can be approximately represented as two adjoining slabs of charge, one
negative and one positive. Away from the junction, outside these charge layers, the
potential is constant, with a value of Vn in the n-type material and Vp in the p-type
material. Given that the difference between Vp and Vn is 0.3 V, and that the thickness
of each of the two slabs of charge is 10^-4 m, find the charge density in each of the
two slabs, and make a graph of the potential V as a function of position through the
junction. What is the strength of the electric field at the midplane?


Homework Equations



I using the relationship that the second derivative of the potential is equal to σ/ε.
I have certain conditions. Putting the middle of the bar at x=0, the potential must be continuous through the middle and I have conditions set at the endpoints

phi_1(-10^-4)=0
phi_2(10^-4)=.3
phi_1(0)=phi_2(0)
σ1+σ2 = 0

The Attempt at a Solution



I get two expressions

phi_1(x)= σ1/(2ε)x^2+Ax + B
phi_2(x) = σ2/(2ε)x^2+Cx+D

I found that A=C and B=D using the conditions, but now I have too many unknowns and not enough equations.
 
Physics news on Phys.org
Update 1. Found that B = .15
by substituting σ1 for -σ2 and plugging in the values of 10^-4 and -10^-4 into the respective equations and added them.
 

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