How to solve steady state excess hole density

In summary: J)/qSubstituting the values for p and div(J) from parts a and b, we get:dp/dt = -(p0 - 1.5625*10^12)/2.5*10^-6 - (-1.1992*10^12)/1.6*10^-19 = -40*10^9 + 7.495*10^24 = 7.455*10^24Therefore, the rate of generation and recombination of electron-hole pairs at x=100μm is
  • #1
alex8214997
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Homework Statement



A hole current of 10^(-5) A/cm2 is injected into the side (x=0) of a long N-silicon. Assuming the holes flow only by diffusion and that at very large values of x, the distribution of excess holes decays to zero, Determine

a)The steady-state excess hole density at x=0
b)Hole current density at x=100μm
c)the rate of generation and recombination of electron-hole pair at x=100μm

Answers:
a)2.794*10^(10)cm-3
b) 1.667*10^(-6) A/cm2


Given:
J=10^(-5) A/cm2
μp=480 cm2/Vs
μn= 1350 cm2/Vs
lifetime of hole, τ=2.5μs


Homework Equations



J= -q*D*(dp/dx) D= k*T*μp/q

continuity equation:
dp/dt = -(p-p0)/τ- div(J)/q

where p: hole density; p0= hole density at equilibrium.
p-po=Δp

The Attempt at a Solution



dp/dx= J/(-q*D)= -5*10^(12)

I think Δp=p-p0=0 when t=τ=2.5μs
and Δp is at max. when t=0, and x=0

I tried to solve the continuity equation, which is 1 ODE

dp/dt = -(p-p0)/τ- div(J)/q
p'=p0/τ-p/τ-div(J)/q

p= p0-τ*div(J)/q+C*exp(-t/τ)

Since i think Δp=p-p0=0 when t=τ

p=p0-τ*div(J)/q+τ*e*div(J)/q*exp(-t/τ)


at t=0;
Δp=p-p0=τ*div(J)/q*(e-1)

but i can't find div(J)

b) i think J is constant, how it can be a function of x.
c) generation rate: p0/τ= (ni/τ)=4*10^(15)
recombination rate: Δp/τ= (p(x=100μm)-p0)/τ

 
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  • #2
=2*10^(-6)

Hello, thank you for your post. Based on the given information, here is my attempt at solving the problem:

a) The steady-state excess hole density at x=0 can be found by using the continuity equation, setting the time derivative equal to zero, and solving for p:

dp/dt = -(p-p0)/τ- div(J)/q = 0

Since at steady-state, dp/dt = 0, the equation becomes:

0 = -(p-p0)/τ- div(J)/q

Rearranging gives:

p = p0 - τ*div(J)/q

We can find div(J) by using Ohm's law and the fact that J = -q*D*(dp/dx):

div(J) = -q*D*(dp/dx) = -q*D*(-5*10^12) = 5*10^7 A/cm^3

Substituting this into the equation for p, we get:

p = p0 - (τ*5*10^7)/q = p0 - (2.5*10^-6*5*10^7)/1.6*10^-19 = p0 - 1.5625*10^12

Therefore, the steady-state excess hole density at x=0 is p = p0 - 1.5625*10^12.

b) The hole current density at x=100μm can be found by using Ohm's law and the fact that J = -q*D*(dp/dx):

J = -q*D*(dp/dx) = -q*D*(p-p0)/τ = -(1.6*10^-19*480*10^4*(p-p0))/2.5*10^-6 = -0.768(p-p0)

At x=100μm, p-p0 = Δp and we can use the answer from part a to find Δp:

Δp = p-p0 = p0 - (p0 - 1.5625*10^12) = 1.5625*10^12

Therefore, the hole current density at x=100μm is J = -0.768(1.5625*10^12) = -1.1992*10^12 A/cm^3.

c) The rate of generation and recombination of electron
 

1. What is steady state excess hole density?

Steady state excess hole density is the concentration of holes (positively charged particles) in a material at equilibrium, when the rate of hole generation is equal to the rate of hole recombination.

2. Why is it important to solve for steady state excess hole density?

Solving for steady state excess hole density is important in understanding the electrical properties of a material, such as its conductivity and resistivity. It also helps in optimizing the performance of electronic devices, such as solar cells and transistors.

3. What factors affect the steady state excess hole density?

The steady state excess hole density is influenced by the material's band gap, temperature, doping concentration, and the presence of defects or impurities. These factors affect the rate of hole generation and recombination, which ultimately determines the steady state excess hole density.

4. What methods can be used to solve for steady state excess hole density?

There are several methods used to solve for steady state excess hole density, including the continuity equation, the Shockley-Read-Hall recombination equation, and numerical simulations using software programs like MATLAB or TCAD.

5. How can the steady state excess hole density be experimentally measured?

The steady state excess hole density can be measured using techniques such as Hall effect measurements, capacitance-voltage measurements, and transient photocurrent measurements. These methods involve applying an external electric field or light to the material and measuring the resulting changes in electrical properties.

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