Solving Quasi Fermi Levels: EHP Generation & Conductivity Change

In summary, to find the separation of the quasi Fermi level and the change of conductivity upon shining the light, you must first solve for ni using the given donor concentration. Then, use the quasi formulas to solve for Fn and Fp. The separation of the quasi Fermi level is the difference between Fn and Fp, and the change in conductivity is calculated using the relation Δσ=μn(nd)(Fn-Fp).
  • #1
EE_or_Bust
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Can someone please help with this problem. I've been looking at it for a week!
I can't figure out what equation to use.

A si sample with 10^15/cm^3 donors is uniformly optically excited at room temperature such that 10^19 EHPs (Electron Hole Pairs) are generated per second. Find the separation of the quasi Fermi level and the change of conductivity upon shinig the light. Electron and hole lifetimes are both 10μs. =12. {Hint: to find Fn-Fp , use the relation relating (np) and nd (ni, Fn, Fp). μn=1300[cm^2/ V-s].

I know that Fn and Fp are the quasi fermi electron and hole levels. And I know the common quasi formulas are
n=(ni)(e^-(ei-Fn)/KT)
p=(ni)(e^-(-Fp-Ei)/KT)

How do I use these equations to find the separation of the quasi fermi level?
 
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  • #2
First, use the given information to solve for ni. nd = 10^15/cm^3ni = (nd)^(1/2) = 10^7.5/cm^3Next, solve for the quasi-Fermi levels: Fn = Ei - KT ln (nd/ni) Fp = -Ei - KT ln (nd/ni) Substitute in the given information to solve for Fn and Fp: Fn = Ei -kt ln (10^15/10^7.5) = 0.026V Fp = -Ei -kt ln (10^15/10^7.5) = -0.026V The separation of the quasi Fermi level is then the difference between Fn and Fp, which is 0.052V. To find the change in conductivity upon shining the light, use the relation Δσ=μn(nd)(Fn-Fp)Substitute in the given information to solve for Δσ: Δσ = μn (10^15/cm^3) (0.052V) = 6.6 x 10^-13 (Ω-cm)^-1 Therefore, the separation of the quasi Fermi level is 0.052V and the change in conductivity upon shining the light is 6.6 x 10^-13 (Ω-cm)^-1.
 
  • #3


The separation of the quasi Fermi level can be found by using the relation between the electron and hole concentrations (n and p) and the intrinsic carrier concentration (ni). This relation is given by the equation:

np = ni^2 * e^( (Fn-Fp)/kT)

Where k is the Boltzmann constant and T is the temperature. This equation is known as the law of mass action and it describes the balance between the generation and recombination of electron-hole pairs in a semiconductor material.

To solve for the separation of the quasi Fermi level, we can rearrange this equation to:

Fn-Fp = kT * ln(np/ni^2)

Now, we can plug in the given values for n, p, and ni:

Fn-Fp = (8.62 x 10^-5 eV/K) * ln(10^19/10^30)

= (8.62 x 10^-5 eV/K) * ln(10^-11)

= (8.62 x 10^-5 eV/K) * (-25.8)

= -0.00222 eV

Therefore, the separation of the quasi Fermi level is -0.00222 eV.

To find the change in conductivity upon shining light, we can use the equation:

σ = q * μ * (n + p)

Where q is the elementary charge, μ is the carrier mobility, and n and p are the electron and hole concentrations.

We can find the change in conductivity by subtracting the initial conductivity (before shining light) from the final conductivity (after shining light). The initial conductivity can be calculated using the given donor concentration:

σ_initial = q * μ * (n + p)

= (1.6 x 10^-19 C) * (1300 cm^2/V-s) * (10^15/cm^3 + 0/cm^3)

= 2.08 x 10^-4 (Ω*m)^-1

The final conductivity can be calculated by adding the additional electron-hole pairs generated by the light:

σ_final = q * μ * (n + p + Δn + Δp)

= (1.6 x 10^-19 C) * (1300 cm^2/V-s) * (10^15/cm^3 + 10^19/cm^3)

= 2.08 x 10^-4 (Ω*m)^-1
 

1. What is the concept of quasi Fermi levels?

Quasi Fermi levels are energy levels that describe the distribution of charge carriers (electrons and holes) in a semiconductor material. They represent the average energy of the electrons and holes in a material and are used to calculate the probability of a carrier occupying a particular energy state.

2. How are quasi Fermi levels affected by EHP (electron-hole pair) generation?

EHP generation occurs when a photon of sufficient energy is absorbed by a semiconductor material, creating an electron-hole pair. This increases the number of carriers in the material, causing a shift in the quasi Fermi levels towards the direction of the excess carriers. The magnitude of this shift depends on the efficiency of EHP generation and the material properties.

3. How does conductivity change with changes in quasi Fermi levels?

Conductivity is directly related to the number of charge carriers in a material, which in turn is affected by the quasi Fermi levels. As the levels shift, the number of carriers also changes, leading to a change in conductivity. Higher quasi Fermi levels result in increased conductivity and vice versa.

4. What factors influence the magnitude of the change in quasi Fermi levels?

The magnitude of the change in quasi Fermi levels depends on several factors, including the material's bandgap, the efficiency of EHP generation, and the rate of recombination of carriers. Additionally, the presence of impurities and defects in the material can also affect the magnitude of the shift.

5. How can the concept of quasi Fermi levels be applied in practical applications?

The understanding of quasi Fermi levels is crucial in various semiconductor devices such as solar cells, photodetectors, and transistors. By controlling the quasi Fermi levels, the performance of these devices can be optimized for specific applications. Additionally, the concept is also used in photovoltaic research to study the efficiency of different materials in converting solar energy into electricity.

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