Conduction band, valence band and Fermi energy

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SUMMARY

The discussion focuses on the relationship between conduction band energy (E_c), valence band energy (E_v), and Fermi energy (E_f) in semiconductor physics. The probability equations for states in the valence band and conduction band are derived using the Boltzmann distribution, specifically the equations P_v and P_c. Participants clarify the conditions under which these probabilities are valid, particularly emphasizing the significance of the inequality E_f - E_v >> k_BT. The conversation also addresses potential errors in the original equations and the correct interpretation of occupancy probabilities.

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  • Understanding of semiconductor physics, specifically conduction and valence bands.
  • Familiarity with the Boltzmann distribution and its application in statistical mechanics.
  • Knowledge of Fermi energy and its significance in determining electron occupancy.
  • Basic proficiency in mathematical manipulation of exponential functions.
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  • Study the derivation of the Boltzmann distribution in the context of semiconductor theory.
  • Explore the implications of Fermi-Dirac statistics on electron occupancy in semiconductors.
  • Investigate the effects of temperature on the occupancy probabilities of conduction and valence bands.
  • Learn about equilibrium conditions in semiconductors and how to mathematically express charge neutrality.
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Pushoam
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Homework Statement


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Homework Equations

The Attempt at a Solution



The probability of getting a state with energy ## E_v## is ## \frac { N_v } { N_v +N_c } = \frac1{ e^{-(E_v – E_f)/k_BT} +1} ## ………….(1)

Since, ## E_v < E_f, e^{-(E_v – E_f)/k_BT}>>1 ## as ## E_f – E_v>> k_BT ##……….(2)

So, ## \frac { N_v } { N_v +N_c } = \frac1{ e^{-(E_v – E_f)/k_BT} } ## ……….(3)

Similarly, probability of getting a state with energy ## E_c## is ## \frac { N_c} { N_v +N_c } = \frac1{ e^{-(E_c – E_f)/k_BT} +1} ##...(4)

Dividing (1) by (4) gives,

## \frac { N_v } {N_c } =## ## \frac{ e^{-(E_c – E_f)/k_BT} +1}{ e^{-(E_v – E_f)/k_BT} } ## ## = \frac{ e^{-(E_c – E_f)/k_BT} }{ e^{-(E_v – E_f)/k_BT} } ##

## k_BT \ln \frac { N_v } {N_c } = -(E_c – E_f) +(E_v – E_f) =E_v – E_c ##

Is this correct?
 

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Correct or not, it's not an answer to the question.
And why do you say e-(Ec-Ef)/kT + 1 = e-(Ec-Ef)/kT ?
 
mjc123 said:
Correct or not, it's not an answer to the question.
I meant : Is this correct so far?
As I doubted the correctness of what I had done in the original post.
 
mjc123 said:
And why do you say e-(##E_c-E_f##)/kT + 1 = e-(##E_c-E_f##)/kT ?
I said about ##E_v##, not ##E_c##.
According to the question, ##E_f - E_v >>k_B T##. So, ##exp\{(E_f - E_v )/k_BT \}>> 1 ##.
Hence, ignoring 1 to make calculation simple,##exp\{(E_f - E_v )/k_BT\} +1 \approx exp\{(E_f - E_v )/k_BT\}##.
 
But you say it implicitly in the penultimate line of your calculation.
 
mjc123 said:
But you say it implicitly in the penultimate line of your calculation.
It is said implicitly in eqn(2).
 
I need to know whether my approach so far is correct. So, please help me here.
 
Pushoam said:
It is said implicitly in eqn(2).
No, that's Ev. I'm talking about Ec. Look at the line after "dividing 1 by 4 gives"
I have my suspicions that the question is not correct. The formula gives Pv << 1, which does not look sensible. Should the minus sign before (E-Ef)/kT be a plus sign?
 
OK, I've had a closer look at it. It should be a plus sign in that expression, i.e. P = 1/(e(E-Ef)/kT +1). This is not the "probability of getting a state", but the probability of an individual state being occupied. It is not a function of Nc and Nv.
Now take the statement that at equilibrium the number of electrons in the conduction band is equal to the number of holes in the valence band. How would you express that mathematically in terms of the quantities you are given?
 

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