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Show that Eq. 41-5 can be written as N(E)=CE1/2. (b) Evaluatein terms of meters and electron-volts. (c) CalculateN(E)forE=5.00eV for .

Short Answer

Expert verified
  1. The density of the states of conduction electrons is NE=CE1/2.
  2. The value of the constant in meters and electron-volts is 6.81×1027m-3.eV-2/3.
  3. The density of states for is E=5eVis1.52×1028eV-1.m-3.

Step by step solution

01

The given data

  1. The given energy value,E=5eV
02

Understanding the concept of density of states

Using the formula of the density of states associated with the conduction electrons of metal, we can get the required value of the density of the state for the given energy and constant values.

N(E)=82ττ³¾3/2h3E1/2

03

a) Calculation of the formula of density of states

From the given equation of density of states of the conduction electrons of a metal, we get thatNE=CE1/2....................a

where

C=82Ï€³¾3/2h3=82Ï€9.1×10-31kg3/26.63×10-34J.s3=1062×1056kg3/2J3.s3

Hence, the density of the states of conduction electrons is NE=CE1/2.

04

b) Calculation of the value of constant C in meters and electron-volts

We know that 1J=1kg.m2/s2

So, considering the equation of kinetic energy K=12mv2the unit of mass is 1kg=1J.s2m-2.

Thus, the units of C becomes-

J.s23/2.m-23/2.J-3.s-3=J-3/2m-3

Now, the value of C in meters and electron-volts can be given as:

C=1.062×1056kg3/2/J3.s31.602×10-19J/eV3/2=6.81×1027m-3.eV-2/3

Hence, the value of C is 6.81×1027m-3.eV-2/3.

05

c) Calculation of the density of states for the given energy

Using the given energy value in equation (a) of density in part (a), we can get the density of the states of the conduction electrons of the metal as follows:

NE=6.81×1027m-3.eV-2/35eV1/2=1.52×1028eV-1.m-3

Hence, the value of the density of electrons is 1.52×1028eV-1.m-3.

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Most popular questions from this chapter

(a) Using the result of Problem 23 and 7.00eVfor copper’s Fermi energy, determine how much energy would be released by the conduction electrons in a copper coin with mass3.10g if we could suddenly turn off the Pauli exclusion principle. (b) For how long would this amount of energy light a100 Wlamp? (Note: There is no way to turn off the Pauli principle!)

A silicon sample is doped with atoms having donor states 0.110eV below the bottom of the conduction band. (The energy gap in silicon is 1.11eV ) If each of these donor states is occupied with a probability of 5.00×10-5at T=300K, (a) is the Fermi level above or below the top of the silicon valence band and (b) how far above or below? (c) What then is the probability that a state at the bottom of the silicon conduction band is occupied?

In a simplified model of an undoped semiconductor, the actual distribution of energy states may be replaced by one in which there are NVstates in the valence band, all having the same energyEV, andNCstates in the conduction band all these states having the same energyEc. The number of electrons in the conduction band equals the number of holes in the valence band.

  1. Show that this last condition implies that Ncexp(∆Ec/kT)+1=Nvexp(∆Ev/kT)+1in which∆Ec=∆Ec-∆EF and ∆Ev=-(∆Ev-∆EF).
  2. If the Fermi level is in the gap between the two bands and its distance from each band is large relative to kT then the exponentials dominate in the denominators. Under these conditions, show that EF=(Ec+Ev)2+kTIn(Nv+Nc)2and that ifNv≈Nc , the Fermi level for the undoped semiconductor is close to the gap’s center.

Zinc is a bivalent metal. Calculate (a) the number density of conduction electrons, (b) the Fermi energy, (c) the Fermi speed, and (d) the de Broglie wavelength corresponding to this electron speed. See Appendix F for the needed data on zinc.

Calculate the density of states N(E)for metal at energy E=8.0eVand show that your result is consistent with the curve of Fig. 41-6.

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