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Electric Field of 1 V/m is applied to a Boron doped Silicon semiconductor slab having a doping density of 1016 atoms/cm3 at 300 K temperature. Determine the approximate resistivity of the slab.
(Consider intrinsic carrier concentration of Silicon at 300 K = 1.5 × 1010 /cm3; Hole Mobility = 500 cm2/Vs at 300 K; Electron Mobility = 1300 cm2/Vs at 300 K).
  • a)
    0.48 Ω - cm
  • b)
    0.35 Ω - cm
  • c)
    0.16 Ω - cm
  • d)
    1.25 Ω - cm
Correct answer is option 'D'. Can you explain this answer?
Verified Answer
Electric Field of 1 V/m is applied to a Boron doped Silicon semiconduc...
Concept:
For a semiconductor slab doped with excess carriers and placed in an electric field, the current equation is given by:-
J = σ E
Where J = Current Density
σ = Conductivity of the semiconductor defined as:
σ = qnμn + qpμp
n = excess electrons contributing to the current conduction.
p = excess holes contributing to the current conduction.
Also, the Resistivity is defined as the reciprocal of conductivity.
Calculation:
The given Si semiconductor is doped with Boron impurity.
So, Na = 1016 /cm(p-type)
q = 1.6 × 10-19 C
μn = 1300 cm2/V-s and μp = 500 cm2/V-s
The excess electrons is given by; 
Since, Na ≫ ni, we can assume that the conduction current exists only because of acceptor impunities, i.e. because of Na.
So, σ = q Na μp
ρ = Resistivity of the given Slab
Putting on the respective values, we get:
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Most Upvoted Answer
Electric Field of 1 V/m is applied to a Boron doped Silicon semiconduc...
Concept:
For a semiconductor slab doped with excess carriers and placed in an electric field, the current equation is given by:-
J = σ E
Where J = Current Density
σ = Conductivity of the semiconductor defined as:
σ = qnμn + qpμp
n = excess electrons contributing to the current conduction.
p = excess holes contributing to the current conduction.
Also, the Resistivity is defined as the reciprocal of conductivity.
Calculation:
The given Si semiconductor is doped with Boron impurity.
So, Na = 1016 /cm(p-type)
q = 1.6 × 10-19 C
μn = 1300 cm2/V-s and μp = 500 cm2/V-s
The excess electrons is given by; 
Since, Na ≫ ni, we can assume that the conduction current exists only because of acceptor impunities, i.e. because of Na.
So, σ = q Na μp
ρ = Resistivity of the given Slab
Putting on the respective values, we get:
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Community Answer
Electric Field of 1 V/m is applied to a Boron doped Silicon semiconduc...
X 10^10 cm^-3)

First, we need to calculate the electron and hole concentration in the Boron doped Silicon slab. Since the slab is doped with Boron, it will act as a p-type semiconductor.

Given:
Doping density = 10^16 atoms/cm^3
Intrinsic carrier concentration of Silicon at 300 K = 1.5 x 10^10 cm^-3

Since the slab is p-type, the majority carrier concentration (holes) is equal to the doping density:
p = 10^16 cm^-3

The minority carrier concentration (electrons) can be calculated using the law of mass action:
n_i^2 = p*n
n = n_i^2 / p
n = (1.5 x 10^10)^2 / 10^16
n ≈ 2.25 x 10^4 cm^-3

Now, we can calculate the resistivity of the Boron doped Silicon slab using the formula:
ρ = 1 / (q * μ * (p + n))
where,
q = 1.6 x 10^-19 C (charge of an electron)
μ = 1300 cm^2/Vs (mobility of electrons in Silicon at 300 K)
p = 10^16 cm^-3 (majority carrier concentration - holes)
n = 2.25 x 10^4 cm^-3 (minority carrier concentration - electrons)

ρ = 1 / (1.6 x 10^-19 * 1300 * (10^16 + 2.25 x 10^4))
ρ ≈ 6.1 x 10^-3 Ω-cm

Therefore, the approximate resistivity of the Boron doped Silicon slab is 6.1 x 10^-3 Ω-cm.
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