Electron Devices: Chapter 1: Semiconductor

Equation of Charge Neutrality

Semiconductor

Questions: 1. Explain the equation of charge neutrality. 2. Important Example Solved Problems

Equation of Charge Neutrality

• Consider a semiconductor material which is doped with both type of impurities, donor as well as acceptor. The concentration of donor impurity is ND and that of acceptor impurity is NA.

• Each donor atom donates one electron and as it loses electron it becomes positively charged ion, due to the process of ionization.

• Thus assuming ionization of all the impurity atoms, the concentration of positive ions generated due to donor impurity becomes ND.

• There are positive charge carriers i.e. holes present in the material whose concentration is p.

• Thus the concentration of total positive charge in the material is given by,

Total positive charge concentration = ND + P            ……………(1)

• The acceptor impurity atom when added to the material accepts an electron and becomes negatively charged ion.

• Assuming ionization of all the impurity atoms, the concentration of negative ions generated due to acceptor impurity is NA.

• There are negative charge carriers i.e. electrons present in the material whose concentration is n.

• Thus the concentration of total negative charge in the material is given by,

Total negative charge concentration = NA + n                   ……………(2)

• The material as a whole is always electrically neutral hence the total positive charge concentration in the material must be equal to the total negative charge concentration in the material. Hence equating (1) and (2) we can write,

 ND + p = NA + n                …………..(3)

The equation (3) is called the equation of charge neutrality.

• Observations:

1. The equation is important when a semiconductor is doped with both the types of impurities, donor as well as acceptor.

2. The equation is effective in obtaining the actual concentrations of electrons and holes in a material which is doped with both the types of impurities.

3. The equation helps to determine whether the material doped with both the types of impurities will behave as n‒type or p‒type.

 

Ex. 1.15.1 In a sample of germanium at 300 °K, it is found that donor concentration is 2×1014 atoms/cm3 and acceptor concentration is 3× 1014 atoms/cm3.

Determine the actual concentrations of free electrons and holes in the sample. Will it behave as p‒type or n‒type? Assume ni at 300 °K = 2.5 × 1013 per cm3.

Solution:

In this sample,

 ND = 2×1014 atoms/cm3 = 2×1014 / 10‒6 = 2×1020 m3

 NA = 3×1014 atoms/cm3 = 3×1014 / 10‒6 = 3×1020 m3

Using equation of charge neutrality, p + ND = n + NA.

NA ‒ ND = p‒n

3×1020  ‒ 2×1020 = p‒n

i.e. p = n + 1×1020

where p and n are actual concentrations of holes and electrons.

 ni = 2.5×1013 per cm3

 = 2.5×1013 / 10‒6

= 2.5×1019 per cm3

According to law of mass action, np = ni2

 n (n + 1×1020) = (2.5 × 1019)2      i.e. n2 + 1×1020n − 6.25×1038 = 0

Solving

n = 5.901×1018 electrons/m3

p = 1.059×1020 holes/m3

 As holes are much more than electrons, sample will behave as p‒type.

 

Ex. 1.15.2 A sample of Ge is doped to the extent of 1014 donor atoms/cm3 and 7 × 1013 acceptor atoms/cm3. At the temperature of the sample, the resistivity of pure Ge is 60 ohm‒cm. If the applied electric field is 2 V/cm, find the total conduction current density.

Solution:

 ND = 1014/cm3 and NA =7×1013/cm3

 ρi = 60 Ω‒cm

 J = (nμn + Pμp) qE

   …….. μn = 3800, μp = 1800

According to law of electrical neutrality,

 ND + P = NA + n

i.e. n‒p = 3 × 1013

According to law of mass action, np =ni2

σi = ninp) q

i.e. 1/ρi = nin+ μp) q

1/60 = ni (3800 + 1800) × 1.6 × 10‒19

i.e. n=1.86 × 1013/cm3

Solve equations (1) and (2) to obtain n and p as,

n = 3.88×1013/cm3 and

p=0.88×1013/cm3

 J = (3.88 × 1013 × 3800 + 0.88 × 1013 × 1800) × 1.6 × 10‒19 × 2 = 0.0522 A/cm


Review Question

1. Explain the equation of charge neutrality.

 

Electron Devices: Chapter 1: Semiconductor : Tag: electronics : Semiconductor - Equation of Charge Neutrality


Electron Devices: Chapter 1: Semiconductor



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