N-type and P-type Semiconductors Class 12 Notes | EduRev

Semiconductors are the materials that have a conductivity between conductors (generally metals) and non-conductors or insulators (such as ceramics). Semiconductors can be compounds such as gallium arsenide or pure elements, such as germanium or silicon. Physics explains the theories, properties and mathematical approach governing semiconductors.

Properties of Semiconductors

• Semiconducting elements are tetra-valent i.e. there are four electrons in their outermost orbit.
• Their lattice is face centered cubic (F.C.C.)
• The number of electrons or cotters is given by
  
  i.e. on increasing temperature, the number of current carriers increases.
• There are uncharged.
• Semiconductor acts like an insulator at Zero Kelvin. On increasing the temperature, it works as a conductor.
• Due to their exceptional electrical properties, semiconductors can be modified by doping to make semiconductor devices suitable for energy conversion, switches, and amplifiers.
• Lesser power losses.
• Semiconductors are smaller in size and possess less weight.
• Their resistivity is higher than conductors but lesser than insulators.
• The resistance of semiconductor materials decreases with the increase in temperature and vice-versa.

Example of different semi-conductors 

• Holes or cotters
  (i) The deficiency of electrons in covalent band formation in the valence band in defined as hole or cotter,
  (ii) These are positively charged. The value of positive charge on them is equal to the electron charge.
  (iii)  Their effective mass is less than that of electrons.
  (iv)  In an external electric field, holes move in a direction opposite to that of electrons i,e. they move from positive to negative terminal.
  (v)  They contribute to current flow.
  (vi)  Holes are produced when covalent bonds in valence band break.

Transfer of electrons from valence band to conduction band

Types of Semiconductor

Semiconductors can be classified as:

• Intrinsic Semiconductor
• Extrinsic Semiconductor

Intrinsic Semiconductor

• An intrinsic type of semiconductor material is made to be very pure chemically. It is made up of only a single type of element.

Conduction Mechanism in Case of Intrinsic Semiconductors (a) In absence of electric field (b) In presence of electric Field

• Germanium (Ge) and Silicon (Si) are the most common type of intrinsic semiconductor elements. They have four valence electrons (tetravalent). They are bound to the atom by covalent bond at absolute zero temperature.
• When the temperature rises, due to collisions, few electrons are unbounded and become free to move through the lattice, thus creating an absence in its original position (hole). These free electrons and holes contribute to the conduction of electricity in the semiconductor. The negative and positive charge carriers are equal in number.
• The thermal energy is capable of ionizing a few atoms in the lattice, and hence their conductivity is less.

➢ The Lattice of Pure Silicon Semiconductor at Different Temperatures

• At absolute zero Kelvin temperature: At this temperature, the covalent bonds are very strong and there are no free electrons and the semiconductor behaves as a perfect insulator.
• Above absolute temperature: With the increase in temperature few valence electrons jump into the conduction band and hence it behaves like a poor conductor.

➢ Energy Band Diagram of Intrinsic Semiconductor

• The energy band diagram of an intrinsic semiconductor is shown below:
  
  
  (a) Intrinsic Semiconductor at T = 0 Kelvin, behaves like an insulator (b) At t>0, four thermally generated electron pairs
• In intrinsic semiconductors, current flows due to the motion of free electrons as well as holes. The total current is the sum of the electron current Ie due to thermally generated electrons and the hole current Ih
  Total Current (I) = Ie + Ih
• For an intrinsic semiconductor, at finite temperature, the probability of electrons to exist in conduction band decreases exponentially with increasing bandgap (Eg)
  Where,
  E_g = Energy bandgap
  K_b = Boltzmann’s constants

Extrinsic Semiconductor

• The conductivity of semiconductors can be greatly improved by introducing a small number of suitable replacement atoms called impurities.
  
• The process of adding impurity atoms to the pure semiconductor is called doping. 
• Usually, only 1 atom in 107 is replaced by a dopant atom in the doped semiconductor. 
• An extrinsic semiconductor can be further classified into:
  (i) N-type Semiconductor
  (ii) P-type Semiconductor

Table: Difference between intrinsic and extrinsic semiconductors

➢ Properties of Extrinsic Semiconductors

• At absolute zero temperature (0 K) there are no free electrons in them.
• At room temperature, the electron-hole pair in sufficient number are produced.
• Electric conduction takes place via both electrons and holes.
• The drift velocities of electrons and holes are different.
• The drift velocity of electrons (V_dn) is greater than that of holes (V_dp).
• The total current is I = I_n + J_p.
• In connecting wires the current flows only via electrons.
• The current density is given by:
  
  Where V_dn = drift velocity of electrons
  μ_n = mobility of electrons
  V_dp = drift velocity of holes
  μp = mobility of holes
• The electric conductivity is given by s = nq(m_n + m_p).
• Mobility of electron m_n = V_dn / E.
• Mobility of holes m_p = V_dp/E.
• At room temperature s_Ge > s_Si because n_Ge > n_Si 
  where n_Ge = 2.5' 10¹³/cm³ and n_Si = 1.4' 10¹⁰ /cm³.