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1 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
1 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
ENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICS
Mr. Gouri Kumar Sahu
Senior Lecturer in Physics
C.U. T. M.
2 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
2 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
SESSION-7
7.1 Band theory of solids
In a single free atom, the energy levels of electrons are well defined
In crystals the atoms do not have well defined energy levels, as in crystal
there are large number of atoms, interaction takes place between
neighboring levels which will modify the energy levels.
consider the case of silicon atom
Atomic number 14
configuration 1s2., 2s2, 2p6, 3s2, 3p2.
The outer most shell containing
4 electrons and 4 vacant spaces.
3 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
3 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
SESSION-7
7.1 Band theory of solids
Suppose interatomic separation between the silicon atoms = ‘a’
Let the atoms are brought from locations r>>a to their actual location
[a] When r=d1; energy levels are well defined
[b]When r=d2: Splitting of energy level takes place.
The 2N s level will not have same
energy but will spread in a small
energy band, similarly 6N p levels
will split into energy band,.
4 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
4 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
SESSION-7
7.1 Band theory of solids
[c] When r=d3 , Energy gap between 3s and 3p level completely disappears
and all 8N levels are continuously distributed in an energy band.
There are 8N energy levels with 4N levels filled and 4N levels empty.
[d] When r=a =actual interatomic
separation a, the 8N levels splits
into 2 bands, the 4N filled energy
level forming valance band and
the 4N empty energy levels
forming conduction band.
The energy difference between valance and conduction band is called
forbidden energy gap.
5 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
5 ENGINEERING PHYSICS
Mr. Gouri Kumar Sahu
Sr. Lecturer in Physics.
END OF SESSION -7
SESSION-7
THANK YOU

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Engineering physics 6(Band theory of solids)

  • 1. 1 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. 1 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. ENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICSENGINERING PHYSICS Mr. Gouri Kumar Sahu Senior Lecturer in Physics C.U. T. M.
  • 2. 2 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. 2 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. SESSION-7 7.1 Band theory of solids In a single free atom, the energy levels of electrons are well defined In crystals the atoms do not have well defined energy levels, as in crystal there are large number of atoms, interaction takes place between neighboring levels which will modify the energy levels. consider the case of silicon atom Atomic number 14 configuration 1s2., 2s2, 2p6, 3s2, 3p2. The outer most shell containing 4 electrons and 4 vacant spaces.
  • 3. 3 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. 3 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. SESSION-7 7.1 Band theory of solids Suppose interatomic separation between the silicon atoms = ‘a’ Let the atoms are brought from locations r>>a to their actual location [a] When r=d1; energy levels are well defined [b]When r=d2: Splitting of energy level takes place. The 2N s level will not have same energy but will spread in a small energy band, similarly 6N p levels will split into energy band,.
  • 4. 4 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. 4 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. SESSION-7 7.1 Band theory of solids [c] When r=d3 , Energy gap between 3s and 3p level completely disappears and all 8N levels are continuously distributed in an energy band. There are 8N energy levels with 4N levels filled and 4N levels empty. [d] When r=a =actual interatomic separation a, the 8N levels splits into 2 bands, the 4N filled energy level forming valance band and the 4N empty energy levels forming conduction band. The energy difference between valance and conduction band is called forbidden energy gap.
  • 5. 5 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. 5 ENGINEERING PHYSICS Mr. Gouri Kumar Sahu Sr. Lecturer in Physics. END OF SESSION -7 SESSION-7 THANK YOU