A simplified picture of the periodic potential is given in Fig. 3.5
It is quite similar to the finite potential analysis
periodicity = a + b 
, where k is continuous
We will first consider the case: 0 < E < U 0
Inside well wave function = 
Outside well wave function = 
Schrödinger equation for 0 < x < a:

Schrödinger equation for -b < x < 0:

The general solutions to equations (1) and (2) are:



Now applying the continuity condition on wave function and its derivative at x = 0
Fig. 3.6
continuity requirement
Note that x = -b is the same boundary as that of x = a.
Now wave function and its derivative must observe Bloch Theorem
With
periodicity requirements.
Applying Boundary and Periodicity conditions
Eliminating and by using first two equations in last two equations
2 eqns in 2 unknown constants. For non trivial values of , the determinant formed from coefficient should be equal to zero.
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