16.8 Ballooning transformation

To construct a periodic function about πœƒ, we introduces a function z(πœƒ) which is defined over βˆ’βˆž < πœƒ < ∞ and vanishes sufficiently fast as |πœƒ|β†’βˆž so that the following infinite summation converge:

 βˆžβˆ‘  -
    z(πœƒ +2Ο€l).
l=βˆ’ ∞
(502)

If we use the above sum to define a function

       βˆžβˆ‘  -
z(πœƒ) =     z(πœƒ +2Ο€l),
      l=βˆ’ ∞
(503)

then it is obvious that

z(πœƒ +2Ο€ ) = z(πœƒ),
(504)

i.e., z(πœƒ) is a periodic function about πœƒ with period of 2Ο€.

If we use the right-hand-side of Eq. (503) to represent z(πœƒ), then we do not need to worry about the periodic property of z(πœƒ) (the periodic property is guaranteed by the representation)