Summation by parts

The summation by parts is the equivalent for the series of the Intégration by parts. It is also called transformation of Abel or summation of Abel .

Method

Are two continuations (a_n) \, and (b_n) \, , with n \ in \ N. The following series is considered:
S_N = \ sum_ {n=0} ^N a_n b_n

If one poses B_n = \ sum_ {k=0} ^n b_k,
then for all n>0, b_n = B_n - B_ {n-1} \,

S_N = a_0 b_0 + \ sum_ {n=1} ^N a_n (B_n - B_ {n-1})
S_N = a_0 b_0 - a_1 B_0 + a_N B_N + \ sum_ {n=1} ^ {N-1} B_n (a_n - a_ {n+1})
One obtains finally the following equality: S_N = a_N B_N - \ sum_ {n=0} ^ {N-1} B_n (a_ {n+1} - a_n)

This operation, which transforms the expression of the series to be studied, is useful to prove certain criteria of convergence of S_N \, .

Similarity with integration by parts

The formula of integration is written: \ int_a^b F (X) g' (X) \, dx = \ left F (X) G (X) \ right_ {has} ^ {B} - \ int_a^b f' (X) G (X) \, dx
If one leaves side the boundary conditions, one realizes that integration by parts consists in integrating one of the two functions present in the initial integral (g' \, becomes g \, ) and to derive the other (f \, becomes f' \, ).

The summation by parts consists of a similar operation in the discrete field, since one of the two series is summoned (b_n \, becomes B_n \, ) and the other is differentiated (a_n \, becomes a_ {n+1} - a_n \, ).

Applications

One places oneself thereafter if a_N b_N \ rightarrow 0, because if not one knows that (S_N) \, is trivialement divergent.

If (B_n) \, is limited by a reality M and that \ sum_ {k=0} ^N (a_ {n+1} - a_n) is an absolutely convergent series , then the series (S_N) \, is convergent.

|S_N| \ it |a_N B_N| + \ sum_ {n=0} ^ {N-1} |B_n| |a_ {n+1} - a_n|

The sum of the series checks the inequality in addition: S = \ sum_ {n=0} ^ \ infty a_n b_n \ the M \ sum_ {n=0} ^ \ infty |a_ {n+1} - a_n|

Examples

  1. a_n = \ frac {1} {n+1} and b_n = (- 1) ^n \,
    |B_n| \ the 1 and |a_ {n+1} - a_n| = \ frac {1} {(n+1) (n+2)} \ the \ frac {1} {n^2}
    On knows that the series \ sum_0^ \ infty \ frac {1} {n^2} converges (see Fonction zeta of Riemann), therefore the conditions mentioned above are all réunies.
    S = 1 - \ frac {1} {2} + \ frac {1} {3} - \ frac {1} {4} +… converge.
    NB: This example can also be proven thanks to the Critère of convergence of the alternate series.

  2. a_n = \ frac {1} {N} and b_n = \ sin (N) \,
    (We define here the sum only starting from the row n=1 instead of n=0, but that does not affect of anything the existence limit of the series.)
    Comme previously \ sum_ {n=1} ^ \ infty (\ frac {1} {n+1} - \ frac {1} {N}) converges absolutely, and \ sum_ {k=1} ^n \ sin (K) is limited according to the expression of the Noyau of Dirichlet.
    Consequently \ sum_ {n=1} ^ \ infty \ frac {\ sin (N)}{N} converges.
  3. the summation by parts is useful in the proof of the theorem of Abel.

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