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Abel's summation formula

Integration by parts version of Abel's method for summation by parts

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Formula

Let (an)n=0∞ be a sequence of real or complex numbers. Define the partial sum function A by

A(t)=∑0≤n≤tan

for any real number t. Fix real numbers x<y, and let ϕ be a continuously differentiable function on [x,y]. Then:

∑x<n≤yanϕ(n)=A(y)ϕ(y)−A(x)ϕ(x)−∫xyA(u)ϕ′(u)du.

The formula is derived by applying integration by parts for a Riemann–Stieltjes integral to the functions A and ϕ.

Variations

Taking the left endpoint to be −1 gives the formula

∑0≤n≤xanϕ(n)=A(x)ϕ(x)−∫0xA(u)ϕ′(u)du.

If the sequence (an) is indexed starting at n=1, then we may formally define a0=0. The previous formula becomes

∑1≤n≤xanϕ(n)=A(x)ϕ(x)−∫1xA(u)ϕ′(u)du.

A common way to apply Abel's summation formula is to take the limit of one of these formulas as x→∞. The resulting formulas are

∑n=0∞anϕ(n)=limx→∞(A(x)ϕ(x))−∫0∞A(u)ϕ′(u)du,∑n=1∞anϕ(n)=limx→∞(A(x)ϕ(x))−∫1∞A(u)ϕ′(u)du.

These equations hold whenever both limits on the right-hand side exist and are finite.

A particularly useful case is the sequence an=1 for all n≥0. In this case, A(x)=⌊x+1⌋. For this sequence, Abel's summation formula simplifies to

∑0≤n≤xϕ(n)=⌊x+1⌋ϕ(x)−∫0x⌊u+1⌋ϕ′(u)du.

Similarly, for the sequence a0=0 and an=1 for all n≥1, the formula becomes

∑1≤n≤xϕ(n)=⌊x⌋ϕ(x)−∫1x⌊u⌋ϕ′(u)du.

Upon taking the limit as x→∞, we find

∑n=0∞ϕ(n)=limx→∞(⌊x+1⌋ϕ(x))−∫0∞⌊u+1⌋ϕ′(u)du,∑n=1∞ϕ(n)=limx→∞(⌊x⌋ϕ(x))−∫1∞⌊u⌋ϕ′(u)du,

assuming that both terms on the right-hand side exist and are finite.

Abel's summation formula can be generalized to the case where ϕ is only assumed to be continuous if the integral is interpreted as a Riemann–Stieltjes integral:

∑x<n≤yanϕ(n)=A(y)ϕ(y)−A(x)ϕ(x)−∫xyA(u)dϕ(u).

By taking ϕ to be the partial sum function associated to some sequence, this leads to the summation by parts formula.

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