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\rm \sum\limits_{ {n}=0}^(\infty) \frac{1}{(2 {n}^(2) + 3 n + 1) n!} \\

User Ali Moghadam
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1 Answer

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20 votes

Factorize the denominator:

2n² + 3n + 1 = (2n + 1) (n + 1)

Expand the summand into partial fractions:


\frac1{2n^2+3n+1} = \frac2{2n+1} - \frac1{n+1}

Then the sum is


\displaystyle \sum_(n=0)^\infty \frac2{(2n+1)n!} - \sum_(n=0)^\infty \frac1{(n+1)n!}

(by the way, you can use \displaystyle to make things like fractions, limits, or sums/integrals render the "right" way)

Recall that for all x,


\displaystyle e^x = \sum_(k=0)^\infty (x^k)/(k!)

Integrating both sides yields


\displaystyle e^x = C + \sum_(k=0)^\infty (x^(k+1))/((k+1)k!)

Taking x = 0 leads to C = e⁰ = 1. Move the constant to the left side and divide by x :


\displaystyle \frac{e^x - 1}x = \sum_(k=0)^\infty (x^k)/((k+1)k!)

Replacing x with x² in the series for eˣ gives


\displaystyle e^(x^2) = \sum_(k=0)^\infty (x^(2k))/(k!)

By the fundamental theorem of calculus,


\displaystyle \int_(x_0)^x e^(t^2) \, dt = C + \sum_(k=0)^\infty (x^(2k+1))/((2k+1)k!)

where x₀ is some constant. If we choose x₀ = 0, setting x = 0 elsewhere leads to C = 0.

Putting everything together, the series has a value of


\displaystyle \sum_(n=0)^\infty \frac1{(2n^2+3n+1)n!} = \boxed{2\int_0^1 e^(t^2) \, dt - (e-1)}

and you could write the integral in terms of the so-called error function,


\mathrm{erf}(z) = \displaystyle \frac2{\sqrt\pi} \int_0^z e^(-t^2) \, dt

or perhaps more appropriately, the imaginary error function,


\mathrm{erfi}(z) = \frac{\mathrm{erf}(iz)}i

User NorbertM
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