For an times continuously differentiable function, Taylor's theorem gives
where lies between and . An infinite Taylor series represents the function when its remainder tends to zero; this holds locally for an analytic function, rather than for every smooth function automatically.
Integrate the geometric series for from zero to . The first three nonzero terms are
The resulting Taylor series converges for .
For fixed real , write the square root as and use the binomial series with exponent :
The absolute values are necessary for negative . This Taylor series is valid for . If , the quotient is for ; it has no continuous extension at zero and therefore has no Taylor expansion about zero.
Factor the Gaussian function as . Multiplying the two exponential series gives
For , its first three nonzero terms are
Vanishing coefficients require separate treatment in this Taylor expansion of a translated Gaussian. If , the first three nonzero terms are . If , they are
The latter expression retains the cubic term because the quadratic coefficient is zero.
Use the real logarithm near zero and subtract its two Taylor series:
Thus the first three nonzero terms are

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