Consider the Taylor expansion centered around $x_0 = 0$ for $$f(x) = e^{x-1 + \sqrt{x^2+1}} ~,\qquad x\in\mathbb{R}$$
The goal is to arrive at $\sum c_k x^k$ by hand, and I wonder if there is an efficient way to obtain the coefficients of each power $x^k$ directly?
Below are examples of three approaches I know of, which are NOT efficient because they involve cumbersome combinatorial identities or further rearrangements that are too complicated (to me).
Take the whole exponent into the formula $e^z = \sum z^k / k!$ where $z = x-1 + \sqrt{x^2+1}$
Split the exponent into two so that $\displaystyle f(x) = \left( \sum \frac{ z_1^k }{ k! }\right) \left( \sum \frac{ z_2^m }{ m! }\right)$ where $z_1 = x-1$ and $z_2 = \sqrt{x^2-1}$.
Back to the definition of Taylor expansion $f(x) = \sum (x - x_0)^k f^{(k)}(x_0)\, /\, k!$ and do the derivatives with chain rules, for every order.
Note that wherever $\sqrt{x^2 + 1}$ appears, it has to be expanded into power series $1 + \frac12 x^2 - \frac18 x^4 + \ldots$ sooner or later to yield the final result in the desired form $f(x) = \sum x^k / k!$
I consider these calculations as indirect because the procedure itself by definition doesn't yield $c_k$ "directly", and one has to go through more rearrangements that are error prone.
When one wants only the first few terms, these might be okay, but when it comes to exact expressions (in summations), I personally don't find them to be practical.
There are many posts on this site pertaining to finding series expansion of various functions. However, so far what I've seen are all "indirect" methods like described above. For example, this post.
One can always throw the expression to Wolfram Alpha if one cares only about the result. However, sometimes one needs the exact expression for some further steps of proving etc, that is, doing the analysis based on the series.
Thank you for your time.
I'm trying to provide another way to do it, but I cannot say it is efficient enough.
Let $$f(x)=e^{x-1+\sqrt{x^2+1}}=\sum_{k=0}^\infty a_k x^k=a_0+a_1x+a_2x^2+\cdots$$ as usual. Since $$\dfrac d{dx}e^{x-1+\sqrt{x^2+1}}=\bigg(1+\dfrac x{\sqrt{x^2+1}}\bigg)e^{x-1+\sqrt{x^2+1}}=\sum_{k=0}^\infty(k+1)a_{k+1}x^k$$ We have $$\frac{x}{\sqrt{x^2+1}}e^{x-1+\sqrt{x^2+1}}=\sum_{k=0}^\infty [(k+1)a_{k+1}-a_k]x^k$$ Turning back to Taylor series aspect, since when $x=0$, we have $f(0)=1$ and $f'(0)=1$, hence $a_0=a_1=1$, then we can write $$\dfrac{x}{\sqrt{x^2+1}}f(x)=\sum_{k=1}^\infty [(k+1)a_{k+1}-a_k]x^k$$ By shifting the index we have $$\sum_{k=0}^\infty a_kx^k=\sqrt{x^2+1}\sum_{k=0}^\infty[(k+2)a_{k+2}-a_{k+1}]x^k$$ By using the Binomial expansion of $\sqrt{x^2+1}$ and solving some simultaneous equation system, we can solve up to $a_n$ for any natural number $n$, despite you would required to have a powerful brain or computer.