I am having trouble understanding these indices, and exactly what this is saying. I learned the multivariable Taylor series from Lang and it is presented in completely different manner. The highest he displays in this sort of format is of order 2, and he displays some order 3 terms using $D_i$ type notation. The second order terms and beyond is where I'm getting lost.
Could someone point me to a source so that I can unravel this formula and really interpret it, or perhaps explain it? If you were to explain it could you please give examples. Perhaps this can be translated into this form, $((H \cdot \nabla)^rf)(p)$ or vice versa.
This is paraphrased from a book which drops this out on page 4, page three being the introductory paragraphs. Reading onward it is not really explained, and I assume assumed that the reader understand all of it. I typed the formula exactly as it appears. This is from Tu's, An Introduction to Manifolds.
"The function f $\ldots$ it's Taylor series at p: $$f(x) = f(p) + \sum_{i} \frac{\partial f}{\partial x^{i}} (p) (x^{i}-p^{i}) + \frac{1}{2!}\sum_{i,j} \frac{\partial^2 f}{\partial x^{i} \partial x^{j}}(p)(x^i-p^i)(x^j-p^j) \\+ \cdots +\frac{1}{k!}\sum_{i_1, \ldots, i_k} \frac{\partial^k f}{\partial x^{i_1} \cdots \partial x^{i_k}}(p)(x^{i_1}-p^{i_1}) \cdots (x^{i_k}-p^{i_k})+ \cdots,$$ in which the general term is summed over all $ 1 \le i_1, \ldots i_k, \le n.$"
Thank you for your time.