Suppose we take two measurements for each of the $n$ subjects, where each subject is independent of one another. Let $X_i$ and $Y_i$ denote these measurements for $i=1, \cdots, n$. Let $Z_i = Y_i - X_i$ and let $R_i$ denote the rank of $|Z_i|$. Assume that there are no ties.
The Wilcoxon signed-rank test statistic is defined as $T = \mbox{min}(T^{+}, T^{-})$. Since we have assumed no ties, $T^{-} = n(n+1)/2 - T^{+}$. Clearly, the variance of $T$ equals the variance of $T^{+}$ since $T^{-}$ is the difference of $T^{+}$ and a constant. The expectation of $T$ can also be shown to equal the expectation of $T^{+}$ under the null hypothesis.
For these types of problems, assumptions about the test statistic under the null hypothesis are not as illuminating as writing the test statistic as a function of random variables. Since the two populations are identical under the null hypothesis and no ties are allowed, we can treat the ranks $R_1, \cdots, R_n$ as known, but the signs of $Z_1, \cdots, Z_n$ as unknown. Let $\psi_i = \mbox{I} \left[Z_i > 0\right]$, where $\mbox{I} \left[\cdot \right]$ denotes the indicator function. Then we may write $T^{+} = \sum_{i=1}^n R_i \psi_i$. Under the null hypothesis, $\psi_i \sim Bernoulli(.5)$. Hence,
\begin{eqnarray*}
\mbox{E} \left[T^{+}\right] &=& \mbox{E} \left[\sum_{i=1}^n R_i \psi_i\right] \\
&=& \sum_{i=1}^n R_i \mbox{E} \left[\psi_i\right] \\
&=& \frac{1}{2} \sum_{i=1}^n i \\
&=& \frac{n(n+1)}{4}.
\end{eqnarray*}
Likewise, the variance of $T^{+}$ is
\begin{eqnarray*}
\mbox{Var} \left[T^{+}\right] &=& \mbox{Var} \left[\sum_{i=1}^n R_i \psi_i\right] \\
&=& \sum_{i=1}^n R_i^2 \mbox{Var} \left[\psi_i\right] \\
&=& \frac{1}{4}\sum_{i=1}^n i^2 \\
&=& \frac{n(n+1)(2n+1)}{24}.
\end{eqnarray*}
Now your reasoning about the second raw moment of $T$, equivalently $T^{+}$, is incorrect. Perhaps another could comment on where you went amiss with your reasoning, but as I have stated it is important to write your test statistic as a function of random variables to avoid such mistakes. The correct derivation of the second moment is as follows
\begin{eqnarray*}
\mbox{E} \left[\left(T^{+}\right)^2\right] &=& \mbox{E} \left[\left(\sum_{i=1}^n R_i \psi_i\right)^2\right] \\
&=& \sum_{i=1}^n R_i^2 \mbox{E}\left[\psi_i^2\right] + \sum_{i=1}^n \sum_{\substack{j=1 \\ j \ne i}}^n R_i R_j \mbox{E} \left[\psi_i \psi_j \right] \\
&=& \frac{1}{2}\sum_{i=1}^n i^2 + \frac{1}{4} \sum_{i=1}^n \sum_{\substack{j=1 \\ j \ne i}}^n ij \\
&=& \frac{1}{2}\sum_{i=1}^n i^2 + \frac{1}{4} \sum_{i=1}^n i \left[\frac{n(n+1)}{2} - i\right] \\
&=& \frac{n(n+1)(2n+1)}{12} + \frac{n^2(n+1)^2}{16} - \frac{n(n+1)(2n+1)}{24} \\
&=& \frac{n(n+1)(n+2)(3n+1)}{48}.
\end{eqnarray*}