Random Walk - expected distance from Origin I am looking for publications dealing with the expected Distance from Origin (not RMS mean) 
after a Random Walk in a 2 or 3 dimensional space (not latticed).
I would appreciate if anyone can point to some references to publications related to (or 
including) this subject.
 I am speaking about a Random Walk of N equal steps with random directions in a 2 dimensional
space (plane) or in a 3 dimensional (space). No lattice will restrict the possible locations 
after each step. The request is for references and not for the solution itself! Thanks.
 A: In an arbitrary dimension d:
Let $\vec{R}$ be the end-to-end distance vector of a random walk of fixed step length $|\vec{r}_i| = l$. $\vec{R}$ can then be expressed as $\displaystyle \vec{R} = \sum_{i=1}^N \vec{r}_i$, where $\vec{r}_i$ is the vector of the $i$-th step. The Root-Mean-Square End-to-End Distance is given by $\textrm{RMS}=\sqrt { \langle R^2 \rangle }$. Since the steps are mutually independent, the covariance of two steps $\vec{r}_i$ and $\vec{r}_j$ is zero if $i\neq j$ and $\textrm{Cov}(\vec{r}_i, \ \vec{r}_j)= \textrm{Var}(\vec{r}_i)$ if $i=j$. The variance of $ \vec{r}_i$ can be expressed as $ \textrm{Var}(\vec{r}_i)= \langle   \vec{r}_i \cdot  \vec{r}_i \rangle - \langle   \vec{r}_i \rangle^2$. Due to symmetry $\langle \vec{r}_i \rangle=\vec{0}$ and therefore the variance of 
of $ \vec{r}_i$ is simply $ \textrm{Var}(\vec{r}_i)= \langle   \vec{r}_i \cdot  \vec{r}_i \rangle = |\vec{r}_i|^2 = l^2$. Altogether, the covariance of $\vec{r}_i$ and $\vec{r}_j$ equals $\textrm{Cov}(\vec{r}_i, \ \vec{r}_j)=\delta_{ij}l^2$. The covariance of $\vec{r}_i$ and $\vec{r}_j$ can also be expressed as $\textrm{Cov}(\vec{r}_i, \ \vec{r}_j) = \langle   \vec{r}_i \cdot  \vec{r}_j \rangle - \langle   \vec{r}_i \rangle \cdot \langle   \vec{r}_j \rangle$. Combining the two different expressions for the covariance and using that
$\langle   \vec{r}_i \rangle=0$, results in $\langle   \vec{r}_i \cdot  \vec{r}_j \rangle =\delta_{ij}l^2$. This result can be used to determine the RMS:
$$\textrm{RMS}=\sqrt { \langle R^2 \rangle } = \sqrt { \langle \vec{R} \cdot \vec{R} \rangle } 
=\sqrt { \big\langle  \sum_{i=1}^N \vec{r}_i \cdot  \sum_{j=1}^N \vec{r}_j \big\rangle }
=\sqrt { \sum_{i=1}^N \sum_{j=1}^N \langle   \vec{r}_i \cdot  \vec{r}_j \rangle }= $$
$$=\sqrt { \sum_{i=1}^N \sum_{j=1}^N l^2 \delta_{ij} + 0^2}=\sqrt { \sum_{i=1}^N l^2}=\sqrt { N l^2}=l\sqrt { N }$$
Let $Z_i$ denote the $i$-th coordinate of the end-to-end distance vector $\vec{R}$ after $N$ steps, and let $X_i$ and $Y_i$ denote the number of steps taken in the $i$-th dimension in the positive and negative direction respectively. Then the set of random variables $\{X_i, Y_i\}_{i=1}^d$ follows a multinomial distribution with parameters  $N$ and $\displaystyle p_i=\frac{N}{2d}$. For sufficiently large values of $N$, $\{X_i, Y_i\}_{i=1}^d$ are approximately iid (independent and identically distributed) Poisson random variables with parameters $\displaystyle \lambda_i = \frac{N}{2d}$. For $\lambda > 20$, i.e. $N>40d$, $\textrm{Po}(\lambda) \sim \textrm{N}(\lambda, \lambda)$. $ Z_i = l(X_i - Y_i)$ and therefore  $\displaystyle Z_i \sim \textrm{N}(l(\lambda - \lambda), l^2(\lambda+\lambda))=\textrm{N}(0, 2l\lambda)=\textrm{N}\left(0, \frac{l^2N}{d}\right)$. 
$\displaystyle \langle R \rangle
= \langle \sqrt{R^2} \rangle
= \left\langle \sqrt{ \sum_{i=1}^d Z_i^2} \right\rangle$. The square root of a sum of $k$ independent $\textrm{N}(0, 1)$-distributed random variables is distributed according to the chi distribution, $\chi_k$. Therefore $\displaystyle  \sqrt{ \sum_{i=1}^d \frac{dZ_i^2}{l^2N}}$ is approximately  $\chi_d$-distributed for large values of $N$. The expected value of a $\chi_k$-distributed random variable
is $\displaystyle \sqrt{2} \frac{
\Gamma \left(\frac{k+1}{2}\right)
}{\Gamma \left( \frac{k}{2}\right)}$.
Hence $\displaystyle \langle R \rangle
=\left\langle\sqrt{ \sum_{i=1}^d Z_i^2}\right\rangle
=\left\langle l \sqrt{\frac{N}{d}} \sqrt{ \sum_{i=1}^d  \frac{dZ_i^2}{l^2N} }\right\rangle
=  l \sqrt{\frac{2N}{d} }\frac{
\Gamma \left(\frac{d+1}{2}\right)
}{\Gamma \left( \frac{d}{2}\right)}$.
