Let $Q=(Q_{0},Q_{1},h,t)$ be a finite quiver where $Q_{0}$ are the vertices, $Q_{1}$ the arrows and we have two maps $h: Q_{1} \rightarrow Q_{0}$ (head) and $t: Q_{1} \rightarrow Q_{0}$ (tail). Fix a field $K$ and associative to $Q$ two vector spaces $R=K^{Q_{0}}$ and $A=K^{Q_{1}}$ i.e vector spaces consisting of $K$-valued functions on $Q_{0}$ and $Q_{1}$ respectively. Then the path algebra of $Q$ is defined as the tensor algebra $$R\langle A\rangle=\bigoplus_{d=0}^{\infty}A^d$$ You can see more details in Derksen, Weyman, Zelevinsky's first paper about quivers with potentials: http://arxiv.org/abs/0704.0649 at the beginning of section two.
But I know the path algebra $KQ$ of $Q$ is the K-algebra whose underlying K-vector space has as its basis the set of all paths and multiplication given by concatenation of paths.
My question is how to understand the two def. are equivalent? Whether Derksen, Weyman, Zelevinsky define the path algebra as the tensor algebra firstly? If not ,who can give me some related papers?