proton-proton collisions with a centre-of-mass (CM) energy of $\sqrt{s}=8 {\,\mathrm{TeV}}$ were simulated. The lightest graviton, $G$, was produced as a resonance and allowed to decay via $G \rightarrow gg $ and $G \rightarrow q \bar{q}$ for $q = u,d,s,c,b $. The mass of the graviton was chosen to be $m_G = 2.23 {\,\mathrm{TeV}}$ which corresponds to the lower bound on the allowed graviton mass for the coupling $k/ \bar{M}_{pl} = 0.1 $ in [@Aad:2012cy]. An analysis based on the ATLAS experiment’s search for new phenomena in dijet distributions [@ATLAS:2012pu] was then carried out. Jets were constructed using the [@Cacciari:2011ma] implementation of the anti-$k_t$ algorithm [@Cacciari:2008gp] with the energy recombination scheme and a distance parameter $R=0.6$. Jets with $|y| \geq 4.4 $ were discarded, where $y$ is the rapidity of the jet in the $pp$ CM frame. Events with less than two jets passing this constraint were vetoed. The rapidities of the two highest $p_T$ jets in the $pp$ CM frame are given by $y_{1}$ and $y_{2}$. In the dijet CM frame formed by the two hardest jets, their corresponding rapidities are $y_{*}$ and $-y_{*}$ where $y_{*}= \frac{1}{2} (y_1 - y_2)$. Events not satisfying $|y_{*}| < 0.6$ and $|y_{1,2}| < 2.8$ 