$O(3)$, $N=1$               14.6%              14.6%               0.6%                 70.2%                       0.40

  : \[tab:brs\] The branching ratios of $g^1$ into tops, bottoms, light quarks (jets), and custodial partners, as well as the total width $\Gamma_{g^1} / M_{g^1}$, for several different RS scenarios in the limit $M_{g^1} \gg m_f$.

![\[fig:tevatron\] Cross section for $p \bar{p} \rightarrow g^1 \rightarrow t \bar{t}$ at the Tevatron as a function of the mass of $g^1$, compared with the CDF exclusion curve. The mass of custodial partners is 360GeV.](Tevatron.pdf)

In models with large boundary kinetic terms, $g^1$ primarily decays into light quarks, swamping the decay into tops, and its over-all width becomes much narrower. This fact, combined with the enhancement of $g^1$ production, allows for the possibility that one could discover $g^1$ in the dijet mode, against the large QCD background. To explore this possibility, in Figure \[fig:jetplot\] we plot the invariant mass distribution of QCD dijets (with rough acceptance cuts $|\eta| <1.0$ and $p_T > 20$ GeV to reduce the SM background). For $M_{g^1} = 2$ or $3$ TeV, we can reconstruct a peak against the dijet background with ample statistics. Based on the size of the signal and background, we estimate that one could potentially discover $g^1$ even if 