direct three-body decay $\sGlu \to \cPq \cPaq \chiz_1$ (T1), and squark-antisquark production with the direct two-body decay $\sQua \to \cPq
\chiz_1$ (T2). For $\cPqb$-quark enriched final states, we have considered two additional gluino SMS scenarios, where each gluino is forced into the three-body decay $\sGlu \to \cPqb \cPaqb
\chiz_1$ with 100% branching fraction (T1bbbb), or where each gluino decays through $\sGlu \to \cPqt \cPaqt \chiz_1$ (T1tttt). For $\cPqb$-quark enriched final states we also consider SMS that describe the direct pair production of bottom or top squarks, with the two-body decays $\sBot \to \cPqb \chiz_1$ (T2bb) and $\sTop \to
\cPqt \chiz_1$ (T2tt).

Note that first-generation $\sQua\sQua$ production (unlike $\sQua\sQua^*$ production) is not part of the simplified models used for the interpretation of the razor results, even though it is often the dominant process in the CMSSM for low values of the scalar-mass parameter $m_0$. This is because of the additional complication that the production rate depends on the gluino mass. However, the acceptance for $\sQua\sQua$ production is expected to be somewhat higher than for $\sQua\sQua^*$, so the limits from T2 can be conservatively applied to $\sQua\sQua$ production with analogous decays.

For each SMS, simulated samples are generated for a range of 