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The molecular ion CH$\mathrm{2+}$ is of special theoretical interest because it is both quasi-linear and exhibits a strong Renner-Teller interaction between its ground and first-excited electronic states. At linearity, the ground state is a $\mathrm{<mrow\; data-mjx-texclass="ORD">2</mrow>}\Pi u$ state that splits into $X~2A1$ and $A~2B2$ states as the molecule bends. The $A~$ state is linear, while the $X~$ is quasi-linear with a barrier to linearity of only 1089 \wn. Thus, only the ground vibrational state is bound by the barrier to linearity. \vspace{2ex} The spectrum of CH$\mathrm{2+}$ in the region 11,000--13,000 \wn\ has been recorded with our Ti:sapphire laser spectrometer. This spectrometer couples velocity modulation with heterodyne detection for near shot-noise-limited sensitivity. Since our initial letter on this spectrum,} \textbf{121}, 11527 (2004).} we have selectively rescanned portions of this spectrum with improved signal-to-noise. As a result, we have been able to assign the $A~(0,3,0)3\leftarrow X~(0,0,0)2$ band and detect the $X~(0,9,0)2\leftarrow X~(0,0,0)1$ band, whose assignment is in progress. A more detailed analysis of the entire spectrum, including spin splitting, is underway.