CONDOR, the CO, N + , Deuterium Observations Receiver, is designed to make velocity-resolved observations of the CO, [NII], and p-H 2 D + lines in the 1.4 THz (200-240 µm) atmospheric windows. CONDOR's first light observations were made with the APEX telescope in November 2005. The CONDOR beam on APEX (at ν = 1.5 THz) was expected to consist of a 4.3 main beam and a 73 error beam; this beam structure was verified from scans of Mars. The pointing accuracy, also determined from Mars scans, was better than 7 . The average atmospheric transmission during our Orion observations (elev∼ 57 • ) was 19 ± 4 % along the line-of-sight. A forward efficiency of F ef f = 0.8 was determined from sky dips, and observations of the Moon and Mars were used to couple the CONDOR beam to sources of different sizes (η c = 0.40 and ∼ 0.10, respectively). For more information, see Wiedner et al. 2006.With CONDOR, we observed CO J = 13 − 12 emission from three sites of highmass star formation in Orion (IRc2, FIR4, and NGC2024). A sample spectrum from Orion IRc2 is shown in Fig. 1. In our analysis of IRc2, we assume that all spectra from positions < ±20 include a "spike" (∆v ≈ 5 km s −1 ) and a "hot core" component (∆v ≈ 35 km s −1 ). The optically thin spike emission arises from the interface of the Orion Ridge and the energizing M42 HII region. A simple isothermal model fit to the J = 13 − 12 and higher-J CO lines (e.g. Boreiko et al. 1989) reveals that the layer must indeed be warm (T kin ≈ 620 K), dense (n(H 2 ) ≈ 2 × 10 6 cm −3 ), and thin (N (CO) ≈ 1.2 × 10 16 cm −2 ). Because the Ridge has a temperature gradient, we are currently modeling the data using a PDR code. We are also analyzing the line wings to constrain the outflow properties. This research is supported within SFB 494 of the Deutsche ForschungsGemeinschaft.