We present high sensitivity and high angular resolution images of the high
velocity (upsilon(LSR) > 30 km s(-1)) CO emission in the J = 1 --> 0 and J
= 2 --> 1 lines of the Orion KL region. These results reveal the morphology
of the high-velocity CO emission at the most extreme velocities. High velo
city emission has only been detected in two regions: BN/KL (IRc2/I) and Ori
on-S.
The Orion-S region contains a very young (dynamical age of similar to 10(3)
years), very fast (similar to 110 km s(-1)) and very compact (less than or
similar to 0.16 pc) bipolar outflow, From the morphology of the high-veloc
ity gas we estimate that the position of the powering source must be 20 " n
orth of FIR 4. So far, the exciting source of this outflow has not been det
ected. For the IRc2/I molecular outflow the morphology of the moderate velo
city (less than or similar to 60 km s(-1)) gas shows a weak bipolarity arou
nd IRc2/I. The gas at the most extreme velocities does not show any bipolar
ity around IRc2/I, if any, it is found similar to 30 " north from these sou
rces. The blue and redshifted gas at moderate velocities shows similar spat
ial distribution with a systematic trend for the size of the high-velocity
gas to decrease as the terminal radial velocity increases. The same trend i
s also found for the jet driven molecular outflows L 1448 and IRAS 03282 3035. The size-velocity relationship is fitted with a simple velocity law w
hich considers a highly collimated jet and entrained material outside the j
et moving in the radial direction. We also find that most of the CO outflow
ing at moderate velocities is located at the head of the jet. Our results a
nd the spatial distribution and kinematics of the shock tracers in this out
flow can be explained if the IRc2/I outflow is driven by a precessing jet o
riented along the line of sight. The implication of these findings in the e
volution of molecular outflows is discussed.