The highly collimated bipolar outflow of OH231.8+4.2

We present high spatial resolution observations of the CO molecular emissio n (J = 1-0 and J = 2-1 lines) in the post-AGB bipolar nebula OH 231.8+4.2. High-quality NIR images (J, H, K' bands) of light scattered by grains were also obtained. Our observations probe the bulk of the nebular material, pro viding maps with a resolution similar to1" of the mass distribution, both C O and NIR images being very closely coincident. The combination of the two (CO)-C-12 lines has been used to measure the distribution of the kinetic te mperature in the nebula, which is found to be very low, ranging between 8 K , in the outer southern clumps, and 35 K, in the central region. A relative temperature increase is found in the northernmost condensation, probably a ssociated to a strong bow-like shock. Since velocities are also measured in CO, the dynamic parameters (kinetic momentum and energy) are also measured with high resolution. Most of the nebular mass (similar to0.64 M-.) is loc ated in the central condensation and flows at expansion velocities less tha n or equal to 40 km s(-1). The rest of the gas, similar to0.3 M-. almost eq ually distributed in the two lobes, flows along the nebular axis at high ve locities, that increase proportionally to the distance to the central star reaching values as large as 430 km s(-1), as a result of a sudden accelerat ion happened about 770 yr ago. The general mass distribution in OH231.8+4.2 is found to be clumpy and very elongated, with a length/width ratio reachi ng a factor 20 in the southern tail. In the center, however, we find a doub le hollow-lobe structure, similar to those found in other well studied prot oplanetary nebulae. We stress the enormous kinetic linear momentum carried by the molecular nebula, about 27 M-. km s(-1) (5.5 x 10(39) g cm s(-1)). T he kinetic energy is also very high, similar to 1700 M-. km(2) s(-4) simila r to 3.4 x 10(46) erg. Given the short time during which the acceleration o f the molecular out ow took place, we conclude that the linear momentum car ried by the stellar photons is about a factor 100 smaller than that carried by the out ow, even if the effects of multiple scattering are taken into a ccount. We independently argue that radiation pressure directly acting onto grains (the mechanism thought to be responsible for the mass ejection in A GB envelopes) cannot explain the observed bipolar ow, since this would prod uce a significant shift between the dust and gas features that is not obser ved. Finally, we review the uncertain nature and evolutionary status of thi s unique object.