We surveyed 81 dense molecular cores associated with regions of massive sta
r formation and Sgr A in the J(K-1K1) = 5(05) - 4(04) and 10(010) - 9(09) l
ines of HNCO. Line emission was detected towards 57 objects. Selected subsa
mples were also observed in the lot - 0(00), 4(04) - 3(03), 7(07) - 6(06),
15(015) - 14(014), 16(016) - 15(015) and 21(021) - 20(020) lines, covering
a frequency range from 22 to 461 GHz. HNCO lines from the K-1 = 2, 3 ladder
s were detected in several sources. Towards Orion-KL, K-1 = 5 transitions w
ith upper state energies E-u/k similar to 1100 and 1300 K could be observed
.
Five HNCO cores were mapped. The sources remain spatially unresolved at 220
and 461 GHz (10(010) - 9(09) and 21(010) 20(020) transitions) with beam si
zes of 24 " and 18 ", respectively. The detection of hyperfine structure in
the 1(01) - 0(00) transition is consistent with optically thin emission un
der conditions of Local Thermodynamic Equilibrium (LTE). This is corroborat
ed by a rotational diagram analysis of Orion-KL that indicates optically th
in line emission also for transitions between higher excited states. At the
same time a tentative detection of interstellar (HNCO)-C-13 (the 10(0,10)
- 9(0,9) line at 220 GHz toward G 310.12-0.20) suggests optically thick emi
ssion from some rotational transitions.
Typical HNCO abundances relative to Hz as derived from a population diagram
analysis are similar to 10(-9). The rotational temperatures reach similar
to 500 K The gas densities in regions of HNCO K-1 = 0 emission should be n
greater than or similar to 10(6) cm(-3) and in regions of K-1 > 0 emission
about an order of magnitude higher even for radiative excitation.
HNCO abundances are found to be enhanced in high-velocity gas. KNCO integra
ted line intensities correlate well with those of thermal SiO emission. Thi
s indicates a spatial coexistence of the two species and may hint at a comm
on production mechanism, presumably based on shock chemistry.