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EMBEDDED PROTOSTARS IN THE DUST, ICE, AND GAS IN TIME (DIGIT) HERSCHEL KEY PROGRAM: CONTINUUM SEDs, AND AN INVENTORY OF CHARACTERISTIC FAR-INFRARED LINES FROM PACS SPECTROSCOPY.

Authors :
GREEN, JOEL D.
EVANS II, NEAL J.
JØRGENSEN, JES K.
HERCZEG, GREGORY J.
KRISTENSEN, LARS E.
JEONG-EUN LEE
DIONATOS, ODYSSEAS
YILDIZ, UMUT A.
SALYK, COLETTE
MEEUS, GWENDOLYN
BOUWMAN, JEROEN
VISSER, RUUD
BERGIN, EDWIN A.
VAN DISHOECK, EWINE F.
RASCATI, MICHELLE R.
KARSKA, AGATA
VAN KEMPEN, TIM A.
DUNHAM, MICHAEL M.
LINDBERG, JOHAN E.
FEDELE, DAVIDE
Source :
Astrophysical Journal; 6/20/2013, Vol. 770 Issue 2, p1-45, 45p
Publication Year :
2013

Abstract

We present 50-210μm spectral scans of 30 Class 0/I protostellar sources, obtained with Herschel-PACS, and 0.5-1000μm spectral energy distributions, as part of the Dust, Ice, and Gas in Time Key Program. Some sources exhibit up to 75 H<subscript>2</subscript>O lines ranging in excitation energy from 100 to 2000 K, 12 transitions of OH, and CO rotational lines ranging from J = 14 → 13 up to J = 40 → 39. [O I] is detected in all but one source in the entire sample; among the sources with detectable [O I] are two very low luminosity objects. The mean 63/145μm [O I] flux ratio is 17.2 ± 9.2. The [O I] 63μm line correlates with L<subscript>bol</subscript>, but not with the time-averaged outflow rate derived from low-J CO maps. [C II] emission is in general not local to the source. The sample Lbol increased by 1.25 (1.06) and T<subscript>bol</subscript> decreased to 0.96 (0.96) of mean (median) values with the inclusion of the Herschel data. Most CO rotational diagrams are characterized by two optically thin components (〈N〉 = (0.70 ± 1.12) × 10<superscript>49</superscript> total particles). NCO correlates strongly with L<subscript>bol</subscript>, but neither T<subscript>rot</subscript> nor N<subscript>CO</subscript>(warm)/N<subscript>CO</subscript>(hot) correlates with L<subscript>bol</subscript>, suggesting that the total excited gas is related to the current source luminosity, but that the excitation is primarily determined by the physics of the interaction (e.g., UV-heating/shocks). Rotational temperatures for H<subscript>2</subscript>O (〈T<subscript>rot</subscript>〉 = 194 ± 85 K) and OH (〈T<subscript>rot</subscript>〉 = 183 ± 117 K) are generally lower than for CO, and much of the scatter in the observations about the best fit is attributed to differences in excitation conditions and optical depths among the detected lines. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
0004637X
Volume :
770
Issue :
2
Database :
Complementary Index
Journal :
Astrophysical Journal
Publication Type :
Academic Journal
Accession number :
90179211
Full Text :
https://doi.org/10.1088/0004-637X/770/2/123