GREAT observations reveal strong self-absorption in [CII] 158 µm emission from NGC Urs U. Graf

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GREAT observations reveal strong self-absorption in [CII] 158 µm emission from NGC 2024 Urs U. Graf

Collaborators and Acknowledgements U.U. Graf, R. Simon, J. Stutzki, S.W.J. Colgan, X. Guan, R. Güsten, C.E. Honingh, H.-W. Hübers, GREAT special volume: A&A 2012, Vol. 542, L16 The GREAT team SOFIA staff in Palmdale and beyond 2

Outline GREAT Introduction NGC 2024: Introduction [12CII] map [13CII] map Line profile analysis [CII] Hyperfine line ratios 3

The GREAT team (part of it) GREAT: a modular dual color heterodyne spectrometer Basic Science observing period (2011): mostly L1 (~1400 GHz) and L2 (~1900GHz) 4

GREAT in the Lab Cryostats Oscilloscope Cold-load LO-synthesizer #1 Optics control Mixer-BIAS #1 & #2 Instrument computer SI mounting flange Power-supply SOFIA PI-rack LO-synthesizer #2 Monitor drawler 1.9 THz Solid-state LO 1.4 THz Solid-state LO Power distributor Ethernet-HUB Obs-computer IF-Power-supply IF Pre-processor FFTS CTS #1 and #2 IF LO-supply AOS-system IF-processor Chopper control Picture taken by DLR 5

and in SOFIA GREAT configuration during NGC 2024 observations (Nov 2012): L2 (1900 GHz) M (2500 GHz, experimental) inoperable due to LO failure 6

Receiver Noise Temperature TRX ~ 4000 K @ 1.9 THz 7

First Detection of Interstellar [CII] was made in NGC 2024 Russell et al. 1980 8

NGC 2024 Bright HII region shadowed by an optically opaque dust lane

NGC 2024 (zoomed) E-W Ionization front Radio absorption lines at 9 km/s Molecular lines N-S extended Optically thin CO lines have 2 peaks @ 9 km/s and 11 km/s 10

Standard source model: 2 emission components cold foreground @9 km/s Graf et al. 1993 warm background @11 km/s 11

[CII] integrated intensity map [12CII] & 8 µm (MSX) [CII] is very strong: > 600 K km/s Closely follows 8 µm continuum (i.e. UV heated dust) 12

[CII] Channel maps 2 main velocity components: 8-9 km/s and 11-12 km/s Dip at 10 km/s Slight spatial anticorrelation between the 2 velocity components 13

C18O 2-1 vs. [CII] near FIR5 C18O 2-1 Suggests 2 emission components in [CII] too, but we also got [13CII]... 14

CII fine structure lines at 1.9 THz Cooksy, Blake, Saykally 1986 15

Strong [12CII] & [13CII] emission NGC 2024 [12CII] & 8 µm (MSX) All three [13CII] HFS satellites detected [13CII] & [12CII] q 16

[13CII] reveals self-absorption! Data replotted on common vlsr scale [12CII] line divided by 10 17

Physical Properties [13CII] emission requires column density of N(13C+) 2.6x1017 cm-2 N(H) 1.6x1023 cm-2 This is as high as the molecular column density! Temperature of background component not well constrained due to foreground absorption, but needs to be >165 K, probably several 100 K Optically thin limit: 800 K Temperature of absorbing foreground: TFG < 90 K Column density of absorbing foreground: NFG(C+) 1018 cm-2 NFG(H) 1022 cm-2 18

HII region / molecular cloud IF Photon Dominated Region (PDR) C+, C, CO layered within ~1-2 Av (NH2 = 1021 cm-2) Many (10-100) IFs required for large column density of warm CO emission Clumpy interface C+, C, and warm CO spatially coexistent 19

PDR Modelling One PDR surface cannot produce the strong emission that we observe Edge-on geometry (ionization front) may help locally Clumpiness could make the difference. Preliminary estimates show that a clumpy cloud model can reproduce the observed intensities Need more data for detailed modelling 20

Anomalous Hyperfine Ratio? Orion Bar, Ossenkopf et al. 2011 62.5 % 59.9% 12.5 % 8.8% 25.0 % 31.4% 2-1/1-0 ratio should be 1.25 measured ratio is ~2 D. Neufeld: Corrected HFS weights yield ratio of 2.5 21

Simultaneous Fit with Fixed Hyperfine Ratios Original HF ratios Recalculated HF ratios Fit is believable now! 22

Conclusion [CII] is self-absorbed Kinematic signature differs from CO isotopes Column densities are very high: 1023 cm-2 @ several 100 K in background 1022 cm-2 @ 100 K in absorbing foreground Anomalous hyperfine intensity ratio probably explained by error in original paper High spectral resolution is crucial! 23

Conclusion [CII] is self-absorbed Kinematic signature differs from CO isotopes Column densities are very high: 1023 cm-2 @ several 100 K in background 1022 cm-2 @ 100 K in absorbing foreground Anomalous hyperfine intensity ratio probably explained by error in original paper High spectral resolution is crucial! 24

Thank You