the serpens star forming region in hco + , hcn, and n 2 h +
DESCRIPTION
The Serpens Star Forming Region in HCO + , HCN, and N 2 H +. Michiel R. Hogerheijde Steward Observatory The University of Arizona. Outline. Molecular clouds and star formation The Serpens star-forming region Single-dish images Interferometer images - PowerPoint PPT PresentationTRANSCRIPT
The Serpens Star Forming Region in HCO+, HCN, and N2H+
Michiel R. HogerheijdeSteward ObservatoryThe University of Arizona
Outline
Molecular clouds and star formation The Serpens star-forming region Single-dish images Interferometer images Combination single-dish and interferometer Abundances A shock model for HCN and N2H+
Conclusions
Molecular clouds and star formation
Stars form in condensations in interstellar clouds
Cloud structure determines stellar masses
Jets, outflows affect cloud chemistry and structure
The Serpens star-forming region
Dense cluster of pre–main-sequence stars
Two condensations, NW and SE
~Dozen submm continuum peaks
Many associated with YSOs, some starless cores
SCUBA 850 µm on DSS imageDavis et al. (1999)
JCMT/SCUBA images of Serpens
Davis et al. (1999)
SMM4
SMM11
SMM6
SMM2
SMM3SMM1/FIRS1
SMM8 SMM9/S68N
SMM10
SMM5
Many outflows ‘Tangle’ of outflows
Intermediatevelocities:±7 km s-1
Extreme velocities:±11 km s-1
Davis et al. (1999)
How do outflows affect structure and chemistry in Serpens? J=1–0 transitions (≈3 mm) of HCO+, HCN, N2H+
Common tracers of dense [n(H2)≈105–6 cm-3] and cool (Tkin≈30 K) gas
Morphology chemistry
Single-dish on-the-fly maps from Kitt Peak 12-meter telescope
Interferometer mosaics from the Berkeley-Illinois-Maryland array (SE region only)
Single-dish maps
HCO+ 1–0 HCN 1–0 N2H+ 1–0
Resolution 1 = 0.12 pc = 21,000 AU
Single-dish maps
N2H+ equally strong in NE and SE– Follows submillimeter continuum
HCO+ and HCN peak in SE – Where most embedded YSOs and their
outflows are E-W velocity gradient
– Solid-body rotation, also noted by Olmi & Testi (2002)
Interferometer mosaics
Higher resolution: 10–20 arcsec; 140 arcsecs primary field of view
Filters out large-scale emission ~ 115 arcsec 13-point ‘mosaic’: overlapping pointings
Interferometer mosaics: N2H+
Resolution 17 = 0.033 pc = 7000 AU
Interferometer mosaics: N2H+
Color: N2H+
Contours: 850 µm
Interferometer mosaics: HCNResolution 21 = 0.041 pc = 8500 AU
Interferometer mosaics: HCO+
Resolution 12 = 0.022 pc = 4600 AU
Interferometer mosaics
N2H+:– At continuum peaks– Ahead of SMM3’s jet– North of ‘shock position’
HCO+ and HCN:– near YSOs, outflows
Strong blue-shifted HCN west of SMM4:– ‘shock position’
Combining single-dish and interferometer data Interferometers filter out emission on
scales larger ~ shortest antenna spacing
Missing ‘zero-spacing’ flux KP12m well matched to 6-m BIMA
antennas Method: joint deconvolution
Combined BIMA and KP12m
Combined BIMA and KP12m
Combined maps qualitatively look as expected
High resolution of BIMA brings out velocity details on small scales
‘Washed out’ in KP12m map BIMA recovers ~30% of line flux
Abundances
Are HCO+ and HCN enhanced by outflow action?
Throughout core, or only locally?
Abundances
Olmi & Testi (2002) C18O 1–0 map FCRAO: 1 arcmin
resolution Tex
N(H2) Use to derive
abundances on 1 arcmin scales
Abundances
HCO+ HCN N2H+
AbundancesAverageSerpens
Peakpositions
Dark cloud valuesa
N2H+ 3.8x10-10 7.8x10-10 (5–10)x10-10
HCO+ 3.0x10-10 6.5x10-10 (2–8)x10-9
HCN 5.4x10-10 9.6x10-10 (0.5–5)x10-8
Factor 2 enhancement near YSOs (outflows)Abundances HCN, HCO+<< dark clouds: depletion; Tex?
a) van Dishoeck et al. 1993; Ohishi et al. 1992; Turner 2000
Shock model for HCN and N2H+
Offsets between HCN (color) and N2H+ (contours)
SMM3’s jet Shock position
Shock model for HCN and N2H+
C-type shock Magnetic precursor Ions accelerate, compress,
and heat before neutrals N2H+ emission up in
precursor HCN abundance up in
warm region: evaporation of ices
Accompanying H2O destroys N2H+
Draine & Katz (1986)
Two models for shock position: 1
Jet driven by SMM4, deflected by dense material. N2H+ in magnetic precursor of C-type shock.
Two models for shock position: 2
Jet driven by SMM1, hitting dense matter. HCN at bow shock, N2H+ along the sides where shock speeds are lower.
Conclusions
HCN, HCO+ locally enhanced by shocks Depleted in rest of cloud compared to dark-cloud
values Unresolved observations would trace outflow-
affected material preferrentially
N2H+ undepleted: traces condensations N2H+ emission ahead of shocks: enhancement in
magnetic precursor, destruction in warm region?
Future work
C18O on 10–20 arcsec scales, fully sampled
Higher-J lines: excitation HCN, HCO+, and N2H+
High-resolution interferometry shock region; additional species
Time-dependent shock-chemistry model
Many thanks to…
Staff of the Kitt Peak 12 meter Radio Telescope Staff of the Berkeley-Illinois-Maryland Association
millimeter array Chris Davis and Luca Olmi for making their data
available electronically