Line emission in shocks and PDR - Observatoire de Paris
Line emission in shocks and PDR - Observatoire de Paris
Line emission in shocks and PDR - Observatoire de Paris
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<strong>L<strong>in</strong>e</strong> <strong>emission</strong> from <strong>shocks</strong><br />
Sylvie Cabrit (<strong>Observatoire</strong> <strong>de</strong> <strong>Paris</strong>)<br />
G. P<strong>in</strong>eau <strong>de</strong>s Forêts, D. Flower, J. Le Bourlot (shock<br />
mo<strong>de</strong>ls), C. Ceccarelli (CO <strong>and</strong> H 2<br />
O predictions)<br />
•Shocks <strong>in</strong> outflows: evi<strong>de</strong>nce for C-precursors (ISO)<br />
•Water <strong>emission</strong> from <strong>shocks</strong>: need for Herschel<br />
•Chemistry <strong>and</strong> <strong>in</strong>ternal structure: need for ALMA<br />
<strong>and</strong> <strong>PDR</strong>s<br />
M. Gér<strong>in</strong> <strong>and</strong> J. Le Bourlot<br />
(<strong>Observatoire</strong> <strong>de</strong> <strong>Paris</strong>)<br />
Dusty04 - <strong>Paris</strong>, October 2004
Magnetic molecular <strong>shocks</strong><br />
Low ionisation, magnetized<br />
medium ion/neutral<br />
<strong>de</strong>coupl<strong>in</strong>g Cont<strong>in</strong>uous<br />
(C-type) « shock »<br />
Magnetic precursor<br />
Viscous J-type front<br />
Long time-scales to reach<br />
full C steady-state<br />
t ~ 10 4 yrs x (10 4 cm-3/nH)<br />
Young <strong>shocks</strong> comb<strong>in</strong>e C-<br />
precursor + viscous J-front<br />
(Chieze et al. 1998; Lesaffre et al.<br />
2004)<br />
« Age typical 1000 » yrs stationary : C+J structure C-shock nH<br />
nH = 10 4 cm-3, Vs = 25 km/s B = 100µ G.<br />
Dusty04 - <strong>Paris</strong>, October 2004
Evi<strong>de</strong>nce for C-precursors: H2 pure<br />
rotational l<strong>in</strong>es <strong>in</strong> molecular flows<br />
H2 v=0-0 S(5) l<strong>in</strong>e flux (6’’ to 20’’ beams)<br />
H2 v=0 excitation temperature<br />
HH2 with ISOCAM (Lefloch et al. 2003)<br />
Cabrit et al. 2003 (with SWS data from Wright et<br />
al., Rosenthal et al.)<br />
Dusty04 - <strong>Paris</strong>, October 2004
CO <strong>and</strong> H2O: The ISO-LWS view<br />
LVG (Giann<strong>in</strong>i et al. 2001):<br />
Warm gas (200-2000 K)<br />
Dense (3x10 4 -10 7 cm-3)<br />
Compact (ff ~ 1% : typical<br />
size 10’’)<br />
L(CO + H2O) ~ outflow Lk<strong>in</strong><br />
Shocked gas ?<br />
X(H2O)/X(CO)<br />
3<br />
1<br />
0.3<br />
0.1<br />
C-shock mo<strong>de</strong>ls (Tgas<br />
= Tmax)<br />
X(H2O)/X(CO) <strong>in</strong>creases with<br />
temperature: mantle<br />
<strong>de</strong>sorption <strong>and</strong> O to H 2<br />
O<br />
conversion.<br />
Dusty04 - <strong>Paris</strong>, October 2004
Shocks sampled by ISO-LWS:<br />
of NGC 1333-IRS4<br />
The example<br />
(CO fluxes from Giann<strong>in</strong>i et al. 2001)<br />
High-J CO l<strong>in</strong>es not very<br />
discrim<strong>in</strong>ant; can be<br />
fitted by various shock<br />
mo<strong>de</strong>ls of age 1000 yrs:<br />
Dense C<br />
CJ<br />
C<br />
ff=0.017<br />
ff=0.2<br />
J<br />
ff=1<br />
Dusty04 - <strong>Paris</strong>, October 2004
Shocks sampled by ISO-LWS:<br />
of NGC 1333-IRS4<br />
The example<br />
H2O l<strong>in</strong>es very discrim<strong>in</strong>ant:<br />
only <strong>de</strong>nse C-<strong>shocks</strong> of low ff<br />
can fit both 179µ m <strong>and</strong> 80µ m<br />
(H2O fluxes from Giann<strong>in</strong>i et al. 2001)<br />
nH = 10 4 cm-3:<br />
Pure J: Vs = 15 km/s, b=0.1 (ff = 1)<br />
C+J: Vs = 25 km/s, b=1 (ff = 1)<br />
Pure C: Vs = 50 km/s, b=1 (ff =<br />
0.2)<br />
nH = 10 5 cm-3:<br />
Pure C: Vs = 25 km/s, b=1 (ff =<br />
0.017)<br />
Dusty04 - <strong>Paris</strong>, October 2004
The 557GHz ortho-H2O l<strong>in</strong>e<br />
SWAS observations of molecular outflows: broad<br />
w<strong>in</strong>gs shocked gas, but 2-3 times stronger than<br />
expected from ISO-LWS (Bene<strong>de</strong>tt<strong>in</strong>i et al. 2003)<br />
Exten<strong>de</strong>d component, too cold for ISO<br />
Estimated H 2<br />
O abundance ~ 10 -6 if dom<strong>in</strong>ated by<br />
cold swept-up CO (Neufeld et al. 2000)<br />
lower than expected for <strong>shocks</strong> of V > 5 km/s…<br />
ODIN observations of IRAS 16293 (Ristorcelli et al.<br />
2004) : similar lobe size to ISO-LWS (120’’ vs 80’’).<br />
Dusty04 - <strong>Paris</strong>, October 2004
Comparison of H2O(557GHz) <strong>and</strong> CO(3-2) <strong>in</strong><br />
the ODIN beam<br />
CO(3-2)/1.5 (Lis<br />
et al.)<br />
CO(3-2)/H 2<br />
O(557GHz)<br />
H 2<br />
O 557GHz<br />
X(H 2<br />
O)/X(CO)<br />
-20 0 20 km/s<br />
CO(3-2)/H 2<br />
O ~ 1.5 <strong>in</strong> red w<strong>in</strong>g, ~ 2.5 <strong>in</strong> blue w<strong>in</strong>g<br />
C-Shocks with Vs ~ 12-15 km/s (ff ~ 0.2 <strong>in</strong> 120’’ beam)<br />
X(H 2<br />
O) ~ 0.05-0.2 X(CO) ~ 1-3 10 -5 of H 2<br />
Dusty04 - <strong>Paris</strong>, October 2004
Comparison with other CO l<strong>in</strong>es (CSO<br />
observations <strong>and</strong> ISO-LWS)<br />
CO(6-5) <strong>and</strong> CO(4-3) also<br />
compatible with C-<strong>shocks</strong><br />
of Vs ~ 10-15 km/s (ff~0.7<br />
<strong>in</strong> CSO beam).<br />
CO high-J (ISOLWS) trace<br />
hotter component:<br />
protostellar envelope or<br />
faster/<strong>de</strong>nser <strong>shocks</strong> <strong>in</strong> jet<br />
bullets ?<br />
data from Lis et al. 2002 (CSO) <strong>and</strong> Ceccarelli et<br />
al. 1998 (LWS)<br />
CSO (ff=0.7)<br />
LWS (ff=1)<br />
Need for Herschel water maps <strong>and</strong> nH diagnostics!<br />
Dusty04 - <strong>Paris</strong>, October 2004
Shock Chemistry<br />
C-precursor is<br />
chemically active<br />
H2 S(5)<br />
(Flower & P<strong>in</strong>eau <strong>de</strong>s<br />
Forêts, Schilke et al., Berg<strong>in</strong><br />
et al.)<br />
Mantle <strong>de</strong>sorption<br />
(eg. CH 3<br />
OH)<br />
Gra<strong>in</strong> core sputter<strong>in</strong>g<br />
(SiO)<br />
Endothermic<br />
reactions (SO, CN…)<br />
L1157 (Bachiller et al. 2001)<br />
Dusty04 - <strong>Paris</strong>, October 2004<br />
Cabrit et al. 1998
Shock chemistry: mo<strong>de</strong>ls<br />
Complex variations (both<br />
spatially <strong>and</strong> from source<br />
to source) <strong>in</strong> abundances<br />
of enhanced species<br />
Evolutionary trends ?<br />
Vary<strong>in</strong>g shock conditions ?<br />
(nH,Vs,B)<br />
Pre-processed medium ?<br />
(Bachiller et al. 2001, Jorgensen etal.<br />
2004)<br />
Dusty04 - <strong>Paris</strong>, October 2004
Shock chemistry: mo<strong>de</strong>ls<br />
C-shock nH = 10 4 cm-3 Vs = 30 km/s B = 100µ G<br />
Complex variations (both<br />
spatially <strong>and</strong> from source<br />
to source) <strong>in</strong> abundances<br />
of enhanced species<br />
Evolutionary trends ?<br />
CS<br />
Vary<strong>in</strong>g shock SO conditions ?<br />
(nH,Vs,B)<br />
Pre-processed medium ?<br />
CH3OH<br />
H2CO<br />
HCN<br />
SiO<br />
HCO+<br />
Dusty04 - <strong>Paris</strong>, October 2004<br />
N(CO)<br />
(cm-2)
Shock chemistry <strong>and</strong> <strong>in</strong>ternal structure<br />
Herschel: CH + , H 3<br />
O + , NH, Tex(H 2<br />
S,NH 3<br />
…)<br />
ALMA: Fully resolved magnetic precursor (size ~ 10 3<br />
AU) <strong>in</strong> many tracers:<br />
Chemical stratification vs. Mo<strong>de</strong>ls<br />
Ion-neutral <strong>de</strong>coupl<strong>in</strong>g (HCO+)<br />
J-front <strong>and</strong> H2 reformation zones vs. Optical/nearIR<br />
Shock proper motions<br />
Turbulent mix<strong>in</strong>g-layers <strong>in</strong> non-planar <strong>shocks</strong><br />
Constra<strong>in</strong>ts on shock age <strong>and</strong> B-field<br />
outflow dynamics, protostellar mass-loss & collimation<br />
mechanism, evolutionary Dusty04 - scheme<br />
<strong>Paris</strong>, October 2004
Photo Dissociation Regions<br />
(<strong>PDR</strong>s)<br />
I<strong>de</strong>al laboratories for ISM physical <strong>and</strong> chemical processes<br />
important targets for ALMA <strong>and</strong> Herschel<br />
Herschel :<br />
Cool<strong>in</strong>g processes ([CII], [OI], CO, H 2<br />
O) <strong>and</strong> thermal balance<br />
Chemistry (H 2<br />
O ; C- N- <strong>and</strong> O- hydri<strong>de</strong>s <strong>in</strong>clud<strong>in</strong>g CH + )<br />
Complex molecules (C clusters, PAHs, ...)<br />
Dynamics of the hot <strong>in</strong>terface<br />
Dust properties (from SED)<br />
ALMA : Small scale structures <strong>in</strong> the <strong>in</strong>terface, turbulence, coupl<strong>in</strong>g of<br />
gas dynamics <strong>and</strong> chemistry : time <strong>de</strong>pen<strong>de</strong>nt effects<br />
<strong>L<strong>in</strong>e</strong> <strong>and</strong> cont<strong>in</strong>uum polarisation us<strong>in</strong>g radicals<br />
Dusty04 - <strong>Paris</strong>, October 2004
C x<br />
B x<br />
B" x<br />
A x<br />
A" x<br />
C" x<br />
ODIN beams <strong>in</strong> IRAS 16293 outflow on CO map of Lis et al.(2002)