Probing isotopic ratios at z=0.89 Molecular line absorptions in front of the quasar PKS 1830-211 Sébastien Muller (ASIAA, Taiwan) M. Guélin (IRAM) M. Dumke (ESO) R. Lucas (IRAM) IAU Colloquium 199 Probing galaxies through quasar absorption lines, ShangHai, China, 2005 March 14-19 Absorption systems - Lyman forest 1012 - 1019 cm-2 gas filaments in extragalactic medium - Damped Lyman & HI 21 cm absorption 1019 - 1021 cm-2 outer parts of spiral galaxies - Molecular absorption 1020 - 1024 cm-2 central parts of galaxies Background quasars & molecular absorption Need a background continuum source … mm flux of quasars weaker than in the radio cm (SNR depending on the background continuum source) And an absorption system ! Dense gas, closer to the center of the intervening galaxy (small impact parameter) Highly probable association with gravitational lensing Molecular absorption systems in the mm Zabs N H2 (cm-2) Cen A 0.002 2. 10 3C293 0.04 > 6. 10 PKS 1413+135 0.25 5. 10 B3 1504+377 0.67 1.2 10 B 0218+357 0.68 4. 10 23 Background QSR PKS 1830-211 0.89 4. 10 22 Background QSR 20 20 Host galaxy Host galaxy 20 Host galaxy 21 Host galaxy PKS 1830-211 Intervening galaxy : MERLIN 6cmz=0.89 Typical spiral HST WFPC2 I band image Photometry from HST NE 1’’ (Winn et al 2002) I = 22 V > 24.7 SW position I > 24.9 V > 26.3 1st case of QSR lensed SWby a face-on spiral Mass within 3 kpc: (Wiklind & Combes 1998) Patnaik et al 1994 6 – 9 1010 M 2–4 kpc Plateau de Bure Interferometer observations HCO+ (1-2) 94.6 GHz H13CO (1-2) 92.0 GHz + HC18O + HC17O + Summer time between 1999 – 2002 Compact configuration Self calibration 14 (1-2) 92.3 GHz N/15N 16O/18O (1-2) 94.0 GHz (1-2) 91.3 GHz HNC (1-2) 96.2 GHz HN13C (1-2) 92.4 GHz H15NC (1-2) 94.2 GHz HCN Observations : (1-2) 90.3 GHz 12C/13C H13CN HC15N 18 (1-2) O/17O91.6 GHz 32S/34S Main isotopomers 2 components NE and SW SW : complete absorption for HCO+ non symetric profiles = sum of velocity components with widths similar to MW clouds (~10 km/s) Iabs = IO (1-exp-) Let’s compare the isotopic ratios in: One beam pencil in a galaxy at z = 0.89 6.4 Gyr ago Solar System 4.5 Gyr ago Local ISM now ! (Lucas & Liszt 1998) Galactic Center IRC +10216 LMC (Cernicharo et al 2000) (Chin 1999) NGC 4945 (Wanf et al 2004) archetype of AGB star low metallicity galaxy nucleus of a nearby SB galaxy Is there a clear chemical evolution ??? 12C : produced directly from He in massive stars (primary) 13C : produced from 12C and 16O in H burning (secondary) Problems : selected photodissociation, chemical fractionation, optically thin lines for 12C 14N : secondary, enhanced in CNO cycle at equilibrium 15N : secondary, destroyed in CNO, produced in explosive H or He burning 14N / 15N : increases with metallicity (gradient in the MW) 16O : primary, produced in massive stars 18O : secondary, produced in He burning from 14N 18O / 17O : constant value through the disk of the MW 17O : secondary, produced in low mass stars Sulfur : product of explosive O burning in MASSIVE stars Ratio 32S / 34S ??? Summary Isotopic ratios in the z=0.89 galaxy are : Different from SS, local ISM, GC Very different from IRC+10216 ! Closer to SBs no time for the low and intermediate mass stars to release the processed materials Nearby SB : because of time scale, outputs from massive stars dominate Different from LMC (O) (metallicity ?) Conclusion Isotopic ratios = signature of the chemical evolution and nuclear processing (???) Molecular absorption measurements Galaxy at z = 0.89 : look back time of 6.4 Gyr But only one beam pencil STATISTICS and chemical evolution : MORE SOURCES !!! Need to observe more absorption systems at different z ! ALMA Background source Absorption And even 2 lensed images ! Solar System Local ISM IRC +10216 Nuclei of nearby SB NGC 4945 LMC 10 89 40 - 70 45 50 62 -50+130 270 240 > 4400 100 114 490 600 1300 200 > 2000 PKS 1830 12C / 13C 32 14N / 15N 140 16O / 18O 18O / 17O 13 3 5.5 3.5 0.7 6 2 32S / 34S 10 1 20 19 22 13.5 18 67 24 Lucas & Liszt 1998 Cernicharo et al 2000 Wang et al 2004 Chin 1999
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