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Extragalactic Absorption – The Promise of the EVLA Karl M. Menten Max-Planck-Institute for Radio Astronomy Christian Henkel (MPIfR), with Christian Henkel.

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Presentation on theme: "Extragalactic Absorption – The Promise of the EVLA Karl M. Menten Max-Planck-Institute for Radio Astronomy Christian Henkel (MPIfR), with Christian Henkel."— Presentation transcript:

1 Extragalactic Absorption – The Promise of the EVLA Karl M. Menten Max-Planck-Institute for Radio Astronomy Christian Henkel (MPIfR), with Christian Henkel (MPIfR), Chris Carilli (NRAO), Mark Reid (CfA) & many others The EVLA Vision: Galaxies through Cosmic Time December 18, 2008

2 Extragalactic Molecules (other than CO) Since the late 1980s (mostly) Henkel & Mauersberger and their collaborators have detected a large number of molecules toward the nuclei of local galaxies Species include: CH 3 OH, CN, C 2 H, HCN, HNC, HCO +, HC 3 N, CS, N 2 H +, SiO, HNCO, CH 3 CCH, CH 3 CN, SO 2, NS, NO (in addition to CO, H 2 CO, OH, H 2 O, C 3 H 2, and CH) Sources include: NGC 253, IC 342, NGC 6946, M82, NGC 4945, NGC 6946, Maffei 2, Arp 220, Mrk 231 mostly starbursts, some ULIRGs For many species rare isotopes are detected For many species multi-transition studies afford excitation analyses

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4 F x =160 erg cm -2 s -1

5 The interstellar medium in the Central Molecular Zone of our Galaxy The Central Molecular Zone (CMZ) huge Giant Molecular Cloud (GMC) complex: ~0.3º broad band around the center of our Galaxy from l = +1.9º to -1.1º. GMCs in CMZ have properties that are quite different from "normal" (i.e. spiral arm) clouds: they are much denser (n ~ 10 4 cm -3 vs. 10 2 cm -3 ), much warmer (60 K < T < 120 K vs. 10 – 20 K), and much more turbulent (  v ~ 10 – 20 km/s vs. a few km/s). HNCO 5 05 – 4 04 E l = 54 K Dahmen et al. 1997 300 pc

6 100 pc HNCO 5 05 – 4 04 Dahmen et al. 1997

7 Ott et al. 2005 ATCA – Ott, Weiss, Henkel, & Walter (2005) NH 3 in NGC 253 ~ 24 GHz

8 The allure of absorption spectroscopy

9 Impellizzeri et al. 2008 CH 3 OH 5 1 – 4 0 A +

10 CH 3 OH OH 16671665 MHz Impellizzeri et al. 2008 Hagiwara et al. 2004

11 Formaldehyde 6 cm line GBT Mangum, Darling, Menten, & Henkel 2008 EVLA: Can all be observed simultaneously with the 6.7 GHz CH 3 OH + 7 OH lines + …

12 NH 3 (3,3) 23870.1 GHz NH 3 (1,1) 23.6945 GHz NH 3 (2,2) 23.7226 GHz OH 2  3/2 J=9/2 23817.6/26.6 GHz 23 K 64 K 123 K 511 K! Arp 220 ATCA – Ott, Henkel, Weiss, & Walter (2005)

13 1343 MHz 6731 MHz 4488 MHz 9423 MHz Arp 220 Salter et al. 2008 Vibrationally Excited HCN

14 HCN l-type transitions (GHz) E(K)/1.44 J 448.9430 715 1 1346.7652 721 2 2693.3388 730 3 4488.4723 742 4 6731.9105 756 5 9423.3348 774 6 12562.3629 795 7 16148.5495 818 8 20181.3862 845 9 24660.3100 875 10 29584.6600 907 11 34953.7600 942 12 40766.9000 981 13 47023.2000 1022 14 53721.7150 1067 15

15 Thorwirth et al. 2003

16 l-type doublet vibrationally excited HCN lines need 14  m radiation for their excitation and, thus probe mid-IR radiation field unaccessible by other means (due to high opactity)

17 Cesaroni & Walmsley 1991

18 4765 MHz 4660 MHz 4750 MHz 6017/6030/ 6035/6049 MHz 7761 MHz 7820 MHz Rotationally Excited OH Absorption toward Arp 200 Salter et al. 2008 Can all be observed simultaneously with the EVLA Henkel et al. 1987 Henkel et al. 1986

19 Methanimine CH 2 NH 1 10 – 1 11 5290 MHz Arp 220 Salter et al. 2008 EVLA 1  10 min, 1 polz’n Detected in Galactic center region by Godfrey et al. (1973)

20 Chemical Diversity in Hot Molecular Cores (Wyrowski et al. 1999) Hot Cores hot (>150 K) dense (>10 6 cm -3 ) compact (a few thousand AU) 10 4 – 10 5 L  The starburst region inside Arp 220 resembles one gigantic hot core

21 Intermediate Redshift Molecular Absorption Toward Radio-loud (and preferably mm-loud) “Red” QSOs Gravitational lens systems

22 MERLIN 5 GHzPatnaik et al. 1993 Subrahmanyan et al. 1990 VLA 15 GHz B0218+357PKS 1830–211

23 B0218+357 Wiklind & Combes 1995 (from HI absorption, Carilli et al. 1993)

24 HST ACS F814W York et al. 2005 B-image 70 mas from galaxy center (~500 pc) A-image 330 mas from galaxy center (~2.3 kpc) B0218+357 Similar picture in PKS 1830–211

25 CASTLES Menten et al. 1999 (VLA) PKS 1830-211

26 VLA: Menten, Carilli, & Reid 1999 PKS 1830–211 z = 0.88582 So far (mostly) Q-band Note the abyssmal spectral resolution Very many lines can be observed simultaneously with the EVLA in all its frequency bands

27 Energy level diagram NH 3 Metastable levels (J = K) The versatile ammonia molecule – molecular cloud thermometer

28 NH 3 toward B0218+357 |  /  | < 1.8 10 -6 Murphy, Flambaum, Muller, & Henkel 2008

29 15.17 GHz 12.56 GHz E = 23 K E = 1036 K NH 3 toward PKS 1830-211 Henkel, Braatz, Menten, & Ott 2008 Can all be observed simultaneously with the EVLA

30 Background continuum between 6.5 and 8 Jy Apparent optical depths between 0.03 and 0.0008

31 NH 3 T kin ~ 70 K for 80-90% of the ammonia column T kin > 600 K for the remaining 10-20% Weird! This is supposed to be a normal molecular cloud in a random spiral arm location!

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33 APEX - The Atacama Pathfinder Experiment APEX - The Atacama Pathfinder Experiment

34 H2OH2O NH 3 APEX Observations of the Ortho-Ground State Lines of H 2 O and NH 3 Menten et al. 2008 Comparison of redshifts of NH 3 inversion lines and NH 3 rotation line will yield excellent limit on  / 

35 CASTLES CfA-Arizona Space Telescope LEns Survey of gravitational lenses The EVLA’s improved continuum sensitivity will allow self calibration on weak sources and, thus, allow long integrations. This, combined with the wide bandwidths/many channels, will make blind searches for redshifted absorption feasible.

36 Covering the whole redshift range with the EVLA Current Frequency Coverage Additional EVLA Coverage © Rick Perley@NRAO BUT: Will not improve on present VLA for 0.6 for OH lines  Low frequency capability

37 Multi molecule/multi transition observations with the EVLA will probe the hot, dense molecular gas in (even the most extreme) starburst environments allow fascinating studies of the (alien) interstellar media of normal, gas-rich distant galaxies, incl. magnetic field strength measurements provide ever more stringent limits on the evolution of fundamental constants over cosmic history

38 Thanks for your attention


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