Max Voronkov Software Scientist – ASKAP 14th December 2010

Slides:



Advertisements
Similar presentations
Masers and Massive Star Formation Claire Chandler Overview: –Some fundamental questions in massive star formation –Clues from masers –Review of three regions:
Advertisements

High-Mass Star-Forming Regions in the G333 Cloud Indra Bains & the DQS team.
Andrew Walsh, James Cook University Narrated by James Green (CASS) – thanks Jimi! (Psshhh aaahhh sssss push it) The Case for High Frequency Line Observations.
X-ray Properties of Five Galactic SNRs arXiv: Thomas G. Pannuti et al.
The Galactic Center: Molecular Line Mapping with Broadband Spectrometers Jürgen Ott ESO 3D Meeting 11 June 2008 The Galactic Center: Molecular Line Mapping.
A MOPRA CS(1-0) demonstration survey of the Galactic plane G. Fuller, N. Peretto, L. Quinn (University of Manchester UK), J. Green (ATNF ) All dust continuum.
Studying circumstellar envelopes with ALMA
Loránt Sjouwerman, Ylva Pihlström & Vincent Fish.
21 November 2002Millimetre Workshop 2002, ATNF First ATCA results at millimetre wavelengths Vincent Minier School of Physics University of New South Wales.
Portrait of a Forming Massive Protocluster: NGC6334 I(N) Todd Hunter (NRAO/North American ALMA Science Center) Collaborators: Crystal Brogan (NRAO) Ken.
Radio Science and PILOT Tony Wong ATNF/UNSW PILOT Workshop 26 March 2003.
SMA Observations of the Binary Protostar System in L723 Josep Miquel Girart 1, Ramp Rao 2, Robert Estalella 3 & Josep Mª Masqué 3 1 Institut de Ciències.
Spitzer mid-IR image of the DR21 region in the Cygnus-X molecular complex Image Credit: NASA, Spitzer Space Telescope.
EGOs: Massive YSOs in IRDCs Ed Churchwell & Claudia Cyganowski with co-workers: Crystal Brogan, Todd Hunter, Barb Whitney Qizhou Zhang Dense Cores in Dark.
Variable SiO Maser Emission from V838 Mon Mark Claussen May 16, 2006 Nature of V838 Mon and its Light Echo.
Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert C. Byrd Green Bank Telescope Very Long Baseline Array EVLA Observations of.
Class I methanol masers in the regions of high-mass star-formation Max Voronkov Software Scientist – ASKAP In collaboration with: Caswell J.L., Ellingsen.
Millimetre Astronomy with the Australia Telescope Max Voronkov Software Scientist – ASKAP 12 th June 2009.
Star Formation Research Now & With ALMA Debra Shepherd National Radio Astronomy Observatory ALMA Specifications: Today’s (sub)millimeter interferometers.
TURBULENCE AND HEATING OF MOLECULAR CLOUDS IN THE GALACTIC CENTER: Natalie Butterfield (UIowa) Cornelia Lang (UIowa) Betsy Mills (NRAO) Dominic Ludovici.
What is Radio Astronomy? MIT Haystack Observatory This material was developed under a grant from the National Science Foundation.
Masers observations of Magnetic fields during Massive Star Formation Wouter Vlemmings (Argelander-Institut für Astronomie, Bonn) with Gabriele Surcis,
MASERS Johns Hopkins University, Tuesday, December 12 Microwave Amplification by the Stimulated Emission of Radiation (S) connotes plural.
ASTR112 The Galaxy Lecture 8 Prof. John Hearnshaw 12. The interstellar medium (ISM): gas 12.1 Types of IS gas cloud 12.2 H II regions (diffuse gaseous.
Water maser emission in Bok globules Bok Globules Bok globules are small (
Rotating Disks around O-type Young Stars in NGC7538 IRS1 3D Gas Dynamics from Methanol Masers observed with the EVN Ciriaco Goddi.
Mid-infrared Spectral Evolution of Post-AGB Stars Kevin Volk, Gemini Observatory.
Molecular Gas and Dust in SMGs in COSMOS Left panel is the COSMOS field with overlays of single-dish mm surveys. Right panel is a 0.3 sq degree map at.
Hydroxyl Emission from Shock Waves in Interstellar Clouds Catherine Braiding.
HOPS – The H 2 O southern Galactic Plane Survey Image Courtesy: Cormac Purcell.
А.М. Sobolev (Ural Federal University, Ekaterinburg, Russia) S. Deguchi, W.D. Watson, D.M. Cragg, A.B. Ostrovskii, M.A. Voronkov, E.C. Sutton, V.S. Strelnitskii,
The Incredible 6.7 GHz Methanol Masers: A key to understanding high-mass star formation. Jimi Green (for Gary Fuller) CSIRO Astronomy & Space Science,
VLASS – Galactic Science Life cycle of star formation in our Galaxy as a proxy for understanding the Local Universe legacy science Infrared GLIMPSE survey.
The Role of Parkes in Southern Maser VLBI Simon Ellingsen University of Tasmania.
Masers as evolutionary tracers of high-mass star formation Shari BreenSimon Ellingsen Bolton FellowJames Caswell 15th September 2010.
MALT Survey meeting / Masers at 7 and 3mm Max Voronkov Software Scientist – ASKAP 04 th June 2009.
Class I methanol masers in the regions of high-mass star formation Max Voronkov Software Scientist – ASKAP In collaboration with: Caswell J.L., Ellingsen.
Molecular Clouds in in the LMC at High Resolution: The Importance of Short ALMA Baselines T. Wong 1,2,4, J. B. Whiteoak 1, M. Hunt 2, J. Ott 1, Y.-N. Chin.
Imaging Molecular Gas in a Nearby Starburst Galaxy NGC 3256, a nearby luminous infrared galaxy, as imaged by the SMA. (Left) Integrated CO(2-1) intensity.
Class I methanol masers and evolutionary stage of star- formation Max Voronkov Software Scientist – ASKAP In collaboration with: Caswell J.L., Ellingsen.
Observing Strategies at cm wavelengths Making good decisions Jessica Chapman Synthesis Workshop May 2003.
Methanol maser and 3 mm line studies of EGOs Xi Chen (ShAO) 2009 East Asia VLBI Workshop, March , Seoul Simon Ellingsen (UTAS) Zhi-Qiang Shen.
Masers Surveys with Mopra: Which is best 7 or 3 mm? Simon Ellingsen, Maxim Voronkov & Shari Breen 3 November 2008.
Using masers as evolutionary probes in the G333 GMC (as well as some follow up work) Shari Breen, Simon Ellingsen, Ben Lewis, Melanie Johnston-Hollitt,
Methanol Masers in the NGC6334F Star Forming Region Simon Ellingsen & Anne-Marie Brick University of Tasmania Centre for Astrophysics of Compact Objects.
Multiple YSOs in the low-mass star-forming region IRAS CONTENT Introduction Previous work on IRAS Observations Results Discussion.
Radio Galaxies Part 3 Gas in Radio galaxies. Why gas in radio galaxies? Merger origin of radio galaxies. Evidence: mainly optical characteristics (tails,
Nichol Cunningham. Why? Massive stars are the building blocks of the universe. Continuously chemically enrich our galaxy. Release massive amounts of energy.
GBT Future Instrumentation Workshop Fixing the frequency coverage hole in C-Band Jagadheep D. Pandian Cornell University.
Early O-Type Stars in the W51-IRS2 Cluster A template to study the most massive (proto)stars Luis Zapata Max Planck Institut für Radioastronomie, GERMANY.
1 1 CORNISH WORKSHOP Leeds, 13 th April 2007 James Green The Methanol Multibeam Project Project MMB.
Low-luminosity Extragalactic H 2 O Masers Yoshiaki Hagiwara ASTRON.
Cosmic Masers Chris Phillips CSIRO / ATNF. What is a Maser? Microwave Amplification by Stimulated Emission of Radiation Microwave version of a LASER Occur.
Massive Star-Formation in G studied by means of Maser VLBI and Thermal Interferometric Observations Luca Moscadelli INAF – Osservatorio Astrofisico.
Lecture 3 – High Mass Star Formation
Surveys of the Galactic Plane for Massive Young Stellar Objects
Portrait of a Forming Massive Protocluster: NGC6334 I(N)
New Class I methanol masers
SWAN: Survey of Water & Ammonia in Nearby Galaxies
High Resolution Submm Observations of Massive Protostars
Signposts of massive star formation
Class I methanol masers and shocks
Early indications of performance
A Search for water masers in High-redshift un-beamed AGNs: T. Ghosh, S
MASER Microwave Amplification by Stimulated Emission of Radiation
107/108 GHz methanol masers with ALMA
Submillimeter water megamasers in nearby AGNs
Millimeter Megamasers and AGN Feedback
Circumstellar SiO masers in long period variable stars
EVN observations of OH maser burst in OH
Presentation transcript:

Max Voronkov Software Scientist – ASKAP 14th December 2010 Image credit: ALMA Masering ALMA Max Voronkov Software Scientist – ASKAP 14th December 2010

What is a maser? A spectral line formed under special conditions (population inversion) Narrow lines and high brightness temperature (for strong masers, i.e. <-1) Possible in a limited number of transitions Sensitive to physical conditions It is harder to create high-frequency maser Bright masers are often used as tools: to locate targets, to measure parallax, etc Pumping process involves a delicate balance between radiative and collisional transitions. It is not understood well for some masers

Where do we find them? Star-forming regions in our Galaxy High-mass: OH, H2O, CH3OH (both classes), a few SiO, NH3 and formaldehyde Low- and intermediate-mass: OH, H2O, CH3OH (class I) Supernova remnants: OH Late-type stars and circumstellar environment OH, H2O, SiO, SiS, possibly HCN and HC3N Extragalactic masers (also known as kilomasers, megamasers, etc) Star-forming regions in LMC and nearby galaxies (OH, H2O, class II CH3OH) Late-type stars in LMC (SiO, OH) Galactic nuclei (H2O)

Two classes of methanol masers Class I methanol (CH3OH) masers Collisional excitation (e.g. by shocks) Regions of star formation (low-mass ones as well) Usually offset from YSOs (up to a parsec) Many maser spots scattered over tens of arcsec Widespread masers: 36, 44, 84, 95 GHz Rare/weak: 9.9, 23.4, series at 25, 104.3 GHz Class II methanol (CH3OH) masers Radiational excitation (by infrared from YSO) Regions of high mass star formation only Located at the nearest vicinity of YSOs Usually just one maser spot at the arcsec scale Widespread masers: 6.7, 12 GHz Rare/weak: 19.9, 23, 85/86, 37/38, 107, 108 GHz

Masers as evolutionary clocks Image credit: Cormac Purcell Image credit: Simon Ellingsen Ellingsen (2006): class I masers tend to be deeply embedded younger. However recent data show that a significant number of class I masers trace relatively evolved stage of high-mass star-formation Whether class I masers can precede class II masers is unclear

I  methanol From now on, I will concentrate on (Galactic) methanol masers For a good review of submillimetre masers on other molecules see E.M.L. Humphreys, 2007, IAUS 242, 471 I will discuss separately class I and class II methanol masers what we already know from low frequency observations which transitions can be observed with ALMA

My understanding of early ALMA Masers have narrow lines. For methanol we aim at 0.1 km/s resolution ALMA band Frequency Required resolution Correlator mode 3 84-116 GHz 40 kHz 62.5 MHz/2048 channels (mode 18) 6 211-275 GHz 90 kHz 7 275-373 GHz 125 kHz As above, or 500 MHz/4096 channels (mode 9) 9 602-720 GHz 240 kHz 500 MHz/4096 channels (mode 9) The full 2 GHz bandwidth mode is not very useful for masers

G9.62+0.20E: strong class II maser Fine structure at VLBI resolutions (12 GHz maser) 6.7 GHz and 12 GHz masers are the strongest class II methanol masers 107 and 108 GHz transitions are popular weaker masers Image: Goedhart et al. (2005)

ATCA and CABB at 3mm band Frequency below 105 GHz!

Methanol maser series Red is class I Green is class II Interestingly, all but one class II maser series go downwards and eventually terminate at the lowest possible level for that particular series Class I masers are more important for ALMA

Class II methanol maser series J1-(J+1)o A+ Most widespread class II methanol maser series Expect a single cluster of spots at arcsec scale (class II maser) Starts with strongest and most common maser at 6.7 GHz (5000 Jy) But not very impressive for early ALMA except for 107 GHz transition Similar situation is for the second strongest 12.2 GHz transition. Only 108 GHz seems to be useful for early ALMA Transition Approximate frequency 51-60 A+ 6.7 GHz 31-40 A+ 107 GHz 21-30 A+ 157 GHz 11-20 A+ 206 GHz Known masers

Class II methanol maser series J-2-(J+1)-1 E Weak class II methanol maser series (bright in the isotropic case, i.e. no beaming and same optical depth in all directions) Expect a single cluster of spots at arcsec scale (class II maser) Several sources known at 37 GHz (strongest ~ 300 Jy), to be followed up with ATCA in March (PI: S.Ellingsen) Transition Approximate frequency 7-2-8-1 E 37 GHz 6-2-7-1 E 85 GHz 3-2-4-1 E 230 GHz 2-2-3-1 E 279 GHz Known masers

Class II methanol maser series J1-(J+1)2 A- Rare class II methanol maser series (narrow range of density and methanol abundance, quite high densities of 107-108 cm-3) Expect a single cluster of spots at arcsec scale (class II maser) Only two reliable detections: W33(OH) (~10 Jy at 23.1 GHz) and NGC6334-I (~35 Jy at 23.1 GHz) + possible maser in NGC 7538 (0.5 Jy) Transition Approximate frequency 92-101 A+ 23.1 GHz 72-81 A+ 111 GHz 42-51 A+ 247 GHz 32-41 A+ 294 GHz 22-31 A+ 340 GHz Known maser

Class II methanol maser series J2-(J+1)1 A- Rare class II methanol maser series (it is not very clear to me why) Expect a single cluster of spots at arcsec scale (class II maser) Only one known source - W3(OH) Lack of extensive searches (so these masers may be more common than we think they are) Transition Approximate frequency 82-91 A- 28.9 GHz 72-81 A- 81 GHz 42-51 A- 235 GHz 32-41 A- 285 GHz 22-31 A- 335 GHz Known maser

Class II methanol maser series J2-(J-1)3 A± Rare class II methanol maser series (seem to require rather low densities about 104 cm-3) Pair of maser transitions for A+ and A- methanol at close frequencies Expect a single cluster of spots at arcsec scale (class II maser) Several sources known at 38/87 GHz The only class II series which does not terminate Transition Approximate frequency 62-53 A± 38 GHz 72-63 A± 87 GHz 102-93 A± 233 GHz 112-103 A± 281 GHz 122-113 A± 330 GHz 182-173 A± 624 GHz 192-183 A± 673 GHz Known masers

G357.97-0.16 (good maser target for ALMA) Red contour shows 12mm continuum (50% of the peak) Squares are class II methanol masers at 6.7 GHz Crosses are water masers Circle shows position of rare class I masers Background is 8.0µm Spitzer IRAC image Northern source has an OH maser, the associated H2O maser has a large velocity spread with almost continuous emission across 180 km/s

G343.12-0.06 (outflow association) Some maser spots are associated with an outflow traced by H2 emission Rare masers are confined to a single spot near the brightest H2 knot

G309.38-0.13 (high-velocity feature at 36 GHz) Background: Spitzer IRAC data Red: 8.0 µm, green: 4.5 µm, blue: 3.6 µm Excess of 4.5 µm may be a signature of Shocks Red contours: peak of the 36 GHz emission across the velocity cube Circles/crosses: maser spots (36/44 GHz) 36 GHz is one of the widespread Class I maser transitions

Association with expanding Hii regions? Class I masers may be associated with ionisation shocks driven by an expanding HII region into surrounding molecular cloud This result is currently based on observations of 9.9 GHz masers (need higher temperature and density to form than 36/44 GHz) but should apply to other class I methanol masers as well Another possible example (but it has an outflow as well) Crosses: 9.9 GHz masers Open boxes: 6.7 GHz maser (Caswell 2010) Contours: 8.6 GHz continuum Grayscale: Spitzer 4.5µm Grayscale: NH3 (Ho et al. 1986; Garay et al. 1998) G331.13-0.24 W33-Met (G12.80-0.19) G19.61-0.23

Class I methanol maser series J0-(J-1)1 A+ The most widespread and strong class I methanol maser series Strongest known is ~ 500 Jy at 44 GHz Spots (sub-arcsec size) scattered over a large area of 1 arcmin or more Low contamination from thermal emission Transition Approximate frequency 70-61 A+ 44 GHz 80-71 A+ 95 GHz 110-101 A+ 251 GHz 120-111 A+ 303 GHz 130-121 A+ 356 GHz 180-171 A+ 623 GHz 190-181 A+ 677 GHz Known masers

Class I methanol maser series J-1-(J-1)0 E Second strongest class I methanol maser series, widespread Spots (sub-arcsec size) scattered over a large area of 1 arcmin or more Lower excitation energy than for J0-(J-1)1 A+, so thermal emission is more common (at least at 36 GHz) Transition Approximate frequency 4-1-30 E 36 GHz 5-1-40 E 84 GHz 6-1-70 E 133 GHz 8-1-70 E 229 GHz 9-1-80 E 279 GHz 10-1-90 E 327 GHz 16-1-150 E 623 GHz 17-1-160 E 673 GHz Known masers

Class I methanol maser series J-1-(J-1)-2 E Rare class I methanol maser series, traces strongest shocks Usually just a single maser spot (sub-arcsec size) Only few sources are known Strongest maser in G357.97-0.16 (~70 Jy at 9.9 GHz) Transition Approximate frequency 9-1-8-2 E 9.9 GHz 11-1-10-2 E 104.3 GHz 14-1-13-2 E 243 GHz 15-1-14-2 E 287 GHz 16-1-15-2 E 331 GHz 23-1-22-2 E 608 GHz 24-1-23-2 E 642 GHz 25-1-24-2 E 675 GHz 26-1-25-2 E 706 GHz Known masers

Class I methanol maser series J1-(J-1)2 A- Rare class I methanol maser series, traces strongest shocks Very new maser series, properties are not well understood yet Expect a single maser spot (sub-arcsec size) Only two sources known: G357.97-0.16 (~20 Jy at 23.4 GHz) and G343.12-0.06 (~7 Jy at 23.4 GHz) Transition Approximate frequency 101-92 A- 23.4 GHz 111-102 A- 76.3 GHz 141-132 A- 237 GHz 151-142 A- 291 GHz 161-152 A- 346 GHz 211-202 A- 625 GHz 221-212 A- 681 GHz Known maser

What would I do with ALMA? Look for various high-frequency class I methanol masers There are several good targets studied in detail with ATCA Tracing kinematics and morphology of shocks (outflows, expanding HII regions) at high resolution using widespread masers (e.g. 229 GHz) Start with known widespread maser transition, e.g. 229 GHz Constraining maser models Many new transitions are very important, currently number of transitions ~ number of unknowns in the model What is the highest frequency methanol maser? Applicable to both class I and class II, but more important for class I Follow up of the southern class II targets at 107/108 GHz Accurate positions, high-resolution maps to compare with 6.7-GHz Easy project with guaranteed success In addition, masers are good test targets

Thank you Australia Telescope National Facility Max Voronkov Contact Us Phone: 1300 363 400 or +61 3 9545 2176 Email: enquiries@csiro.au Web: www.csiro.au Australia Telescope National Facility Max Voronkov Software Scientist (ASKAP) Phone: 02 9372 4427 Email: maxim.voronkov@csiro.au Web: http://www.narrabri.atnf.csiro.au/~vor010 Thank you