what is millimetre-wave astronomy and why is it different?

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What is Millimetre-Wave Astronomy and why is it different? Michael Burton University of New South Wales

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What is Millimetre-Wave Astronomy and why is it different?. Michael Burton University of New South Wales. Some Millimetre Basics. MM: 1–~12mm, Sub-MM: 0.3–1mm CMBR (T = 2.7K  = 1mm ) Molecular rotational lines Polar molecules (have dipole moment) eg CO (E 1 = 5K), HCN, CS, HCO + - PowerPoint PPT Presentation

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Page 1: What is  Millimetre-Wave Astronomy and why is it different?

What is Millimetre-Wave Astronomyand why is it different?

Michael BurtonUniversity of New South Wales

Page 2: What is  Millimetre-Wave Astronomy and why is it different?

Some Millimetre Basics• MM: 1–~12mm, Sub-MM: 0.3–1mm• CMBR (T = 2.7K = 1mm)• Molecular rotational lines

– Polar molecules (have dipole moment)eg CO (E1 = 5K), HCN, CS, HCO+

• Cold thermal continuum (dust)– Thermal processes: F ~ B ~ 2kT2/c2 . x

• Problem: Atmosphere (O2, H2O)……

Page 3: What is  Millimetre-Wave Astronomy and why is it different?

The Millimetre Advantage

• Thermal Processes B 0.5-2 2

• Decay Rates (linear molecules) 3 • Doppler Widths 0.5 [?]• Level Population (T>>TJ; gJJ) • Number of Photons -1

• Energy • Spatial Resolution -1

Page 4: What is  Millimetre-Wave Astronomy and why is it different?

Transparancies

• Electromagnetic Spectrum• MM transmission for 4mm H2O

• MM transmission for 11mm H2O• Some bright MM-lines

Page 5: What is  Millimetre-Wave Astronomy and why is it different?

Brightness Temperature

Page 6: What is  Millimetre-Wave Astronomy and why is it different?

Atmospheric Transmission

Page 7: What is  Millimetre-Wave Astronomy and why is it different?

The 3mm Millimetre Spectrum

Page 8: What is  Millimetre-Wave Astronomy and why is it different?

Physical Parameters you can derive!

• Temperature: Tex, TBrightness

• Density: nH2 (~ncrit range of densities present!)

• Column Density: N (when optically thin)• Optical Depth: (use isotope ratios)• Mass (with scale length)• Abundances: different species• Velocities: line widths, centres, shapes

Infall, outflow, mass transfer rates

Constrain the properties of your source!!

Page 9: What is  Millimetre-Wave Astronomy and why is it different?

16272-4837SEST molecular line survey

–Gradient: Trot = 27 ± 4 K

–Intercept: N(H2) = 1 x 1024 cm-2

( comes in as well)

– Size + Column: n(H2) = 6 x 105 cm-3

– With Volume: Mass = 6 x 103 M

Garay et al, 2002

Page 10: What is  Millimetre-Wave Astronomy and why is it different?

16272-4837: SEST kinematical studies

– Evidence for infall(profile of optically thick lines)

- Modelling: Vinfall ~ 0.5 km s-1

- Speed + Density + Size:

dMinfall/dt ~10-2 M yr-1

– Evidence for outflow from wings- Extent: Voutflow = 15 km s-1

Brooks et al, 2002

OpticallyThick

OpticallyThin

WideWings

Page 11: What is  Millimetre-Wave Astronomy and why is it different?
Page 12: What is  Millimetre-Wave Astronomy and why is it different?

Mopra: Current Capabilities

• 22-m Telescope for > ~3mm• 85–115 GHz SIS receiver (2.6 – 3.5 mm)• 35” beam @ 100 GHz• Tsys ~ 150K(@85GHz) – 300K (@115GHz)• Beam Efficiency:

mb (86 GHz) = 0.49, mb (115 GHz) = 0.42 xb (86 GHz) = 0.65, xb (115 GHz) = 0.55

• Bandwidth 64, 128 or 256 MHz (200 - 800 km/s)• 1024 Channels (0.2 - 0.8 km/s per channel)• 2 Polarizations

– 1 frequency or 1 polarization + SiO 86 GHz• Must Nod – No chopping• OTF Mapping

Page 13: What is  Millimetre-Wave Astronomy and why is it different?

Methanol Maser-selected Hot Molecular Core SurveyCH3CN CH3OH HCO+ H13CO+ N2H+ HCN HNC

7 lines; 86 Sources

Purcell

Page 14: What is  Millimetre-Wave Astronomy and why is it different?

‘On the Fly’ Mapping with Mopra:The Horsehead Nebula

Optical 12CO 13CO

6 arcminTony Wong

Page 15: What is  Millimetre-Wave Astronomy and why is it different?

Tony Wong 0.17 km/s channel spacing

Page 16: What is  Millimetre-Wave Astronomy and why is it different?

OTF Mapping Specifications

• For a 300” x 300” map:– ~1400 spectra (31 x 46)– ~35” resolution– 0.17 km/s resolution – 120 km/s bandwidth– Dual polarization ~ 0.3K per channel, per beam– ~70 minutes / grid– Upto 7 grids / transit– Processed with LIVEDATA +

GRIDZILLA packages

QuickTime™ and aTIFF (LZW) decompressor

are needed to see this picture.

Page 17: What is  Millimetre-Wave Astronomy and why is it different?

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

The DQS in 13CO: Mopra OTF Mapping

Page 18: What is  Millimetre-Wave Astronomy and why is it different?

How many photons have we lost (or gained)?

00sec(z)

z

Signal on-source:

( ){ })sec()sec( 001 zsou

zatmrecSig eTeTTCT ττ −− +−+=

Trec

Tsou

Tatm

Page 19: What is  Millimetre-Wave Astronomy and why is it different?

Sky (Reference, Off)

Source (On)

Difference

Page 20: What is  Millimetre-Wave Astronomy and why is it different?

Some Radiative Transfer

•Radiative Transfer dI/ds = - I +

•Kirchoff (LTE) / = B(T)

Radiative Transfer dI/d = I + B(T)

•Solution I(s)= I(0)e- (s) + B(T)(1 - e- (s))

Source Atmosphere

Page 21: What is  Millimetre-Wave Astronomy and why is it different?

Obtaining Data:Signal from Source and Reference

• TSig = C{TR+TA(1-e-0secz)+TS e-0secz}• TRef = C{TR+TA(1-e-0secz)}• [TSig-TRef]/[TRef] = TS e-0secz

/ {TR+TA(1-e-0secz)}

Show Plots of Opacity + Brightness Temperature

• TBB = C{TR+TA}• [TSig-TRef]/[TBB - TRef] = TS/TA

Page 22: What is  Millimetre-Wave Astronomy and why is it different?

Calibrating Data:Gated Total Power

• GTPRef = C’ TRef

• GTPPaddle = C’{TA + TR}

• [GTPPaddle - GTPRef] / GTPRef

= TAe- 0secz / {TR+TA(1-e-0secz)}

• GTPHot - GTPCold = C’{THot - TCold} Atmosphere Liquid Nitrogen

Page 23: What is  Millimetre-Wave Astronomy and why is it different?

Calibrating Data:

• {[TSig-TRef]/[TRef]} / {[GTPPaddle - GTPRef] / GTPRef }

= TSource / TAtmosphere

• Actually TSource = T’Source / Efficiency– Usually written as TMB = TA

* / (note the different notation)

Page 24: What is  Millimetre-Wave Astronomy and why is it different?

Mopra Upgrades

• 8 GHz Digital Filter Bank– Zoom modes– 4(?) lines simultaneously

• MMIC receiver– Easier tuning– Higher Tsys

– May loose 115 GHz end?• 7 mm receiver

– New ATNF project?• Focal Plane Array???• Ultra-wide band correlator???

– Needs source of funds……

Page 25: What is  Millimetre-Wave Astronomy and why is it different?

Australia’s MM–Wave Radio Telescopes

3 mm

12 mm

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Page 26: What is  Millimetre-Wave Astronomy and why is it different?
Page 27: What is  Millimetre-Wave Astronomy and why is it different?

Australia Telescope Compact Array• National Facility

– Built for 1–10 GHz operation• MM-upgrades

– 3 mm (85-~105 (115) GHz)• 5 x 22m antennas• EW-array + NS-spur

– Currently 84.9-87.3+88.5-91.3 GHz– 12 mm (22-25 GHz)

• 6 x 22m antennas• 2 GHz bandwidth upgrade • 7 mm (45 GHz) upgrade planned

– 6 antennas• FPAs???

– With ultra-wide-band correlators??

Page 28: What is  Millimetre-Wave Astronomy and why is it different?

Water Vapour and Phase Fluctuations

Page 29: What is  Millimetre-Wave Astronomy and why is it different?

MillimetreInterferometry

Poses special challenges:• Significant atmospheric opacity, mostly due to H2O

• Fluctuations in H2O produce phase shifts• These increase with both baseline and frequency• Instrumental requirements (e.g. surface, pointing, baseline

accuracy) are more severe• Need more bandwidth to cover same velocity range (1

MHz (mm) km/s)

R SaultDesai 1998

Brightness Temperature H2O Turbulence Seeing

Page 30: What is  Millimetre-Wave Astronomy and why is it different?

ALMAAtacama Large Millimetre Array

Page 31: What is  Millimetre-Wave Astronomy and why is it different?

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Antarctica??