radio astronomy intro, part 1 · 2011-01-19 · 1 astronomy 423 at unm radio astronomy radio...
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Astronomy 423 at UNM Radio Astronomy
Radio Astronomy Intro, part 1 Greg Taylor University of New Mexico Jan 19, 2011
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G. Taylor, Astr 423 at UNM
Course Goals
• To understand how radio astronomical instrumentation functions and is used in practice.
• To understand some of the exciting science carried out at radio wavelengths.
• To understand the astrophysical processes which give rise to radio emission
• A chance to see and work with real radio data from the Expanded Very Large Array, the Very Long Baseline Array, and the Long Wavelength Array
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G. Taylor, Astr 423 at UNM
Course Outline
• Exploring the Invisible Universe • Some basic information (radiative transfer, thermal
emission, electromagnetic waves) • Signals and noise, receivers • Antennas – Our Connection to the Universe • The Two-Element Interferometer • Aperture Synthesis techniques
– Connected element interferometers (EVLA) – Very Long Baseline Interferometry (VLBA) – Long Wavelength Interferometry (LWA)
• Synchrotron Emission and Magnetic Fields • Active Galactic Nuclei and their Jets • See the Syllabus for more details
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G. Taylor, Astr 423 at UNM
Course Methods
• Materials will be posted at: http://www.phys.unm.edu/~gbtaylor/astr423-2011/
• Weekly homework assignments • Reading assignments • Lectures
– Powerpoint slides (will be posted) – Traditional chalkboard lectures (not posted) – data reduction tutorials (~1 or 2, not posted)
• Two mid-term exams • Observing project with the VLBA (VLBA schedule by Feb 2 !) • A day at the EVLA observing/touring (Saturday Feb 19) • Homework analyzing our EVLA data and VLBA data • Written and oral reports based on the observations • Grad students will be expected to do some extra work (present
a hw solution, schedule observations, etc. - meet me to discuss)
• No final exam
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G. Taylor, Astr 423 at UNM
How to Use a Radio Telescope
1. Come up with a great idea 2. Write a compelling proposal 3. Submit your great proposal for review 4. Wait a while 5. Schedule the observations 6. Watch the observations take place 7. Calibrate the data 8. Make images and perform detailed analysis 9. Write up your results and submit them for publication
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G. Taylor, Astr 423 at UNM
How we will use the VLA/VLBA
1. Come up with a great idea (start thinking about this now!) 2. Write a compelling proposal (one paragraph) 3. Submit your great proposal for review (proposals due Tuesday Jan 25) 4. Wait a while (TAC decision on Jan 26; 2 hours EVLA observing and 4
hours of VLBA observing time to allocate) 5. Schedule the observations (by Feb 2 and 4 for VLBA and EVLA) 6. Watch the observations take place (EVLA tour Feb 19) 7. Calibrate the data (homework) 8. Make images and perform detailed analysis (homeworks & project) 9. Write up your results and submit them for publication (for a grade)
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G. Taylor, Astr 423 at UNM
How we will use the LWA
1. Learn how to install Front Ends in February 2. Wait for LWA to be completed in March 3. Take some data and practice RFI excision techniques 4. Make some images of the sky at long wavelengths 5. Look for transient radio sources
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G. Taylor, Astr 423 at UNM
The Very Large Array
• On Feb 19 the EVLA will be in B config
Angular resolution ~ 1” at 5 GHz, sensitivity = 58 microJy/beam in 10 minutes @ 5 GHz
Frequency range: 1 to 50 GHz
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G. Taylor, Astr 423 at UNM
Observing Constraints
• EVLA time should be nighttime (2h – 17h LST) so targets should be between RA 1:00:00 and 18:00:00 and Declination > -40:00:00
• EVLA Frequency range 1 – 50 GHz (avoid 15 GHz) • VLBA time can be at any RA, DEC > -20:00:00 • VLBA Frequency range 0.33 – 90 GHz (some gaps)
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G. Taylor, Astr 423 at UNM
The FULL Electromagnetic
Spectrum
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G. Taylor, Astr 423 at UNM
EM Radiation – basic properties
• speed of light = c = λ v c = constant = 3 x 1010 cm/s = 3 x 105 km/s λ has units of length (cm) - we will use c.g.s. units (mostly) v has units of 1/s (Hz)
• Photons carry energy depending on their frequency (or wavelength) E=hν
h = 6.63 x 10-27 erg s, ν is frequency, E energy h = 4.14 x 10-15 eV s • note: “high energy” astronomers (X-ray, Gamma Ray) usually use the corresponding energy rather than wavelength, i.e., 10 keV, 2 GeV For example: 1017 Hz = 0.4 keV
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G. Taylor, Astr 423 at UNM
Radio Window
spans a wide range of λ and ν from λ ~ 0.33 mm to ~ 20 m! (ν = 1300 GHz to 15 MHz )
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G. Taylor, Astr 423 at UNM
LWA
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G. Taylor, Astr 423 at UNM
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G. Taylor, Astr 423 at UNM
Radio High frequency cut off
- due to the troposphere layers
- H2O, O2 absorb incoming “high frequency” radio photons
- particularly bad spectral windows include: H2O at 22.2 GHz (1.35 cm) 183 GHz (1.63 mm) O2 at 60 GHz (5 mm) 119 GHz (2.52 mm)
- water/oxygen “band” features are closely spaced absorption lines - high frequencies good for molecular lines
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G. Taylor, Astr 423 at UNM
Because the main culprit for high frequency radio astronomy is WATER VAPOR in the atmosphere, you can improve your observing conditions!
- go to HIGH or DRY locations:
High Frequency Observing
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G. Taylor, Astr 423 at UNM
Atmospheric Opacity at the VLA and ALMA sites
Transmission of the atmosphere from 0 to 1000 GHz for the ALMA site in Chile, and for the VLA site in New Mexico
⇒ atmosphere little problem for λ > cm (most VLA bands up to 15 GHz) ⇒ some problems from 20 to 50 GHz
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G. Taylor, Astr 423 at UNM
Highest, driest telescope site: (~ 16,400 feet) Atacama desert, Northern Chile
Site of millimeter array telescope: ALMA
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G. Taylor, Astr 423 at UNM
ALMA prototype telescope (Vertex design): ~50 12-m telescopes!
ALMA 20
G. Taylor, Astr 423 at UNM
First ~12 ALMA Antennas now at high site.
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G. Taylor, Astr 423 at UNM
Radio Low frequency cut off
- due to the ionospheric layers
- free electrons in the ionosphere start to absorb low frequency radio radiation IF the frequency is LESS than the plasma frequency νp = 8.97 ne
1/2
where ne is the electron density (cm-3) and νp is in kHz
- ne does depend on solar activity! and day/night, location on Earth
- e.g., at night ν=4.5 MHz (66 m) daytime ν=11 MHz (27 m)
The LWA Project
State of New Mexico, USA
LWA-1
• 10-88 MHz Aperture Synthesis Telescope • 4 beams x 2 pol. x 2 tunings x 16 MHz • 2 all-sky transient obs. modes
• LWA-1 completed Spring 2011 • Goal of 53 LWA stations, baselines up to 400 km for resolution 2” at 80 MHz with mJy sensitivity • Cost is ~$1M/station
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G. Taylor, Astr 423 at UNM
Radio Frequency Interference
Grote Reber’s telescope and Radio Frequency Interference in 1938
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G. Taylor, Astr 423 at UNM
Average Spectrum at VLA site, Jan 14, 2009
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Radio Frequency Interference (RFI) 26
G. Taylor, Astr 423 at UNM
The Radio Sky
5 GHz image from 300 ft,Condon et al.
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G. Taylor, Astr 423 at UNM
Supernovae
Cass A Rudnick et al.
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G. Taylor, Astr 423 at UNM
A Young Supernova
SN 1993J Rupen et al.
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G. Taylor, Astr 423 at UNM
GRB 970508
• First GRB Afterglow detected in the radio • Size < 1019 cm (3 lt years) • absolute position to < 1 mas • Distance > 10000 lt years
Taylor et al 1997
Gamma Ray Bursts 30
G. Taylor, Astr 423 at UNM
R ~ (E/n)^1/8
Relativistic Expansion v ~ 0.96c
E ~ 10^53 ergs (isotropic equivalent)
Pihlstrom et al 2007
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The Duck
Gaensler et al.
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G. Taylor, Astr 423 at UNM
Giant Flare from the Magnetar SGR 1806-20
Gaensler et al 2005
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G. Taylor, Astr 423 at UNM
Star forming regions - Orion nebula (M42)
Yusef-Zadeh et al.
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Planetary Nebulae - NGC 7027
Hjellming et al.
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Normal Galaxies
M51
Beck et al.
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3C31
Active galaxy
Laing et al.
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Cygnus A – prototypical radio galaxy -- FR II
Carilli et al.
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G. Taylor, Astr 423 at UNM
1 kpc
Taylor et al.
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Quasar 40
G. Taylor, Astr 423 at UNM
J12448+4048
Baby radio galaxy
Tremblay et al. 2011
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G. Taylor, Astr 423 at UNM
Compact Symmetric Objects (CSOs) 42
G. Taylor, Astr 423 at UNM
3C279 with the VLBA
Wehrle et al. 2001, ApJS, 133, 297
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G. Taylor, Astr 423 at UNM
Why so many types of Active Galactic Nuclei?
We see AGN : • from different orientations • at different evolutionary stages • in different environments • with different instruments
Synchrotron Emission depends on the distribution of both relativistic particles and magnetic fields.
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G. Taylor, Astr 423 at UNM
Why we care about the environment:
• a black hole alone does not make for an AGN
• what are the fueling rates and fueling mechanisms?
• how is the jet collimated?
• what is the ambient magnetic field strength & topology?
• environment plays a key role in unified schemes
• investigate torus chemistry and physics
• Disturbed morphologies may indicate interactions with surrounding gas
• look for inflows/outflows
• use gas kinematics to weigh the central engine
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G. Taylor, Astr 423 at UNM
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G. Taylor, Astr 423 at UNM
Carilli & Taylor 2002 (ARA&A)
B ~ 10 µG
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G. Taylor, Astr 423 at UNM
Carilli & Taylor 2002 (ARA&A)
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G. Taylor, Astr 423 at UNM
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G. Taylor, Astr 423 at UNM
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G. Taylor, Astr 423 at UNM
KEY red = embedded blue = background black = control
Clarke et al.
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G. Taylor, Astr 423 at UNM
Feretti et al. 1998
WSRT at 90cm
B ~ 0.4 µG
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0218+35
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G. Taylor, Astr 423 at UNM
Astrophysics Talks
UNM institute for astrophysics seminar series Thursdays @ 2pm in PandA 190 next talk Jan 20: Greg, Rich, Steve, Justin … on “News from the Seattle AAS”
NRAO Colloquium Series Fridays @ 11am in PandA 190 broadcast from the Scientific Operations Center in Socorro
UNM Colloquium Series Fridays @ 4pm in 125 Dane Smith Hall
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G. Taylor, Astr 423 at UNM
Further Reading