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Why do we need interferometry? Measuring the gas distribution and rotation in disk galaxies: radio observations with interferometer arrays and aperture.

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Presentation on theme: "Why do we need interferometry? Measuring the gas distribution and rotation in disk galaxies: radio observations with interferometer arrays and aperture."— Presentation transcript:

1 Why do we need interferometry? Measuring the gas distribution and rotation in disk galaxies: radio observations with interferometer arrays and aperture synthesis Why is surface brightness independent of distance? What is the relation between R 25 and H I radius? Radial velocity observations: spider diagrams, evidence of mergers, polar rings

2 Diffraction limit

3 The angular resolution of a 2-element interferometer

4 VLA = Very Large Array, NM

5 A typical radio-map at 20cm Optical image, for comparison : (not to scale) Aperture synthesis at VLA

6 VLBA = Very Long Baseline Array Resolution ~0”.01 at wavelength 21cm

7 NGC 7331 - how far out can we trace the visible light from this galaxy? Until it is a tiny fraction of the sky brightness. Surface brightness of the moonless sky at B band is 22.7 mag/arcsec^2 and grows at I-band to 19.9 mag/arcsec^2 Therefore, we choose the following surface brightness in blue light: I B = 25 mag/arcsec^2 as practically the lowest possible for measurement, thus defining the maximum extent of the visible light from a galaxy: R 25 At radio wavelengths, the sky is much darker than in the visible, so we can see the atomic hydrogen further than the stars in any galaxy.

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9 Why do we use surface brightness (mag/arcsec^2) so much in extragalactic photometry? ( e.g., Freeedman law I B ( 0 ) =21.7 mag ) Because it’s independent of the distance to the object! D=1 D=2 D=4 D=8 A=8 A=4 A=2 A=1 I=1 I =1 I=1 I=1 (try to see that all the lamps in the park seem equally bright, only gradually smaller, as long as they form extended images on the retina) L=1 (luminosity) R=1 (physical radius) D= distance Observed total flux = L/(4 pi D^2) A= angular diameter ~ 1/D I = surface brightness ~ L/(4 pi D^2)*A^2 ~D^0 We often measure the optical size of a galaxy as the radius R 25 at which I B = 25 mag/arcsec^2 A lamp

10 Gas is seen further than the stars in any given galaxy

11 Diffuse HI gas ejected by supernovae?

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13 Evidence of past galaxy mergers How a slit spectrum of such a galaxy may look like: space VrVr

14 A polar ring galaxy: evidence of merger

15 Theoretical spider diagram for a simple rotation curve (axisymmetric disk assumed): set of isovelocity curves in spatially resolved Doppler maps

16 H I Sample spider diagram (can you see which side is approaching and which receding?)


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