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Spectral Line VLBI

Spectral Line VLBI. Chris Phillips JIVE The Netherlands. Spectral Line Sources. VLBI  High brightness temperatures Masers: Galactic OH, H 2 O, SiO, CH 3 OH Extragalactic OH, H 2 O Extra-galactic HI absorption. Image courtesy of Lincoln Greenhill, CfA VLBI Group See also:

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Spectral Line VLBI

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  1. Spectral Line VLBI Chris Phillips JIVE The Netherlands

  2. Spectral Line Sources • VLBI  High brightness temperatures • Masers: • Galactic • OH, H2O, SiO, CH3OH • Extragalactic • OH, H2O • Extra-galactic HI absorption

  3. Image courtesy of Lincoln Greenhill, CfA VLBI Group See also: Hernstein etal, 1999, Nature, 400, 539 Miyoshi etal, 1995, Nature, 373, 127

  4. SiO masers in TX Cam Movie courtesy of Phil Diamond, Jodrell Bank

  5. SiO masers in Orion BN/KL Greenhill etal, 1998, Nature, 396, 650

  6. 6.7-GHz methanol in G339.88-1.26

  7. HI absorption towards NGC 3894 Peck & Taylor, 2000, EVN Symposium 2000

  8. Spectral Line Correlation • Modern digital correlators intrinsically spectral line • Spectral resolution function bandwidth & number of lags (or size of FFT) • Maser components are very narrow • High spectral resolution is needed

  9. Galactic masers typically 1-20” • Short integration time (Time Smearing) • Hanning smooth • Scalar and vector averaging: • Scalar - Noise bias • Vector - Small synthesised beam

  10. ATCA Data (6.7 GHz Methanol)

  11. VLBI Data (12.2 GHz Methanol)

  12. Calibration • Basically the same as for continuum • Estimate time dependent antenna Tsys • Estimate residual delay and rate • Also correct for bandpass Assume time and frequency corrections are independent

  13. Bandpass Calibration • Need relatively strong continuum source • Must observe at same frequency • Can use auto-correlations, but cannot correct phase • Cross-corr allow phase correction • Need enough S/N on calibrator • Need to fringe fit first

  14. Amplitude Calibration • Can do normal Tsys calibration • Optionally, use auto correlations: • Gives very good results (in principle) • Corrects for pointing errors at telescope • Only gives relative calibration • Depends on amplitude calibration of template spectrum

  15. Fringe Fitting • Need to estimate residual delay and rate • Residual rate seen as slope of phase in time (in both frequency and lag domain) • Residual delay seen as shift in lag domain, so a slope of phase across the bandpass in the frequency domain

  16. Measure residual delay by measuring phase slope • Only a couple of channels per feature for spectral line • Cannot measure residual delay • Continuum delay calibrator must be observed every hour or so • Residual rates obtains from a bright spectral feature

  17. Doppler Correction • Each station at different velocity • Need to correct to standard rest frame • Observe at fixed frequency • Fringe rotation at correlator does some • Further velocity correction in software • Application depends critically on design of correlator

  18. Self-calibration • Many separate components at different velocities and position • Cannot selfcal data set as a whole • Cannot run self cal on each frequency channel separately • Selfcal strong (compact) feature and apply calibration to rest of channels

  19. Continuum Subtraction • No need for Galactic masers • Do after all calibration for HI absorption • Image negative hole in image • POSSM plots show as emission

  20. Imaging • Nothing special but… • Large maps with many frequency points yields large data cubes

  21. Water masers in W49N Walker etal 1982, ApJ

  22. Fringe Rate Mapping • Galactic masers sometimes large (10”) • Often many sources in beam • Wide velocity width • Large data cube • Use fringe rate mapping to find where emission is • Also gives absolute position • FRMAP in AIPS tricky to use

  23. Scheduling • Choose enough bandwidth for velocity coverage • Calculate required spectral resolution (Allow for Hanning smoothing) • Find correct velocity (and ref frame!) • Find close (enough) delay calibrator • Choose a strong bandpass calibrator • Turn off phasecal! • Consider over sampling

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