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Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

Deflection of light induced by the Sun gravity field and measured with geodetic VLBI. Oleg Titov (Geoscience Australia) Anastasiia Girdiuk (Institute of Applied Astronomy, RAS). Outline. 1. Introduction – General Relativity in geodetic VLBI 2. Gravitational delay vs light deflection angle

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Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

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  1. Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Oleg Titov (Geoscience Australia) AnastasiiaGirdiuk (Institute of Applied Astronomy, RAS)

  2. Outline • 1. Introduction – General Relativity in geodetic VLBI • 2. Gravitational delay vs light deflection angle • 3. Observational results • 4. Extra deflection with VLBI • 5. Conclusion Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  3. Introduction • Geodetic Very Long Baseline Interferometry (VLBI) measures the group delay with accuracy up to 30 ps; • General relativity is presented by the gravitational delay and a coordinate term in the geometric delay; • Gravitational delay caused by the Sun gravitational field is about 40 ns near the Sun and about 400 ps in opposite direction; Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  4. Introduction • Geodetic Very Long Baseline Interferometry (VLBI) measures the group delay with accuracy up to 30 ps; • General relativity is presented by the gravitational delay and a coordinate term in the geometric delay; • Gravitational delay caused by the Sun gravitational field is about 40 ns near the Sun and about 400 ps in opposite direction; Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  5. Introduction • Effect of general relativity is split into two separate terms; • Gravitational delay is expressed as a function of the barycentric distances and . Geometric delay is a function of baseline length • Light deflection angle is not presented – no link to the optical astrometry. Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  6. Introduction Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  7. Light deflection angle vs gravitational delay • Q – quasar, B – deflecting body (Sun) b Q  s  B Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  8. Light deflection angle vs gravitational delay • Q – quasar, B – deflecting body (Sun) Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  9. Difference between two models Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  10. Light deflection angle vs gravitational delay Deflection angle for arbitrary … …now explicitly presented in the equation for the VLBI group delay Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  11. Light deflection angle vs gravitational delay Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  12. Observational results • 1. Geodetic VLBI data from 1991-2001 • 2. Gravitational delay and coordinate term in geometric delay were switched off for a set of selected radio sources • 3. Equatorial coordinates of the selected radio sources were estimated as daily parameters for each 24-hour VLBI sessions • 4. The estimated coordinates are converted to the deflection angle  and PPN parameter . Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  13. Light deflection angle 1803+784 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  14. Light deflection angle 1606+106 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  15. Light deflection angle 1334-127 • Minimum elongation 2.6 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  16. Light deflection angle vs elongation 1606+106 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  17. Light deflection angle vs elongation 1606+106 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  18. Light deflection angle vs elongation 1606+106 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  19. Light deflection angle vs elongation 0229+131 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  20. Light deflection angle vs elongation 0229+131 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  21. New formula: benefits • 1. Simple; • 2. Consistent with the geometric part of group delay model; • 3. Linked to the deflection angle directly; • 4. Free off coordinate terms; • 5. Partial derivate for  is optimal; • 6. Allows more flexibility; • 7. Looking good as an alternative option for IERS Conventions Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  22. Outreach – “When GR works?” Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  23. Observations If all the general relativity effects are switched off the VLBI group delay model, the light deflection angle will be observed at any moment and at any elongation of a radio sources to the Sun (the closer, the better). The old good time (before 2002) when the radio sources were observed close to the Sun (as close as 1.5). The PPN parameter  was estimated very accurately (0.001) from a standard 24-hour session, if the number of delays is  100. The accuracy would be about 0.0001, were a dedicated session for observation of a strong radio source within 3 arranged. Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  24. The “minor” terms ( = 1) The minor terms are not negligible in the small angle approximation (  0) Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  25. The “minor” terms Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  26. The “minor” terms for the Sun The additional deflection angle is individual for all baselines For geodetic VLBI observation of the radio sources near the Solar limb Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  27. The “minor” terms for Jupiter Angular size Mass g =70.000 km For grazing light For geodetic VLBI observation of the radio sources near Jupiter Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  28. The “minor” terms The additional deflection angle is individual for all baselines and could be detected with observations within 2 from the Sun and 2’ from Jupiter Total magnitude Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  29. Additional angle and its geometric interpretation • Q – apparent position; • Q’ – true position; • B – deflecting body, Q  Q’ b B   Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  30. Additional angle may be observed • Q – apparent position; • Q’ – true position; • B – deflecting body, Q B Q’ b B • Traditional deflection angle (unobservable) • Additional deflection angle (observable), if b/R ~ 0.1 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  31. Close alignment of star and radio source 0758-737 • Separation is less than 2” 0758-737 Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  32. Conclusion • 1. General relativity effects in VLBI could be expressed in term of the light deflection angle ; • 2. The light deflection angle could be estimated for an arbitrary elongation from the Sun with high precision; • 3. The equation for light deflection at arbitrary elongation was tested using a set of VLBI data; • 4. The PPN parameter  was estimated for several 24-hour sessions with accuracy 0.001. • 5. Additional deflection angle could be observed for a close approach to the Sun or Jupiter; • 6. A dedicated observational programs for detection of the additional angle are required. Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

  33. Any Questions? • Thank you for your attention Phone: +61 2 6249 9111 Web: www.ga.gov.au Email: oleg.titov@ga.gov.au Address:Cnr Jerrabomberra Avenue and Hindmarsh Drive, Symonston ACT 2609 Postal Address: GPO Box 378, Canberra ACT 2601

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