Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Oleg Titov (Geoscience Australia) Anastasiia Girdiuk (Institute of.

Slides:



Advertisements
Similar presentations
Accurate light-time correction due to a gravitating mass A mathematical follow-up to Cassinis experiment Bruno Bertotti Dipartimento di Fisica Nucleare.
Advertisements

03/000 First geodetic results from the AuScope VLBI network Oleg Titov Australian Government Geoscience Australia UTAS, Hobart, 20 June 2012.
The Geoscience Australia’s Online GPS Processing Service (AUSPOS)
March , Birmingham GR tests and micro-arcsecond light bending parameters by global and differential Gaia mesurements Maria Teresa Crosta Astronomical.
Processing of VLBI observation in St. Petersburg University Kudryashova Maria Astronomical Institute of Saint Petersburg University.
Optics in Astronomy - Interferometry - Oskar von der Lühe Kiepenheuer-Institut für Sonnenphysik Freiburg, Germany.
Astronomy Instrumentation Astronomy Summer School for West Africa Daniel Okoh.
VLBI component of the NCRIS Australian Government Geoscience Australia 15 August 2006, Canberra.
Outline of the Lectures Lecture 1: The Einstein Equivalence Principle Lecture 2: Post-Newtonian Limit of GR Lecture 3: The Parametrized Post-Newtonian.
General Relativity Physics Honours 2006 A/Prof. Geraint F. Lewis Rm 557, A29 Lecture Notes 5.
The Size and Distance Scale Of The Solar System Our Earth is just one of several Planets that revolve around our Sun, the primary and central object of.
AUSPOS Online GPS Processing Service John Manning, John Dawson.Ramesh Govind Geoscience Australia.
Gravitational lensing in plasma O.Yu. Tsupko 1,2 and G.S. Bisnovatyi-Kogan 1,2 1 Space Research Institute of Russian Academy of Science, Profsoyuznaya.
Sounding of the interior structure of Galilean satellite Io using the parameters of the theory of figure and gravitational field in the second approximation.
Distances in Space. How Far Away are Stars & Other Celestial Bodies? Use Stellarium to observe the sky and discuss what observations you might be able.
GEODETIC INSTITUTE LEIBNIZ UNIVERSITY OF HANNOVER GERMANY Ingo Neumann and Hansjörg Kutterer The probability of type I and type II errors in imprecise.
JOVIAN and SOLAR RADIO DEFLECTION EXPERIMENTS Ed Fomalont National Radio Astronomy Observatory Charlottesville, VA USA Sergei Kopeikin University of Missouri.
1 Gravitational lensing and neutrinos Why not look where natural lenses exist? Proposal of an additional candidate list in point source search: 1. Motivation.
Chapter 1 Introduction to Astronomy. What is Astronomy? Astronomy is the scientific study of celestial bodies. Astrology is a group of beliefs and schools.
03/000 Cosmologic astrometry Australian Government Geoscience Australia Yonsei University, Seoul 18 October 2010.
Effects of ionospheric small- scale structures on GNSS G. WAUTELET Royal Meteorological Institute of Belgium Ionospheric Radio Systems & Techniques (IRST)
03/000 Future operations of the AuScope network Australian Government Geoscience Australia.
Maria Teresa Crosta and Francois Mignard Small field relativistic experiment with Gaia: detection of the quadrupolar light deflection.
Recent GNSS Activities at Geoscience Australia Gary Johnston, Guorong Hu, Anna Riddell Geodesy & Seismic Monitoring Branch, Geoscience Australia.
Recent determination of Gamma with Cassini M.T. Crosta, F. Mignard CNRS-O.C.A. 5th RRFWG, June, Estec.
Quality Assessment for LIDAR Point Cloud Registration using In-Situ Conjugate Features Jen-Yu Han 1, Hui-Ping Tserng 1, Chih-Ting Lin 2 1 Department of.
Geodetic VLBI Lecture 2 18 October Lecture plan 1. From measurement of space and time to measurement of space-time 2. Elements of the Special and.
Gravity. Geocentric vs. Heliocentric Model The Geocentric Model Arguments For: Parallax not seen Almagest says so Fits with “heavenly” perfection Arguments.
An approach to mineral potential mapping using a mineral systems approach: an example of IOCG deposits in the NT Anthony Schofield and David Huston.
GGOS User Requirements and Functional Specifications Richard S. Gross Jet Propulsion Laboratory, California Institute of Technology, Pasadena, USA Global.
Crash Course of Relativistic Astrometry Four Dimensional Spacetime Poincare Transformation Time Dilatation Wavelength Shift Gravitational Deflection of.
Fundamental Principles of General Relativity  general principle: laws of physics must be the same for all observers (accelerated or not)  general covariance:
03/000 Informal presentation on the optical spectroscopic program Oleg Titov Australian Government Geoscience Australia UTAS, Hobart, 5 June 2012.
Prospects for observing quasar jets with the Space Interferometry Mission Ann E. Wehrle Space Science Institute, La Canada Flintridge, CA, and Boulder,
Spatial interpolation of Daily temperatures using an advection scheme Kwang Soo Kim.
Influence of dark energy on gravitational lensing Kabita Sarkar 1, Arunava Bhadra 2 1 Salesian College, Siliguri Campus, India High Energy Cosmic.
10/5/2004New Windows on the Universe Jan Kuijpers Part 1: Gravitation & relativityPart 1: Gravitation & relativity J.A. Peacock, Cosmological Physics,
S/X receiver for Parkes geodetic VLBI program 29 October 2012 ATNF, Sydney 29 October 2012 Оleg Titov (Geoscience Australia)
Orbital evolution of compact Black-hole binaries and white dwarf binaries Wencong Chen Astro-ph/ Astro-ph/
1 Phenomena in the Solar System: need of network of observation J.E. Arlot, M. Stavinschi IMCCE/CNRS/observatoire de Paris Institut astronomique de l’académie.
Signal Propagation  Electro-Magnetic Signal  Geometric Approximation ~ Fast Particle Approximation  Speed of Light in Vacuum.
LLR Analysis – Relativistic Model and Tests of Gravitational Physics James G. Williams Dale H. Boggs Slava G. Turyshev Jet Propulsion Laboratory California.
Spin-orbit Gravitational Radiation Reaction for Two-body Systems Jing Zeng Washington University Gravity Group November
03/000 Statistical properties of CRF solution from VLBI data analysis Oleg Titov Australian Government Geoscience Australia GAIA-2005, Dresden, 15-16,
 Distance is the most important & most difficult quantity to measure in Astronomy  Method of Trigonometric Parallaxes  Direct geometric method of finding.
VISIBLE PROPERTIES OF COSMIC ANTI-STRING Kotvytskiy A.T., Shulga V.M. Institute of Radio Astronomy of Nat. Ac. Sci. of Ukraine Karazin Kharkov National.
Fertility and endowment indices for mineral systems: examples for Zn-Pb systems David Huston All mineral provinces are not created equally.
The Moon’s and Sun’s Effect on Earth
Soichiro Isoyama Collaborators : Norichika Sago, Ryuichi Fujita, and Takahiro Tanaka The gravitational wave from an EMRI binary Influence of the beyond.
Lecture Outlines Astronomy Today 8th Edition Chaisson/McMillan © 2014 Pearson Education, Inc. Chapter 2.
Company LOGO Technology and Application of Laser Tracker in Large Space Measurement Yang Fan, Li Guangyun, Fan Baixing IWAA2014 in Beijing, China Zhengzhou.
Astronomy…It’s far-out! Sun – Earth – Moon. How do we know about space How do we know about space ?
Discrete Global Grid Systems A New Way to Manage ‘Big Earth Data’ Dr. Matthew B.J. Purss Geoscience Australia Co-Chair OGC Discrete Global Grid Systems.
Thomas Herring, IERS ACC, MIT
Sergei Kopeikin Department of Physics and Astronomy,
Positional Astronomy Chapter 3 Fundamentals of Radio Interferometry
Parameterized Newtonian Theory
The Solar System Dimensions
Jupiter Light-Deflection Experiment and Its Results
Universal Gravitation
Universal Gravitation
Observational Astronomy Astrometry
Nicholas Car Scientific Data Platforms & Policy
Binary Stars Palomar Observatory.
Troposphere and Clock Parameterization During Continuous VLBI Campaigns Kamil Teke1, 2, Johannes Boehm1, Hana Spicakova1, Andrea Pany1, Harald Schuh1 1.
ELVIS isn’t leaving the building, its helping you design it.
Optical Telescopes, Radio Telescopes and Other Technologies Advance Our Understanding of Space Unit E: Topic Three.
Selection of the stable radio sources for the ICRF-2
Yun Hao, Yiyi Zhu and Jong-Ping Hsu Department of Physics
Presentation transcript:

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)

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

Introduction 1.Geodetic Very Long Baseline Interferometry (VLBI) measures the group delay with accuracy up to 30 ps; 2.General relativity is presented by the gravitational delay and a coordinate term in the geometric delay; 3.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

Introduction 1.Geodetic Very Long Baseline Interferometry (VLBI) measures the group delay with accuracy up to 30 ps; 2.General relativity is presented by the gravitational delay and a coordinate term in the geometric delay; 3.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

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

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

Light deflection angle vs gravitational delay Q – quasar, B – deflecting body (Sun) b Q B   s

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

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

Light deflection angle vs gravitational delay

Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Observational results 1. Geodetic VLBI data from 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 Light deflection angle

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

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

Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Light deflection angle vs elongation

Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Light deflection angle vs elongation

Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Light deflection angle vs elongation

Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Light deflection angle vs elongation

Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Light deflection angle vs elongation

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

Outreach – “When GR works?” OpticalVLBI During Solar eclipseAny time (365 days, 24/7) Near the SunAny elongation angle Optical instrumentRadio telescopes Nice sunny dayAny weather condition ~1”.75 0”.001  1”

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  , 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

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

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

The “minor” terms for the Sun The additional deflection angle is individual for all baselines R (km)  b=3000 kmb=10000 km 700,000 (grazing light, 0 .25) 1”.750” ”0125 0”.450” ” ”.220” ” ”.090” ” Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

The “minor” terms for Jupiter R (km)  b=3000 kmb=10000 km 70,000 (grazing light, 20”)0”.0160” ” ,000 (1’)0”.00530” ” ,000 (2’)0”.00260” ” For grazing light Deflection of light induced by the Sun gravity field and measured with geodetic VLBI

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

Additional angle and its geometric interpretation Q – apparent position; Q’ – true position; B – deflecting body, b Q B   Q’ 

Deflection of light induced by the Sun gravity field and measured with geodetic VLBI Additional angle may be observed Q – apparent position; Q’ – true position; B – deflecting body, Q Q’ B 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 Close alignment of star and radio source Separation is less than 2”

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

Phone: Web: Address: Cnr Jerrabomberra Avenue and Hindmarsh Drive, Symonston ACT 2609 Postal Address: GPO Box 378, Canberra ACT 2601 Any Questions? Thank you for your attention