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Phys. Rev. D 72, 104006 (2005) [16 pages]

Formalism for testing theories of gravity using lensing by compact objects: Static, spherically symmetric case

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Charles R. Keeton*
Department of Physics & Astronomy, Rutgers University, 136 Frelinghuysen Road, Piscataway, New Jersey 08854, USA

A. O. Petters
Departments of Mathematics and Physics, Duke University, Science Drive, Durham, North Carolina 27708-0320, USA

Received 7 October 2005; published 4 November 2005

We are developing a general, unified, and rigorous analytical framework for using gravitational lensing by compact objects to test different theories of gravity beyond the weak-deflection limit. In this paper we present the formalism for computing corrections to lensing observables for static, spherically symmetric gravity theories in which the corrections to the weak-deflection limit can be expanded as a Taylor series in one parameter, namely, the gravitational radius of the lens object. We take care to derive coordinate-independent expressions and compute quantities that are directly observable. We compute series expansions for the observables that are accurate to second order in the ratio ε=ϑ/ϑE of the angle subtended by the lens’s gravitational radius to the weak-deflection Einstein radius, which scales with mass as εM1/2. The positions, magnifications, and time delays of the individual images have corrections at both first and second order in ε, as does the differential time delay between the two images. Interestingly, we find that the first-order corrections to the total magnification and centroid position vanish in all gravity theories that agree with general relativity in the weak-deflection limit, but they can remain nonzero in modified theories that disagree with general relativity in the weak-deflection limit. For the Reissner-Nordström metric and a related metric from heterotic string theory, our formalism reveals an intriguing connection between lensing observables and the condition for having a naked singularity, which could provide an observational method for testing the existence of such objects. We apply our formalism to the galactic black hole and predict that the corrections to the image positions are at the level of 10  μarc s (microarcseconds), while the correction to the time delay is a few hundredths of a second. These corrections would be measurable today if a pulsar were found to be lensed by the galactic black hole, and they should be readily detectable with planned missions like MAXIM.

© 2005 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.72.104006
DOI:
10.1103/PhysRevD.72.104006
PACS:
04.70.Bw, 04.80.Cc

*Email address: keeton@physics.rutgers.edu

Email address: petters@math.duke.edu