Degeneracies and scaling relations in general power-law models for gravitational lenses |
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Authors: | Olaf Wucknitz |
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Affiliation: | Universität Hamburg, Hamburger Sternwarte, Gojenbergsweg 112, 21029 Hamburg, Germany and; University of Manchester, Jodrell Bank Observatory, Macclesfield, Cheshire SK11 9DL |
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Abstract: | The time-delay in gravitational lenses can be used to derive the Hubble constant in a relatively simple way. The results of this method are less dependent on astrophysical assumptions than in many other methods. For systems with accurately measured positions and time-delays, the most important uncertainty is related to the mass model used. Simple parametric models like isothermal ellipsoidal mass distributions seem to provide consistent results with a reasonably small scatter when applied to several lens systems. We discuss a family of models with a separable radial power law and an arbitrary angular dependence for the potential ψ = r β F ( θ ) . Isothermal potentials are a special case of these models with β =1 . An additional external shear is used to take into account perturbations from other galaxies. Using a simple linear formalism for quadruple lenses, we can derive H 0 as a function of the observables and the shear. If the latter is fixed, the result depends on the assumed power-law exponent according to H 0∝(2- β )/ β . The effect of external shear is quantified by introducing a 'critical shear' γ c as a measure for the amount of shear that changes the result significantly. The analysis shows that in the general case H 0 and γ c do not depend on the position of the lens galaxy. Spherical lens models with images close to the Einstein radius with fitted external shear differ by a factor of β /2 from shearless models, leading to H 0∝2- β in this case. We discuss these results and compare them with numerical models for a number of real lens systems. |
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Keywords: | gravitational lensing quasars: individual: Q2237+0305 quasars: individual: PG 1115+080 quasars: individual: RX J0911.4+0551 quasars: individual: B1608+656 distance scale |
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