A Time Delay for the Largest Gravitationally Lensed Quasar: SDSS J1004+4112
Astrophysical Journal University of Chicago Press (2007)
Abstract:
We present 426 epochs of optical monitoring data spanning 1000 days from December 2003 to June 2006 for the gravitationally lensed quasar SDSS J1004+4112. The time delay between the A and B images is 38.4+/-2.0 days in the expected sense that B leads A and the overall time ordering is C-B-A-D-E. The measured delay invalidates all published models. The models failed because they neglected the perturbations from cluster member galaxies. Models including the galaxies can fit the data well, but strong conclusions about the cluster mass distribution should await the measurement of the longer, and less substructure sensitive, delays of the C and D images. For these images, a CB delay of 681+/-15 days is plausible but requires confirmation, while CB and AD delays of >560 days and > 800 days are required. We clearly detect microlensing of the A/B images, with the delay-corrected flux ratios changing from B-A=0.44+/-0.01 mag in the first season to 0.29+/-0.01 mag in the second season and 0.32+/-0.01 mag in the third season.A time delay for the cluster-lensed quasar SDSS J1004+4112
Astrophysical Journal 662:1 I (2007) 62-71
Abstract:
We present 426 epochs of optical monitoring data spanning 1000 days from 2003 December to 2006 June for the gravitationally lensed quasar SDSS J1004+4112. The time delay between the A and B images is ΔtBA = 38.4 ± 2.0 days (Δχ2 = 4) in the expected sense that B leads A and the overall time ordering is C-B-A-D-E. The measured delay invalidates all published models. The models probably failed because they neglected the perturbations from cluster member galaxies. Models including the galaxies can fit the data well, but conclusions about the cluster mass distribution should await the measurement of the longer, and less substructure sensitive, delays of the C and D images. For these images, a delay of ΔtCB ≃ 681 ± 15 days is plausible but requires confirmation, while delays of ΔtCB 560 days and Δt AD > 800 days are required. We clearly detect microlensing of the A/B images, with the delay-corrected flux ratios changing from mB - mA -0-44 ± 0.01 mag in the first season to 0.29 ± 0.01 mag in the second season and 0.32 ± 0.01 mag in the third season. © 2007. The American Astronomical Society. All rights reserved.Practical implementation of the complex wavefront modulation model for optical alignment
Society of Photo-Optical Instrumentation Engineers (SPIE) 6617 (2007) 0-0
Computer-guided alignment I: Phase and amplitude modulation of alignment-influenced optical wavefront
Optics Express 15:6 (2007) 3127-3139
Abstract:
As the first part of a development programme on computer-guided alignment(CGA), we model the alignment influence on the optical wavefront in terms of the phase and amplitude modulation. This modulation is derived from the interaction between alignment parameters and influence functions, both expressed in complex form. The alignment influence model is used to approximate the ray-traced target wavefront of a randomly mis-aligned multi-element system. The approximated wavefront shows a factor of ∼ 100 improvement in predicting the target, when coupled non-linear influences among elements are included. This demonstrates the significance of the inter-element effect. We discuss the possibility of adopting the model for rectifying mis-alignment of multi-element systems. © 2007 Optical Society of America.Practical implementation of the complex wavefront modulation model for optical alignment
Proceedings of SPIE - The International Society for Optical Engineering 6617 (2007) 21-21