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Part of a WEAVE fibre configuration

Part of the WEAVE focal plane showing optical fibres positioned on a set of targets in the telescope focal plane.

Prof Gavin Dalton

Professor of Astrophysics

Research theme

  • Astronomy and astrophysics

Sub department

  • Astrophysics

Research groups

  • Astronomical instrumentation
  • Extremely Large Telescope
Gavin.Dalton@physics.ox.ac.uk
  • About
  • Research
  • Publications

The Dark UNiverse Explorer (DUNE): proposal to ESA's cosmic vision

Experimental Astronomy: an international journal on astronomical instrumentation and data analysis 23:1 (2008) 17

Authors:

A Refregier, DUNE Collaboration, GB Dalton
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Computer-guided alignment II: Optical system alignment using differential wavefront sampling

Optics Express 15:23 (2007) 15424-15437

Authors:

H Lee, GB Dalton, IAJ Tosh, SW Kim

Abstract:

We present a differential wavefront sampling method for the efficient alignment of centred optical systems. Using the inter-element effects reported in our previous study, this method generates a linear symmetric matrix that relates the optical wavefront to misalignments within the system. The solution vector of this matrix equation provides a unique description of decentre and tilt misalignments of the system. We give a comparison of this approach to the existing method in the first case study and then illustrate characteristics of the new approach using the subsequent four case studies and Monte-Carlo alignment simulations. The results reveal superiority of the method over the existing one in misalignment estimation accuracy and demonstrate the practical feasibility and robustness. © 2007 Optical Society of America.
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A Time Delay for the Largest Gravitationally Lensed Quasar: SDSS J1004+4112

Astrophysical Journal University of Chicago Press (2007)

Authors:

J Fohlmeister, CS Kochanek, EE Falco, J Wambsganss, N Morgan, CW Morgan, EO Ofek, D Maoz, CR Keeton, JC Barentine, G Dalton, J Dembicky, W Ketzeback, R McMillan, CS Peters

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.
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A time delay for the cluster-lensed quasar SDSS J1004+4112

Astrophysical Journal 662:1 I (2007) 62-71

Authors:

J Fohlmeister, CS Kochanek, EE Falco, J Wambsganss, N Morgan, CW Morgan, EO Üfek, D Maoz, CR Keeton, JC Barentine, G Dalton, J Dembicky, W Ketzeback, R McMillan, CS Peters

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.
More details from the publisher

Practical implementation of the complex wavefront modulation model for optical alignment

Society of Photo-Optical Instrumentation Engineers (SPIE) 6617 (2007) 0-0

Authors:

H Lee, GB Dalton, IAJ Tosh, S-W Kim

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