Litcius/Paper detail

The Magnificent Five Images of Supernova Refsdal: Time Delay and Magnification Measurements

Patrick L. Kelly, S. Rodney, Tommaso Treu, Simon Birrer, V. Bonvin, Luc Dessart, R. J. Foley, A. V. Filippenko, Daniel Gilman, Saurabh W. Jha, J. Hjorth, Kaisey S. Mandel, Martin Millon, Justin Pierel, Stephen Thorp, Adi Zitrin, Tom Broadhurst, Wenlei Chen, J. M. Diego, Alan Dressler, Or Graur, Mathilde Jauzac, Matthew A. Malkan, C. McCully, Masamune Oguri, Marc Postman, Kasper Borello Schmidt, Keren Sharon, B. Tucker, Anja von der Linden, Joachim Wambsganß

2023The Astrophysical Journal36 citationsDOIOpen Access PDF

Abstract

Abstract In late 2014, four images of supernova (SN) “Refsdal,” the first known example of a strongly lensed SN with multiple resolved images, were detected in the MACS J1149 galaxy-cluster field. Following the images’ discovery, the SN was predicted to reappear within hundreds of days at a new position ∼8″ away in the field. The observed reappearance in late 2015 makes it possible to carry out Refsdal’s original proposal to use a multiply imaged SN to measure the Hubble constant H 0 , since the time delay between appearances should vary inversely with H 0 . Moreover, the position, brightness, and timing of the reappearance enable a novel test of the blind predictions of galaxy-cluster models, which are typically constrained only by the positions of multiply imaged galaxies. We have developed a new photometry pipeline that uses DOLPHOT to measure the fluxes of the five images of SN Refsdal from difference images. We apply four separate techniques to perform a blind measurement of the relative time delays and magnification ratios between the last image SX and the earlier images S1–S4. We measure the relative time delay of SX–S1 to be <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mstyle displaystyle="true"> <mml:msubsup> <mml:mrow> <mml:mn>376.0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>5.5</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>5.6</mml:mn> </mml:mrow> </mml:msubsup> </mml:mstyle> </mml:math> days and the relative magnification to be <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mstyle displaystyle="true"> <mml:msubsup> <mml:mrow> <mml:mn>0.30</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.3</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.5</mml:mn> </mml:mrow> </mml:msubsup> </mml:mstyle> </mml:math> . This corresponds to a 1.5% precision on the time delay and 17% precision for the magnification ratios and includes uncertainties due to millilensing and microlensing. In an accompanying paper, we place initial and blind constraints on the value of the Hubble constant.

Topics & Concepts

PhysicsMagnificationGravitational microlensingGalaxyPhotometry (optics)AstrophysicsSupernovaBrightnessTelescopeAstronomyStarsOpticsGamma-ray bursts and supernovaeCCD and CMOS Imaging SensorsAdvanced Image Processing Techniques