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Improving the precision of time-delay cosmography with observations of galaxies along the line of sight

Cosmology and Nongalactic Astrophysics · Submitted 14 Mar 2013

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Although deeper multi-band observations of the field of B1608+656 are necessary to obtain a more precise estimate, we conclude that griK photometry, in addition to spectroscopy to characterize the immediate environment, is an effective way to increase the precision of time-delay cosmography.

how it is stated · asserted 0.93 read the record →

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arXiv ID1303.3588 (version 1)
Pith IDPEMTDQJG, Pith's permanent record of this paper and its review
CitationChristopher D. Fassnacht, L\'eon V.E. Koopmans, Marua Bradac, Matthew W. Auger, Philip J. Marshall, Roger D. Blandford, Sherry H. Suyu, Stefan Hilbert, Thomas E. Collett, Tommaso Treu, Zach S. Greene. "Improving the precision of time-delay cosmography with observations of galaxies along the line of sight." arXiv:1303.3588 (2013). https://pith.science/paper/PEMTDQJG
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 8,366 input tokens, $0.0004 reported.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.93 · human participants 0.01 · controlled comparison 0.46 · randomized assignment 0.01 · states quantitative result 0.99 · compares with prior results 0.90 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

In order to use strong gravitational lens time delays to measure precise and accurate cosmological parameters the effects of mass along the line of sight must be taken into account. We present a method to achieve this by constraining the probability distribution function of the effective line of sight convergence k_ext. The method is based on matching the observed overdensity in the weighted number of galaxies to that found in mock catalogs with k_ext obtained by ray-tracing through structure formation simulations. We explore weighting schemes based on projected distance, mass, luminosity, and redshift. This additional information reduces the uncertainty of k_ext from sigma_k $0.06 to ~0.04 for very overdense lines of sight like that of the system B1608+656. For more common lines of sight, sigma_k is reduced to ~<0.03, corresponding to an uncertainty of ~<3% on distance. This uncertainty has comparable effects on cosmological parameters to that arising from the mass model of the deflector and its immediate environment. Photometric redshifts based on g, r, i and K photometries are sufficient to constrain k_ext almost as well as with spectroscopic redshifts. As an illustration, we apply our method to the system B1608+656. Our most reliable k_ext estimator gives sigma_k=0.047 down from 0.065 using only galaxy counts. Although deeper multi-band observations of the field of B1608+656 are necessary to obtain a more precise estimate, we conclude that griK photometry, in addition to spectroscopy to characterize the immediate environment, is an effective way to increase the precision of time-delay cosmography.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 In order to use strong gravitational lens time delays to measure precise and accurate cosmological parameters the effects of mass along the line of sight must be taken into account. background 1.00 0.06 0.05 asserted 0.99
s1 We present a method to achieve this by constraining the probability distribution function of the effective line of sight convergence k_ext. contribution 0.76 0.89 0.08 asserted 1.00
s2 The method is based on matching the observed overdensity in the weighted number of galaxies to that found in mock catalogs with k_ext obtained by ray-tracing through structure formation simulations. method 1.00 0.78 0.04 asserted 1.00
s3 We explore weighting schemes based on projected distance, mass, luminosity, and redshift. method 0.97 0.86 0.02 asserted 0.66
s4 This additional information reduces the uncertainty of k_ext from sigma_k $0.06 to ~0.04 for very overdense lines of sight like that of the system B1608+656. result 1.00 0.91 0.13 asserted 0.99
s5 For more common lines of sight, sigma_k is reduced to ~<0.03, corresponding to an uncertainty of ~<3% on distance. result 0.99 0.89 0.17 asserted 0.99
s6 This uncertainty has comparable effects on cosmological parameters to that arising from the mass model of the deflector and its immediate environment. interpretation 0.95 0.68 0.11 asserted 1.00
s7 Photometric redshifts based on g, r, i and K photometries are sufficient to constrain k_ext almost as well as with spectroscopic redshifts. result 0.94 0.82 0.09 asserted 0.99
s8 As an illustration, we apply our method to the system B1608+656. contribution 0.74 0.92 0.03 asserted 0.86
s9 Our most reliable k_ext estimator gives sigma_k=0.047 down from 0.065 using only galaxy counts. result 1.00 0.96 0.13 asserted 1.00
s10 Although deeper multi-band observations of the field of B1608+656 are necessary to obtain a more precise estimate, we conclude that griK photometry, in addition to spectroscopy to characterize the immediate environment, is an effective way to increase the precision of time-delay cosmography. interpretation 0.69 0.76 0.84 asserted 0.93

What kind of paper the classifier reports this is: method or tool 1.00 · evidence from simulation or computation 0.71.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

In order to use strong gravitational lens time delays to measure precise and accurate cosmological parameters the effects of mass along the line of sight must be taken into account. We present a method to achieve this by constraining the probability distribution function of the effective line of sight convergence k_ext. The method is based on matching the observed overdensity in the weighted number of galaxies to that found in mock catalogs with k_ext obtained by ray-tracing through structure formation simulations. We explore weighting schemes based on projected distance, mass, luminosity, and redshift. This additional information reduces the uncertainty of k_ext from sigma_k $0.06 to ~0.04 for very overdense lines of sight like that of the system B1608+656. For more common lines of sight, sigma_k is reduced to ~<0.03, corresponding to an uncertainty of ~<3% on distance. This uncertainty has comparable effects on cosmological parameters to that arising from the mass model of the deflector and its immediate environment. Photometric redshifts based on g, r, i and K photometries are sufficient to constrain k_ext almost as well as with spectroscopic redshifts. As an illustration, we apply our method to the system B1608+656. Our most reliable k_ext estimator gives sigma_k=0.047 down from 0.065 using only galaxy counts. Although deeper multi-band observations of the field of B1608+656 are necessary to obtain a more precise estimate, we conclude that griK photometry, in addition to spectroscopy to characterize the immediate environment, is an effective way to increase the precision of time-delay cosmography.

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7 arXiv papers cite this in 10 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

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  • Time delay cosmography has made the greatest advances in the last several years, with improved lens modeling [ref] , clear understanding of the cosmological leverage [ref] , high accuracy time delay estimation [ref] , and actual application to cosmological constraints on geometry and dark energy [ref] .

    Doubling Strong Lensing as a Cosmological Probe · Introduction · 0.83

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