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Measuring the power spectrum of dark matter substructure using strong gravitational lensing
Cosmology and Nongalactic Astrophysics · Submitted 11 Mar 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In particular, we show that the power spectrum of projected density fluctuations in galaxy halos can be measured using strong gravitational lensing.
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The abstract, sentence by sentence
In recent years, it has become possible to detect individual dark matter subhalos near images of strongly lensed extended background galaxies. Typically, only the most massive subhalos in the strong lensing region may be detected this way. In this work, we show that strong lenses may also be used to constrain the much more numerous population of lower mass subhalos that are too small to be detected individually. In particular, we show that the power spectrum of projected density fluctuations in galaxy halos can be measured using strong gravitational lensing. We develop the mathematical framework of power spectrum estimation, and test our method on mock observations. We use our results to determine the types of observations required to measure the substructure power spectrum with high significance. We predict that deep observations ($\sim10$ hours on a single target) with current facilities can measure this power spectrum at the $3\sigma$ level, with no apparent degeneracy with unknown clumpiness in the background source structure or fluctuations from detector noise. Upcoming ALMA measurements of strong lenses are capable of placing strong constraints on the abundance of dark matter subhalos and the underlying particle nature of dark matter.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In recent years, it has become possible to detect individual dark matter subhalos near images of strongly lensed extended background galaxies. | background 1.00 | 0.07 | 0.03 | asserted 0.60 |
| s1 | Typically, only the most massive subhalos in the strong lensing region may be detected this way. | background 0.90 | 0.08 | 0.02 | hedged possibility 0.96 |
| s2 | In this work, we show that strong lenses may also be used to constrain the much more numerous population of lower mass subhalos that are too small to be detected individually. | contribution 0.94 | 0.77 | 0.44 | asserted 0.83 |
| s3 | In particular, we show that the power spectrum of projected density fluctuations in galaxy halos can be measured using strong gravitational lensing. | contribution 0.97 | 0.91 | 0.64 | asserted 1.00 |
| s4 | We develop the mathematical framework of power spectrum estimation, and test our method on mock observations. | method 0.84 | 0.96 | 0.04 | asserted 0.99 |
| s5 | We use our results to determine the types of observations required to measure the substructure power spectrum with high significance. | contribution 0.61 | 0.90 | 0.12 | asserted 0.98 |
| s6 | We predict that deep observations ($\sim10$ hours on a single target) with current facilities can measure this power spectrum at the $3\sigma$ level, with no apparent degeneracy with unknown clumpiness in the background source structure or fluctuations from detector noise. | result 0.92 | 0.82 | 0.40 | asserted 0.57 |
| s7 | Upcoming ALMA measurements of strong lenses are capable of placing strong constraints on the abundance of dark matter subhalos and the underlying particle nature of dark matter. | interpretation 0.70 | 0.21 | 0.18 | hedged possibility 0.77 |
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The paper
Original abstract
In recent years, it has become possible to detect individual dark matter subhalos near images of strongly lensed extended background galaxies. Typically, only the most massive subhalos in the strong lensing region may be detected this way. In this work, we show that strong lenses may also be used to constrain the much more numerous population of lower mass subhalos that are too small to be detected individually. In particular, we show that the power spectrum of projected density fluctuations in galaxy halos can be measured using strong gravitational lensing. We develop the mathematical framework of power spectrum estimation, and test our method on mock observations. We use our results to determine the types of observations required to measure the substructure power spectrum with high significance. We predict that deep observations ($\sim10$ hours on a single target) with current facilities can measure this power spectrum at the $3\sigma$ level, with no apparent degeneracy with unknown clumpiness in the background source structure or fluctuations from detector noise. Upcoming ALMA measurements of strong lenses are capable of placing strong constraints on the abundance of dark matter subhalos and the underlying particle nature of dark matter.
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References
How later papers used it
74 later papers cite it
2 later papers by other authors are listed below: 1 built on it and 1 used its method or tool.
Builds on it 1 of 2 papers with this label
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Extended this paper's initial approach to include subhalo populations that are not necessarily isotropic and homogeneous and to take into account the 2-subhalo term.
On the Power Spectrum of Dark Matter Substructure in Strong Gravitational Lenses (2017) · 1.00 · paraphrased: the licence does not allow quoting
Uses its method or tool 1 of 2 papers with this label
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Used this paper's expression for the surface density power spectrum as an integral over the mass function weighted by the surface density profile, assuming negligible spatial correlation between subhalos.
Analytic approach to astrometric perturbations of critical curves by substructures (2023) · 0.92 · paraphrased: the licence does not allow quoting
How the literature uses it
40 arXiv papers cite this in 67 sentences
Papers citing it · 50 sentences without a confident label
Builds on it 2 papers
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We extend the initial approach presented in Ref. [ref] to include subhalo populations that are not necessarily isotropic and homogeneous, and also take into account the 2-subhalo term.
On the Power Spectrum of Dark Matter Substructure in Strong Gravitational Lenses · Introduction · 1.00
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An analogous statistical method has been used before in weak gravitational lensing of the Cosmic Microwave Background radiation (e.g., [ref] , [ref] ), although we have further generalized it to the case of strong galaxy-galaxy lensing but without any assumptions of linear first order approximation in the formalism which goes beyond the current statistical methodology available in the literature (see 2012 BSc thesis of Sander Bus[https://www.astro.rug.nl/opleidingsinstituut/reports/bachelor/]; [ref] ).
The inner mass power spectrum of galaxies using strong gravitational lensing: beyond linear approximation · Introduction · 0.97
Uses its method or tool 1 paper
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Using the halo formalism [ref] and assuming that the spatial correlation between subhalos can be negligible (i.e., subhalos are randomly distributed), we can compute the surface density power spectrum as an integral over the mass function weighted by their surface density profile as [ref] P_δκ(k)=∫^M_max_M_min d n^2D/d M|κ̃_M(k)|^2 d M, where $k=√(k_x^2+k_y^2)$, $M_min$ and $M_max$ are the minimum and maximum mass of subhalos, respectively, $d n^2D/d M$ is the surface number density of subhalos with masses of $[M, M+δM]$, and $κ̃_M(k)$ is the Fourier transform of the convergence $κ_M$ provided by a subhalo of mass $M$.
Analytic approach to astrometric perturbations of critical curves by substructures · Fluctuations of macrocritical curves · 0.92
Compares with it 1 paper
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While our general approach follows a similar philosophy to that of Ref. [ref] , our computational technique differs at several levels, especially in our use of a mode function-based approach.
Beyond subhalos: Probing the collective effect of the Universe's small-scale structure with gravitational lensing · Introduction · 0.88
Cites it as background 9 papers
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As for the surface density power spectrum, previous studies have proposed the expressions for the different types of substructures such as CDM subhalos [ref] and quantum clumps of FDM [ref] .
Analytic approach to astrometric perturbations of critical curves by substructures · Introduction · 0.83
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$P_δ(k)$ is the observational realization of the substructure convergence power spectrum $P_κ(k)$ – the power spectrum of the projected dark matter density field – which [ref] first proposed as a lensing observable and [ref] computed analytically for galaxy-scale systems, showing sensitivity to CDM, warm dark matter, and self-interacting dark matter.
Statistical imprints of wave-like dark matter on multiply-imaged galaxies in strong cluster lenses from JWST · Physical interpretation · 0.83
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The idea of using the subhalo convergence power spectrum [ref] was developed as a statistical detection method to obtain population-level constraints without having to individually resolve clumps.
Quantifying the Line-of-Sight Halo Contribution to the Dark Matter Convergence Power Spectrum from Strong Gravitational Lenses · Conclusions · 0.86
What it cites · 2 sentences without a confident label
Cites as background 2 papers
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The distribution of substructure in ordinary galactic halos has been studied extensively in the literature [ref] .
The Diversity and Similarity of Simulated Cold Dark Matter Halos · The projected substructure power spectrum in dark matter halos · 1.00
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The distribution of substructure in ordinary galactic halos has been studied extensively in the literature [ref] .
Formation and evolution of galaxy dark matter halos and their substructure · The projected substructure power spectrum in dark matter halos · 1.00
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