RECORD
Massive Dark-matter halos and Evolution of Early-type Galaxies to z=1
Astrophysics · Submitted 19 Jan 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Hence, the isothermal approximation is not sufficiently accurate for applications that depend critically on the slope of the mass density profile (i.e. measuring H_0).
The compiled record
The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
Open the compiled record
The abstract, sentence by sentence
(Shortened) The combination of lensing and stellar dynamics breaks the mass-anisotropy degeneracy and provides stringent constraints on the mass distribution in early-type (E/S0) galaxies out to z~1. We present the combined results from the five field E/S0 lens galaxies at z=0.5-1.0 analyzed as part of the LSD Survey. We find: (i) Constant M/L models are ruled out at >99% CL for all five E/S0s. The projected dark-matter mass fractions inside the Einstein (effective) radius is f_DM=0.37-0.72 (0.15-0.65) for isotropic models. (ii) The average power-law slope of the total mass distribution is <\gamma'>=1.75+-0.10 for isotropic models with 0.20 rms scatter. The ratio between the observed central stellar velocity dispersion and that from the best-fit SIE lens model is <f_SIE>=<\sigma/\sigma_SIE>=0.87+-0.04 with 0.08 rms. Considering that \gamma'>2 and f_SIE>1 have been reported for other systems, we conclude that there is a significant intrinsic scatter in the density slopes of E/S0s (rms \~15%). Hence, the isothermal approximation is not sufficiently accurate for applications that depend critically on the slope of the mass density profile (i.e. measuring H_0). (iii) The inner power-law slope of the dark-matter halo is constrained to be <\gamma>=1.3(+0.2/-0.4) (68% CL) for the isotropic model or an upper limit of \gamma<0.6, if the galaxies are radially anisotropic (r_i=R_e). This is consistent with numerical simulations only for an isotropic velocity ellipsoid and if baryonic collapse and star-formation do not steepen dark-matter density profiles. (iv) The average stellar M/L evolves as d\log(M_*/L_B)/dz =-0.72+-0.10, obtained via the FP. Based on lensing and dynamics we find d\log(M_*/L_B)/dz=-0.75+-0.17, indicating that the M/L ratio evolution for our sample of field E/S0s is faster than those in clusters.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | (Shortened) The combination of lensing and stellar dynamics breaks the mass-anisotropy degeneracy and provides stringent constraints on the mass distribution in early-type (E/S0) galaxies out to z~1. | background 0.71 | 0.21 | 0.24 | asserted 1.00 |
| s1 | We present the combined results from the five field E/S0 lens galaxies at z=0.5-1.0 analyzed as part of the LSD Survey. | contribution 0.98 | 0.90 | 0.04 | asserted 0.95 |
| s2 | We find: (i) Constant M/L models are ruled out at >99% CL for all five E/S0s. | result 1.00 | 0.96 | 0.20 | asserted 1.00 |
| s3 | The projected dark-matter mass fractions inside the Einstein (effective) radius is f_DM=0.37-0.72 (0.15-0.65) for isotropic models. | result 1.00 | 0.94 | 0.14 | asserted 1.00 |
| s4 | (ii) The average power-law slope of the total mass distribution is <\gamma'>=1.75+-0.10 for isotropic models with 0.20 rms scatter. | result 1.00 | 0.95 | 0.12 | asserted 1.00 |
| s5 | The ratio between the observed central stellar velocity dispersion and that from the best-fit SIE lens model is <f_SIE>=<\sigma/\sigma_SIE>=0.87+-0.04 with 0.08 rms. | result 1.00 | 0.94 | 0.06 | asserted 1.00 |
| s6 | Considering that \gamma'>2 and f_SIE>1 have been reported for other systems, we conclude that there is a significant intrinsic scatter in the density slopes of E/S0s (rms \~15%). | interpretation 0.94 | 0.39 | 0.18 | asserted 0.99 |
| s7 | Hence, the isothermal approximation is not sufficiently accurate for applications that depend critically on the slope of the mass density profile (i.e. measuring H_0). | interpretation 0.99 | 0.50 | 0.25 | asserted 0.98 |
| s8 | (iii) The inner power-law slope of the dark-matter halo is constrained to be <\gamma>=1.3(+0.2/-0.4) (68% CL) for the isotropic model or an upper limit of \gamma<0.6, if the galaxies are radially anisotropic (r_i=R_e). | result 1.00 | 0.93 | 0.14 | asserted 0.97 |
| s9 | This is consistent with numerical simulations only for an isotropic velocity ellipsoid and if baryonic collapse and star-formation do not steepen dark-matter density profiles. | interpretation 0.98 | 0.16 | 0.08 | hedged possibility 0.94 |
| s10 | (iv) The average stellar M/L evolves as d\log(M_*/L_B)/dz =-0.72+-0.10, obtained via the FP. | result 1.00 | 0.93 | 0.10 | asserted 1.00 |
| s11 | Based on lensing and dynamics we find d\log(M_*/L_B)/dz=-0.75+-0.17, indicating that the M/L ratio evolution for our sample of field E/S0s is faster than those in clusters. | result 0.89 | 0.97 | 0.17 | asserted 0.68 |
What was examined, and what was not
- arXiv listing abstract v2
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
The paper
Original abstract
(Shortened) The combination of lensing and stellar dynamics breaks the mass-anisotropy degeneracy and provides stringent constraints on the mass distribution in early-type (E/S0) galaxies out to z~1. We present the combined results from the five field E/S0 lens galaxies at z=0.5-1.0 analyzed as part of the LSD Survey. We find: (i) Constant M/L models are ruled out at >99% CL for all five E/S0s. The projected dark-matter mass fractions inside the Einstein (effective) radius is f_DM=0.37-0.72 (0.15-0.65) for isotropic models. (ii) The average power-law slope of the total mass distribution is <\gamma'>=1.75+-0.10 for isotropic models with 0.20 rms scatter. The ratio between the observed central stellar velocity dispersion and that from the best-fit SIE lens model is <f_SIE>=<\sigma/\sigma_SIE>=0.87+-0.04 with 0.08 rms. Considering that \gamma'>2 and f_SIE>1 have been reported for other systems, we conclude that there is a significant intrinsic scatter in the density slopes of E/S0s (rms \~15%). Hence, the isothermal approximation is not sufficiently accurate for applications that depend critically on the slope of the mass density profile (i.e. measuring H_0). (iii) The inner power-law slope of the dark-matter halo is constrained to be <\gamma>=1.3(+0.2/-0.4) (68% CL) for the isotropic model or an upper limit of \gamma<0.6, if the galaxies are radially anisotropic (r_i=R_e). This is consistent with numerical simulations only for an isotropic velocity ellipsoid and if baryonic collapse and star-formation do not steepen dark-matter density profiles. (iv) The average stellar M/L evolves as d\log(M_*/L_B)/dz =-0.72+-0.10, obtained via the FP. Based on lensing and dynamics we find d\log(M_*/L_B)/dz=-0.75+-0.17, indicating that the M/L ratio evolution for our sample of field E/S0s is faster than those in clusters.
Human review
References
How later papers used it
74 later papers cite it
1 paper by the same authors is listed below: 1 used its method or tool.
Uses its method or tool 1 of 6 papers with this label · 1 by the same authors
By the same authors
-
Used this paper's equation to give the luminosity-weighted line of sight velocity dispersion within an aperture.
TDCOSMO IV: Hierarchical time-delay cosmography -- joint inference of the Hubble constant and galaxy density profiles (2020) (same authors) · 0.87 · paraphrased: the licence does not allow quoting
How the literature uses it
10 arXiv papers cite this in 11 sentences
Papers citing it · 5 sentences without a confident label
Uses its data or values 2 papers
-
This sample integrates lens systems from six major surveys: the Lens Structure and Dynamics (LSD) survey [ref] , the Strong Lensing Legacy Survey [ref] , the Sloan Lens ACS (SLACS) survey [ref] , the SLACS extension known as “SLACS for the Masses" , the Baryon Oscillation Spectroscopic Survey (BOSS) Emission-Line Lens Survey [ref] .
Testing General Relativity on Galactic Scales via DESI-BAO and Strong Lensing: Circumventing Assumptions on the Hubble Constant, Sound Horizon, and Dark Energy · SGL Data Sample · 0.88
-
This dataset integrates multiple surveys: 5 systems from the LSD survey [ref] , 26 from the Strong Lenses in the Legacy Survey (SL2S) [ref] , 57 from the Sloan Lens ACS Survey (SLACS) [ref] , 38 from the “SLACS for the Masses” extension (S4TM) [ref] , 21 from the BOSS Emission-Line Lens Survey (BELLS) [ref] , and 14 from the BELLS for GALaxy-Ly EmitteR sYstems survey (BELLS-GALLERY) [ref] .
A cosmographic analysis using DESI-DR2 and strong lensing: II. Distance Ratio measurements · Strong Gravitational Lensing- Distance Ratio · 0.97
Cites it as support 2 papers
-
The interpretation gains support from discrepancies observed in the relative astrometric shifts of lensed extended images [ref] .
Measuring Line-of-sight Distances to Haloes with Astrometric Lensing B-mode · Introduction · 0.98
-
Of course, translating kinematic data into estimates of gravitational potential has its own uncertainties and degeneracies (e.g. the mass anisotropy degeneracy for pressure supported systems), but the combination of the two datasets in the context of a single mass model has been proven to be very effective [ref] .
Time Delay Cosmography · The role of stellar kinematics · 0.98
Cites it as background 2 papers
-
Other studies have used astrometric shifts of lensed extended images [ref] .
Probing warm and mixed dark matter models using lensing shift power spectrum · Introduction · 0.84
-
Separating stellar and dark matter distributions requires breaking the degeneracy between the stellar initial mass function (IMF) and the dark matter fraction, which have been attempted using strong gravitational lensing [ref] , stellar dynamics [ref] , combining strong lensing and stellar dynamics [ref] , and combining strong and weak lensing [ref] .
The stellar and dark matter distributions in early-type galaxies measured by stacked weak gravitational lensing · Introduction · 0.80
Discussion
Know something about this paper? Leave a comment, or highlight any passage above to comment on it.