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| [ALB2017] DES J0408-5354 , the SIMBAD biblio (37 results) | C.D.S. - SIMBAD4 rel 1.8 - 2026.10.19CEST04:55:07 |
| Bibcode/DOI | Score |
in Title|Abstract| Keywords |
in a table | in teXt, Caption, ... | Nb occurence | Nb objects in ref |
Citations (from ADS) |
Title | First 3 Authors |
|---|---|---|---|---|---|---|---|---|---|
| 2017ApJ...838L..15L | 756 | T | X C | 17 | 9 | 26 |
Discovery of the lensed quasar system DES J0408-5354. |
LIN H., BUCKLEY-GEER E., AGNELLO A., et al. | |
| 2017MNRAS.471.2013A | 40 | X | 1 | 22 | 22 | Quasar lenses and galactic streams: outlier selection and Gaia multiplet detection. | AGNELLO A. | ||
| 2017MNRAS.472.4038A | 79 | T | 1 | 12 | 14 |
Models of the strongly lensed quasar DES J0408-5354. |
AGNELLO A., LIN H., BUCKLEY-GEER L., et al. | ||
|
2018A&A...616A.183B |
84 | X | 2 | 5 | 21 | COSMOGRAIL. XVII. Time delays for the quadruply imaged quasar PG 1115+080. | BONVIN V., CHAN J.H.H., MILLON M., et al. | ||
|
2018A&A...618A..56D |
80 | C | 4 | 20 | 19 | Gaia GraL: Gaia DR2 gravitational lens systems. II. The known multiply imaged quasars. | DUCOURANT C., WERTZ O., KRONE-MARTINS A., et al. | ||
| 2019MNRAS.483.5649S | 712 | D | X C | 17 | 13 | 70 | Is every strong lens model unhappy in its own way? Uniform modelling of a sample of 13 quadruply+ imaged quasars. | SHAJIB A.J., BIRRER S., TREU T., et al. | |
| 2019MNRAS.485.5086S | 41 | X | 1 | 5 | 2 | Spectroscopic confirmation and modelling of two lensed quadruple quasars in the Dark Energy Survey public footprint. | SPINIELLO C., SERGEYEV A.V., MARCHETTI L., et al. | ||
|
2019A&A...629A..97B |
41 | X | 1 | 11 | ~ | COSMOGRAIL. XVIII. time delays of the quadruply lensed quasar WFI2033-4723. | BONVIN V., MILLON M., CHAN J.H.-H., et al. | ||
| 2020ApJ...892L..27B | 16 | D | 1 | 7 | ~ | Could quasar lensing time delays hint to a core component in halos, instead of H0 tension? | BLUM K., CASTORINA E. and SIMONOVIC M. | ||
| 2020ApJ...895L..29L | 41 | X | 1 | 7 | ~ | Determining model-independent H0 and consistency tests. | LIAO K., SHAFIELOO A., KEELEY R.E., et al. | ||
| 2020MNRAS.494.6072S | 955 | T A | D | X C F | 21 | 18 | 155 |
STRIDES: a 3.9 per cent measurement of the Hubble constant from the strong lens system DES J0408-5354. |
SHAJIB A.J., BIRRER S., TREU T., et al. |
| 2020A&A...639A.101M | 240 | D | X | 6 | 7 | 132 | TDCOSMO. I. An exploration of systematic uncertainties in the inference of H0 from time-delay cosmography. | MILLON M., GALAN A., COURBIN F., et al. | |
|
2020MNRAS.498.3241B |
4157 | T K A | D | S X C | 99 | 11 | ~ |
STRIDES: Spectroscopic and photometric characterization of the environment and effects of mass along the line of sight to the gravitational lenses DES J0408-5354 and WGD 2038-4008. |
BUCKLEY-GEER E.J., LIN H., RUSU C.E., et al. |
| 2020A&A...642A.194G | 387 | D | X C | 9 | 9 | ~ | TDCOSMO. III. Dark matter substructure meets dark energy. The effects of (sub)halos on strong-lensing measurements of H0. | GILMAN D., BIRRER S. and TREU T. | |
| 2020MNRAS.499.2845H | 60 | D | X | 2 | 28 | 58 | The KBC void and Hubble tension contradict ΛCDM on a Gpc scale - Milgromian dynamics as a possible solution. | HASLBAUER M., BANIK I. and KROUPA P. | |
| 2020ApJ...904L..22L | 247 | S X | 5 | 7 | ~ | Investigating the Hubble constant tension: two numbers in the standard cosmological model. | LIN W., MACK K.J. and HOU L. | ||
| 2020A&A...643A.165B | 63 | D | X | 2 | 40 | 233 | TDCOSMO. IV. Hierarchical time-delay cosmography - joint inference of the Hubble constant and galaxy density profiles. | BIRRER S., SHAJIB A.J., GALAN A., et al. | |
| 2021MNRAS.501..784D | 523 | D | S X F | 11 | 8 | 46 | The Hubble constant from eight time-delay galaxy lenses. | DENZEL P., COLES J.P., SAHA P., et al. | |
| 2021MNRAS.503.1096D | 43 | X | 1 | 25 | 31 | Time delay lens modelling challenge. | DING X., TREU T., BIRRER S., et al. | ||
| 2021MNRAS.503.2179Q | 42 | X | 1 | 7 | ~ | Measurements of the Hubble constant and cosmic curvature with quasars: ultracompact radio structure and strong gravitational lensing. | QI J.-Z., ZHAO J.-W., CAO S., et al. | ||
| 2021MNRAS.504.1340G | 17 | D | 1 | 47 | ~ | Galaxy-lens determination of H0: the effect of the ellipse + shear modelling assumption. | GOMER M.R. and WILLIAMS L.L.R. | ||
| 2021A&A...652A...7C | 84 | F | 1 | 8 | ~ | TDCOSMO. VI. Distance measurements in time-delay cosmography under the mass-sheet transformation. | CHEN G.C.-F., FASSNACHT C.D., SUYU S.H., et al. | ||
| 2021MNRAS.508.5449D | 268 | D | X C | 6 | 35 | 6 | Bayesian analysis of quasar light curves with a running optimal average: new time delay measurements of COSMOGRAIL gravitationally lensed quasars. | DONNAN F.R., HORNE K. and HERNANDEZ SANTISTEBAN J.V. | |
| 2022MNRAS.514.1433W | 60 | D | X | 2 | 7 | ~ | Constraints on interacting dark energy models from time-delay cosmography with seven lensed quasars. | WANG L.-F., ZHANG J.-H., HE D.-Z., et al. | |
| 2022MNRAS.517..576H | 49 | X | 1 | 2 | 12 | Revealing the late-time transition of H0: relieve the Hubble crisis. | HU J.P. and WANG F.Y. | ||
| 2022MNRAS.517.3377S | 187 | D | C F | 9 | 17 | 6 | Red quasars blow out molecular gas from galaxies during the peak of cosmic star formation. | STACEY H.R., COSTA T., McKEAN J.P., et al. | |
| 2022A&A...667A.123S | 46 | X | 1 | 4 | 13 | TDCOSMO IX. Systematic comparison between lens modelling software programs: Time-delay prediction for WGD 2038-4008. | SHAJIB A.J., WONG K.C., BIRRER S., et al. | ||
| 2023MNRAS.518.1260S | 131 | X C | 2 | 28 | 18 | STRIDES: automated uniform models for 30 quadruply imaged quasars. | SCHMIDT T., TREU T., BIRRER S., et al. | ||
| 2023MNRAS.520.5982H | 44 | X | 1 | 3 | 2 | Measuring line-of-sight shear with Einstein rings: a proof of concept. | HOGG N.B., FLEURY P., LARENA J., et al. | ||
| 2023MNRAS.521.4963D | 44 | X | 1 | 8 | 1 | Model-independent determination of H0 and Ω_K, 0_ using time-delay galaxy lenses and gamma-ray bursts. | DU S.-S., WEI J.-J., YOU Z.-Q., et al. | ||
| 2023MNRAS.519.2528M | 61 | D | X | 2 | 31 | ~ | Model selection using time-delay lenses. | MELIA F., WEI J.-J. and WU X.-F. | |
| 2023ApJ...953..189D | 87 | X | 2 | 1 | ~ | Mass Reconstruction of Galaxy-scale Strong Gravitational Lenses Using a Broken Power-law Model. | DU W., FU L., SHU Y., et al. | ||
| 2024A&A...685A..15E | 45 | X | 1 | 12 | ~ | The missing quasar image in the gravitationally lensed quasar HE0230-2130: Implications for the cored lens mass distribution and dark satellites. | ERTL S., SCHULDT S., SUYU S.H., et al. | ||
| 2025MNRAS.542.1063H | 47 | X | 1 | 1 | ~ | Constraints on transition redshift utilizing the latest H(z) measurements and comments on the Hubble tension. | HU J.P., JIA X.D., GAO D.H., et al. | ||
| 2025A&A...701A.220L | 47 | X | 1 | 7 | ~ | Determining H0 from a distance sum rule that combines gamma-ray bursts with observational Hubble data and strong gravitational lensing. | LUONGO O. and MUCCINO M. | ||
| 2025A&A...704A..63T | 905 | D | X C | 19 | 23 | ~ | TDCOSMO 2025: Cosmological constraints from strong lensing time delays. | TDCOSMO COLLABORATION, BIRRER S., BUCKLEY-GEER E.J., et al. | |
|
2026A&A...705A..13M |
20 | D | 1 | 69 | ~ | TDCOSMO XXI. Accurate stellar velocity dispersions of the SL2S lens sample and the fundamental plane of the lensing mass. | MOZUMDAR P., KNABEL S., TREU T., et al. |