TY - JOUR
T1 - The redshift of the gravitationally lensed radio source PKS 1830-211
AU - Lidman, C.
AU - Courbin, F.
AU - Meylan, G.
AU - Broadhurst, T.
AU - Frye, B.
AU - Welch, W. J.W.
N1 - Funding Information:
The authors would like to thank D. Hutsemékers for useful conversations on reddening by the lensing galaxy. F. C. is supported by contracts ARC 94/99-178 “Action de Recherche Concertée de la Communauté Franc¸aise” and Pôle d’Attraction Interuniversitaire P4/05 (SSTC, Belgium).
PY - 1999/4/1
Y1 - 1999/4/1
N2 - We report on the spectroscopic identification and the long-awaited redshift measurement of the heavily obscured, gravitationally lensed radio source PKS 1830-211, which was first observed as a radio Einstein ring. The northeast component of the doubly imaged core is identified, in our infrared spectrum covering the wavelength range 1.5-2.5 μm, as an impressively reddened quasar at z = 2.507 ± 0.002. The mass contained within the Einstein ring radius is M(r < 2.1 h-1 kpc) = 6.3 × 1010 h-1 M⊙ for ΩM = 1 or M(r < 2.4 h-1 kpc) = 7.4 × 1010 h-1 M⊙ for ΩM = 0.3. Our redshift measurement, together with the recently measured time delay (Lovell et al.), means that we are a step closer to determining H0 from this lens. Converting the time delay into H0 by using existing models leads to high values of the Hubble parameter, H0 = 65+15-9 for ΩM = 1 and H0 = 7618-10, for ΩM = 0.3. Since the lensing galaxy lies very close to the center of the lensed ring, improving the error bars on H0 will require not only a more precise time delay measurement but also very precise astrometry of the whole system.
AB - We report on the spectroscopic identification and the long-awaited redshift measurement of the heavily obscured, gravitationally lensed radio source PKS 1830-211, which was first observed as a radio Einstein ring. The northeast component of the doubly imaged core is identified, in our infrared spectrum covering the wavelength range 1.5-2.5 μm, as an impressively reddened quasar at z = 2.507 ± 0.002. The mass contained within the Einstein ring radius is M(r < 2.1 h-1 kpc) = 6.3 × 1010 h-1 M⊙ for ΩM = 1 or M(r < 2.4 h-1 kpc) = 7.4 × 1010 h-1 M⊙ for ΩM = 0.3. Our redshift measurement, together with the recently measured time delay (Lovell et al.), means that we are a step closer to determining H0 from this lens. Converting the time delay into H0 by using existing models leads to high values of the Hubble parameter, H0 = 65+15-9 for ΩM = 1 and H0 = 7618-10, for ΩM = 0.3. Since the lensing galaxy lies very close to the center of the lensed ring, improving the error bars on H0 will require not only a more precise time delay measurement but also very precise astrometry of the whole system.
KW - Cosmology: observations
KW - Gravitational lensing
KW - Quasars: individual (PKS 1830-211)
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U2 - 10.1086/311949
DO - 10.1086/311949
M3 - Article
AN - SCOPUS:0033110601
SN - 0004-637X
VL - 514
SP - L57-L60
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 2 PART 2
ER -