A Robust Determination of the Time Delay in 0957+561A, B and a Measurement of the Global Value of Hubble's Constant

Continued photometric monitoring of the gravitational lens system 0957+561A, B in the g and r bands with the Apache Point Observatory (APO) 3.5 m telescope during 1996 shows a sharp g-band event in the trailing (B) image light curve at the precise time predicted in an earlier paper. The prediction was based on the observation of the event during 1995 in the leading (A) image and on a differential time delay of 415 days. This success confirms the so-called short delay, and the absence of any such feature at a delay near 540 days rejects the long delay for this system, thus resolving a long-standing controversy. A series of statistical analyses of our light-curve data yield a best-fit delay of 417 ? 3 days (95% confidence interval) and demonstrate that this result is quite robust against variations in the analysis technique, data subsamples, and assumed parametric relationship of the two light curves. Recent improvements in the modeling of the lens system (consisting of a galaxy plus a galaxy cluster) allow us to derive a value of the global value (at z = 0.36) of Hubble's constant H0 using Refsdal's method, a simple and direct (single-step) distance determination based on experimentally verified and securely understood physics and geometry. The result is H0 = 64 ? 13 km s-1 Mpc-1 (for ? = 1), where this 95% confidence interval is dominantly due to remaining lens model uncertainties. However, it is reassuring that available observations of the lensing mass distribution overconstrain the model and thus provide an internal consistency check on its validity. We argue that this determination of the extragalactic distance scale (10% accurate at 1 ?) is now of comparable quality, in terms of both statistical and systematic uncertainties, to those based on more conventional techniques. Finally, we briefly discuss the prospects for improved H0 determinations using gravitational lenses, and some other possible implications and uses of the 0957+561A, B light curves.

[1]  S. Refsdal On the possibility of determining Hubble's parameter and the masses of galaxies from the gravitational lens effect , 1964 .

[2]  S. Refsdal On the Possibility of Testing Cosmological Theories from the Gravitational Lens Effect , 1966 .

[3]  S. Refsdal,et al.  Flux variations of QSO 0957 + 561 A, B and image splitting by stars near the light path , 1979, Nature.

[4]  D. Walsh,et al.  0957 + 561 A, B: twin quasistellar objects or gravitational lens? , 1979, Nature.

[5]  Iii Gott,et al.  Are heavy halos made of low mass stars - A gravitational lens test , 1981 .

[6]  P. Young,et al.  Q0957+561: Effects of random stars on the gravitational lens , 1981 .

[7]  Intrinsic variations of the double quasar 0957 + 56 AB , 1981, Nature.

[8]  J. B. Oke,et al.  Q0957+561: Detailed models of the gravitational lens effect , 1981 .

[9]  C. Alcock Gravitational lenses , 1982, Nature.

[10]  The nature of the light variations in the double QSO Q0957+561. , 1982 .

[11]  K. Subramanian,et al.  Gravitational lens model of the double QSO 0957+561 A, B incorporating VLBI features , 1984 .

[12]  I. Shapiro,et al.  On model-dependent bounds on H(0) from gravitational images Application of Q0957 + 561A,B , 1985 .

[13]  R. E. Schild,et al.  CCD camera brightness monitoring of Q0957 + 561 A, B , 1986 .

[14]  I. Shapiro,et al.  Degeneracies in parameter estimates for models of gravitational lens systems , 1988 .

[15]  F. Valdes,et al.  Detection of systematic gravitational lens galaxy image alignments - Mapping dark matter in galaxy clusters , 1990 .

[16]  Rudolph E. Schild,et al.  The time delay in the twin QSO Q0957 + 561 , 1990 .

[17]  D. N. Schramm,et al.  The case for the relativistic hot Big Bang cosmology , 1991, Nature.

[18]  A. Dar Are quasar redshifts cosmological , 1991 .

[19]  Gravitational lensing, time delay, and angular diameter distance , 1991 .

[20]  R. Schild,et al.  Microlensing in the Q0957 + 561 gravitational mirage , 1991 .

[21]  G. Rhee An estimate of the Hubble constant from the gravitational lensing of quasar Q0957+561 , 1991, Nature.

[22]  C. Kochanek Systematic effects in lens inversions - Aleph(1) exact models for 0957 + 561 , 1991 .

[23]  E. Falco,et al.  The role of microlensing in estimates of the relative time delay for the gravitational images of Q0957 + 561 , 1991 .

[24]  Irwin I. Shapiro,et al.  New model for the 0957 + 561 gravitational lens system - Bounds on masses of a possible black hole and dark matter and prospects for estimation of H0 , 1991 .

[25]  W. Press,et al.  The time delay of gravitational lens 0957+561. II: Analysis of radio data and combined optical-radio analysis , 1992 .

[26]  William H. Press,et al.  The Time Delay of Gravitational Lens 0957+561. I. Methodology and Analysis of Optical Photometric Data , 1992 .

[27]  Bernard F. Burke,et al.  The radio time delay in the double quasar 0957 + 561 , 1992 .

[28]  Sjur Refsdal Determining the Hubble parameter , 1992 .

[29]  R. Cen,et al.  The relation of local measures of Hubble's constant to its global value , 1992 .

[30]  R. Blandford,et al.  Cosmological Applications of Gravitational Lensing , 1992 .

[31]  G. Bernstein,et al.  A Large Arc in the Gravitational Lens System 0957+561 , 1993 .

[32]  D. Walsh,et al.  Global VLBI Observations of the Gravitational Lens System 0957+561A, B , 1994 .

[33]  J. Wambsganss,et al.  Parameter degeneracy in models of the quadruple lens system Q2237+0305 , 1994, astro-ph/9408084.

[34]  An Event in the Light Curve of 0957+561A and Prediction of the 1996 Image B Light Curve , 1995, astro-ph/9508145.

[35]  Measurement of the mass profile of abell 1689 , 1995, astro-ph/9503119.

[36]  The Dark Matter, Gas and Galaxy Distributions in Abell 2218: A Weak Gravitational Lensing and X-ray Analysis , 1995, astro-ph/9507008.

[37]  D. Thomson,et al.  Twin QSO Q0957+561 Time Delay Dataset , 1995 .

[38]  C. Kochanek,et al.  Astrophysical Applications of Gravitational Lensing , 1996 .

[39]  Optical Photometry of Quasar 0957+561A, B , 1996 .

[40]  N. Grogin,et al.  A New Model of the Gravitational Lens 0957+561 and a Limit on the Hubble Constant , 1996 .

[41]  R. Schild Microlensing Variability of the Gravitationally Lensed Quasar Q0957+561 A,B , 1996 .

[42]  Radio Measurement of the Time Delay in 0218+357 , 1996 .

[43]  Erratum: “A New Model of the Gravitational Lens 0957+561 and a Limit on the Hubble Constant” (ApJ, 464, 92 [1996]) , 1995, astro-ph/9512156.

[44]  Gravitational Lensing Of Quasar 0957+561 And The Determination Of H 0 , 1996 .

[45]  A Weak Gravitational Lensing Analysis of Abell 2390 , 1996, astro-ph/9602105.

[46]  I. Shapiro,et al.  An Estimate of H0 from Keck Spectroscopy of the Gravitational Lens System 0957+561 , 1997, astro-ph/9702152.