Spectroscopic discovery is by far the most prolific means of identification of Galaxy-Galaxy Lensing candidates, with follow-up Hubble Space Telescope (HST) imaging providing high-resolution, high signal-to-noise data for lens modeling, leading to results such as those of the Sloan Lens ACS (SLACS) survey, and ongoing discovery using the Baryon Oscillation Spectroscopic Survey (BOSS) of the Sloan Digital Sky Survey III (SDSS3).
The basic premise behind the spectroscopic selection of Bolton et al. 2004AstronJ127(2004)1860 was to find background emission lines within the same 3 arcsecond-diameter solid angle
covered by the SDSS spectroscopic fiber remaining after subtracting best-fit galaxy templates to the target spectrum (lens candidate). Since the ratio of emission line wavelengths is independent of source redshift, the ratio of background emission lines must be identified at particular, known values.
The procedure following Bolton et al. 2006ApJ638(2006)703, Bolton et al. 2008ApJ682(2008)964 looked for either resolved or blended background OII doublets at 3727.092 Å and 3729.875 Å, respectively, times a factor of (1+z), where z is the computed redshift of the background emission line (source) galaxy. SLACS candidates were also required to exhibit two longer wavelength emission lines: Hβ at a wavelength of 4862.683 Å (1+z), and one (or both) of the OIII emission lines, at wavelengths of 4960.295 Å , or 5008.239 Å times (1+z), respectively.
Each SDSS image of candidate pairs was visually inspected to verify the absence of bright
neighboring galaxies that could produce anomalous emission lines, and to determine the morphology of the lens galaxy
-- SDSS images have been visually inspected to identify spiral galaxies sufficiently inclined for galaxy rotation
curve measurements.
The probability of finding a galaxy-galaxy lens using the spectroscopic discovery method was considered in Dobler et al. 2008ApJ685(2008)57 for the SLACS survey, including selection effects such as the finite size of the spectroscopic fiber which selects against large separation lenses, and the effectiveness of spectral noise modeling which selects against sources that have redshifted emission lines coincident with strong emission lines in the sky. The finite wavelength range of the spectrographs places an upper limit on detecting high source redshifts.
Investigators may download reduced HST exposures