The GALAH survey uses the Two-Degree Field (2dF) fibre positioner with the HERMES spectrograph at the Anglo-Australian Telescope. Explore below to learn more about the Anglo-Australian Telescope and the HERMES spectrograph.
- The Anglo-Australian Telescope
- 2dF and HERMES
The Anglo-Australian Telescope
The Two-Degree Field fibre positioner installed at the top-end of the Anglo-Australian Telescope.
The GALAH Survey primarily uses the Anglo-Australian Telescope, a 4-metre equatorially-mounted telescope. It is located at Siding Spring Observatory in New South Wales, Australia, and is operated by the Australian National University on behalf of a consortium of 13 Australian Universities. Its function is to provide world-class observing facilities for Australian optical astronomers.
2dF and HERMES
The HERMES Spectrograph installed at the AAT.
GALAH observes using the HERMES spectrograph (Sheinis et al. 2015) at the Anglo-Australian Telescope. GALAH was the primary science driver for the HERMES, a high resolution (R~28,000 or 50,000) fibre-fed multi-object spectrometer. It has four non-contiguous spectral bands, covering a total of approximately 100 nm between about 470 nm and 790 nm. These bands were selected to permit the measurement of the abundances of as many elements as possible from the major nucleosynthetic processes.
HERMES utilizes the 2-degree field (2dF) positioner (Lewis et al. 2002). 2dF has two field plates, each of which has 392 science fibres and 8 guide bundles that can be allocated across a circular field with a two-degree diameter. One field plate can be set up by the fibre positioning robot while the other plate is being used for observation. Fibres subtend 2.1 arcseconds on the sky, with a positioning accuracy of 0.3 arcseconds, and have a minimum separation of about 30 arcseconds.
The fibres from the two 2dF plates are arranged in two pseudoslits that can move into place to inject light into the spectrograph. HERMES uses an off-axis collimator mirror, a series of dichroic elements, and volume phase holographic gratings to capture the following wavelength regions in four cameras with independent shutters:
|Band||λmin (nm)||λmax (nm)|
The spectra are dispersed in the horizontal direction in the raw data, with one spectrum trace for each fibre.
The light path of HERMES.
HERMES spectra have a signal-to-noise ratio of 100 per resolution element in one hour of exposure time for stars with an apparent magnitude of 14 in the relevant Johnson/Cousins filter (B for the blue camera, V for the green camera, R for the red camera and I for the IR camera). The blue and green cameras use 16 micron, standard silicon detectors; the red camera has a 40 micron, deep depletion device with fringe suppression and an ER1 coating; and the IR camera has a 100-micron bulk silicon device with fringe suppression and a “Multi-9” coating. Further details on 2dF and HERMES can be found at the Anglo-Australian Telescope website.
2018 Field Flattening Lens Replacement
In the first half of 2018, the original field flattening lenses of HERMES were replaced (Edgar et al. 2018). The original glass contained uranium that emitted α particles, which caused the saturated points and vertical readout streaks when they were captured by the HERMES CCDs. The point spread function in the HERMES cameras changed as a result of changing the field flattening lenses, and is now larger and less symmetric in the corners of the detectors. As part of HERMES recommissioning, the GALAH team fed light from a Fabry-Perot interferometer into HERMES to characterise the new PSF across each detector, and this information has been incorporated into the data reduction procedure.
Technical papers describing HERMES
These technical papers describe various aspects of the design, construction, and first light performance of HERMES.
- Radioactive emission from high-index,optical glasses and atypical effects on CCDs
Edgar et al. (2018) SPIE 10706 1070633 (doi:10.1117/12.2307305)
- First light results from the HERMES spectrograph at the AAT
Sheinis (2016) SPIE 9908 99081C (doi:10.1117/12.2234334, arXiv:1509.00129)
- First light results from the High Efficiency and Resolution Multi-Element Spectrograph at the Anglo-Australian Telescope
Sheinis et al. (2015) JATIS 1 035002 (doi:10.1117/1.JATIS.1.3.035002)
- First light results from the Hermes spectrograph at the AAT
Sheinis et al. (2014) SPIE 9147 91470Y (doi:10.1117/12.2055595)
- The deterministic optical alignment of the HERMES spectrograph
Gers and Staszak (2014) SPIE 9151 915113 (doi:10.1117/12.2055574)
- The software for the AAT’s HERMES instrument
Farrell et al. (2014) SPIE 9152 915223 (doi:10.1117/12.2054805)
- HERMES travels by CAN bus
Waller et al. (2014) SPIE 9152 91522A (doi:10.1117/12.2055022)
- Metrology measurements for large-aperture VPH gratings
Zheng et al. (2013) SPIE 8838 88380G (doi:10.1117/12.2024493)
- Integrating the HERMES spectrograph for the AAT
Heijmans et al. (2012) SPIE 8446 84460W (doi:10.1117/12.925806)
- The AAO fiber instrument data simulator
Goodwin et al. (2012) SPIE 8446 84462D (doi:10.1117/12.924990)
- Hermes: the engineering challenges
Brzeski et al. (2012) SPIE 8446 84464N (doi:10.1117/12.924635)
- Design and development of the high-resolution spectrograph HERMES and the unique volume phase holographic gratings
Heijmans et al. (2011) SPIE 8167 81671A (doi:10.1117/12.897273)
- Design and development of the fibre cable and fore optics of the HERMES Spectrograph for the Anglo-Australian Telescope (AAT)
Brzeski et al. (2011) SPIE 8125 812504 (doi:10.1117/12.896389)
- HERMES: revisions in the design for a high-resolution multi-element spectrograph for the AAT
Barden et al. (2010) SPIE 7735 773509 (doi:10.1117/12.856103)
- Data simulator for the HERMES instrument
Goodwin et al. (2010) SPIE 7735 77357U (doi:10.1117/12.856773)
- Concepts for a high-resolution multi-object spectrograph for galactic archeology on the Anglo-Australian Telescope
Barden et al. (2008) SPIE 7014 70144J (doi:10.1117/12.788549)