Jump to content

GOTO (telescope array)

Add links
From Wikipedia, the free encyclopedia
(Redirected from GOTO (observatory))
For the type of computer-controlled telescope mounts, see GoTo (telescopes).
GOTO
GOTO-N with both domes open.
GOTO-N with both domes open.
Alternative namesGravitational-wave Optical Transient Observer Edit this at Wikidata
Part ofRoque de los Muchachos Observatory
Siding Spring Observatory Edit this on Wikidata
Wavelength420 nm (710 THz)–685 nm (438 THz)
First lightJune 2017 (2017-06)
Telescope styleNewtonian
Number of telescopes32 Edit this on Wikidata
Diameter400 mm (1 ft 4 in) Edit this at Wikidata
Angular resolution0.31 arcsecond Edit this on Wikidata
Collecting area0.4m2 per unit telescope, 3.2m2 per system, 12.8m2 total.
Focal length960mm (f/2.4)
MountingEquatorial
Websitegoto-observatory.org
[edit on Wikidata]

The Gravitational-wave Optical Transient Observer (GOTO) is an array of robotic optical telescopes optimized for the discovery of optical counterparts to gravitational wave events[1] and other multi-messenger signals. The array consists of a network of telescope systems, with each system consisting of eight 0.4m telescopes on a single mounting.[2]

As of May 2023 the network consists of two sites, each with two systems. GOTO-N (North) located at the Roque de los Muchachos Observatory (ORM) on the island of La Palma, Spain[3] and GOTO-S (South) located at Siding Spring Observatory (SSO), Australia.[4]

The project is run by an international consortium of universities and other research institutes, including the University of Warwick, Monash University, the University of Sheffield, the University of Leicester, Armagh Observatory, the National Astronomical Research Institute of Thailand, the Instituto de Astrofísica de Canarias, the University of Portsmouth, and the University of Turku.[5]

Design and operation

[edit]

Telescopes

[edit]

Each GOTO system can point independently, whilst each unit telescope (UT) has a fixed orientation on the mount so all 8 must be pointed at once. Each UT's pointing is offset from the others to cover the adjacent area of sky, with a small overlap between them. This results in each GOTO system acting as a single large telescope with a very wide field of view (FoV).[2]

The Andromeda Galaxy, with an overlay showing the field of view of a single GOTO unit telescope.
Relative positions of each unit telescope in a single GOTO system.

The UTs are ASA H400 Newtonian telescopes, each with an aperture of 400mm and a focal length of 960mm (f/2.4).[2] Attached to each telescope is a focuser, filter wheel, and a Finger Lakes Instrumentation (FLI) ML50100 camera,[2] based on the Onsemi KAF-50100 CCD sensor.[6] The fast focal ratio of f/2.4 and large image sensor result in a relatively large field of view, with each GOTO system having a total FoV of approximately 40 square degrees,[2] around 200x the area of the full Moon in the sky. The fast focal ratio also means that only a small amount of time is needed to observe each area of the sky, with each visit requiring only 3 minutes of exposure time.[2]

Identifying transients

[edit]

GOTO utilises difference imaging to identify changes of existing objects and the appearance of new transients.[7] Images of the sky are matched to previous observations of the same region, finding the difference between these two images will show only the changes in the new image. Sources within these difference images can then be detected automatically. Using difference imaging in this way produces many thousands of candidate sources per image, the vast majority of which are artefacts of the processing and not real transients.[8][9] GOTO utilises a convolutional neural network based 'real-bogus' classifier to identify which sources are likely to be real.[9]

Gamma-ray bursts

[edit]

In addition to follow-up of gravitational wave events, GOTO can respond to detections of gamma-ray bursts (GRBs).[10] On September 11, 2023, the Fermi Gamma-ray Space Telescope detected a gamma ray burst (GRB 230911A)[11] and follow-up observations by GOTO discovered an optical counterpart (GOTO23akf/AT 2023shv),[12] which was later confirmed as a GRB afterglow by the Swift X-ray telescope.[13]

All-sky survey

[edit]
location of GOTO-N in La Palma off the coast of Morocco and GOTO-S in eastern Australia
GOTO-N
GOTO-N
GOTO-S
GOTO-S
class=notpageimage|
Locations of GOTO-N and GOTO-S.

GOTO's typical mode of operation when not performing a follow-up campaign is to survey the entire visible sky. As there are sites located in both the northern and southern hemispheres, the visible sky for GOTO is all areas which are visible at night from anywhere on the Earth. If both sites have good weather conditions the entire visible sky can be observed every 2–3 days.[2]

These observations are processed using difference imaging which allows for serendipitous discovery of transients unrelated to multi-messenger events, like supernovae, tidal disruption events, and fast blue optical transients.[7]

History

[edit]
Total
Monthly
Total (line) and monthly (bar) count of transients discovered by GOTO between 2020 and September 11 2024.

The first phase of GOTO's development was the deployment of a prototype system located at the planned site of the northern node, consisting of four unit telescopes on a custom-built mount.[7] The prototype system was deployed during the second LIGO-Virgo Collaboration (LVC) observing run (O2), achieving first light in June 2017[7] with its official inauguration on July 3, 2017.[3]

The prototype system was active during the first half of the third LVC observing run (O3a), which ran between April and October 2019.[14] During this time GOTO was able to respond to gravitational-wave events and begin observing within one minute of alerts being received (if the source region was visible).[15]

In late 2019 funding was awarded to expand the network with two full GOTO systems a duplicate site in Australia.[16] In 2020 the first full system of the northern node was being deployed, with the second system planned for early 2021 and the Australian site planned for later that year.[17]

The deployment of the second northern system was completed in August 2021[18] and, despite delays due to the 2021 volcanic eruption, the full northern node was completed in December 2021 with the upgrade of the prototype to the final hardware configuration.[19]

By the end of 2022 the site for the second GOTO node (GOTO-S) had been prepared at Siding Spring Observatory (SSO) and the two domes installed.[20][21] In May 2023 it was announced that both systems at SSO had been successfully installed.[22]

Discoveries

[edit]

As of September 11, 2024, data from GOTO has been used in the discovery of 1013 astronomical transients, of which 141 have been classified as supernovae and one as a tidal disruption event.[23][24]

References

[edit]
  1. ^ "Neutron stars: New telescope detects dead suns colliding". BBC News. 21 July 2022. Retrieved 24 January 2024.
  2. ^ a b c d e f g Dyer, Martin J.; Steeghs, Danny; Galloway, Duncan K.; Dhillon, Vik S.; O'Brien, Paul; Ramsay, Gavin; Noysena, Kanthanakorn; Pallé, Enric; Kotak, Rubina; Breton, Rene; Nuttall, Laura; Pollacco, Don; Ulaczyk, Krzysztof; Lyman, Joseph; Ackley, Kendall D. (13 December 2020). "The Gravitational-wave Optical Transient Observer (GOTO)". In Marshall, Heather K.; Spyromilio, Jason; Usuda, Tomonori (eds.). Ground-based and Airborne Telescopes VIII. Vol. 11445. SPIE. pp. 1355–1362. arXiv:2012.02685. Bibcode:2020SPIE11445E..7GD. doi:10.1117/12.2561008. ISBN 978-1-5106-3677-4. S2CID 216906754.
  3. ^ a b "GOTO, a new robotic telescope for the Roque de los Muchachos Observatory". Instituto de Astrofísica de Canarias • IAC. 3 July 2017. Retrieved 24 January 2024.
  4. ^ Yazgin, Evrim (7 July 2022). "New telescopes in Australia to help find gravitational waves". cosmosmagazine.com. Retrieved 24 January 2024.
  5. ^ Steeghs, Danny (2017-11-02). "Chasing light from the crest of a wave". Nature Astronomy. 1 (11): 741. Bibcode:2017NatAs...1..741S. doi:10.1038/s41550-017-0317-8. ISSN 2397-3366.
  6. ^ "New KAF-50100 sensor with microlenses". www.flicamera.com. Retrieved 2024-01-30.
  7. ^ a b c d Steeghs, D; Galloway, D K; Ackley, K; Dyer, M J; Lyman, J; Ulaczyk, K; Cutter, R; Mong, Y-L; Dhillon, V; O'Brien, P; Ramsay, G; Poshyachinda, S; Kotak, R; Nuttall, L K; Pallé, E; Breton, R P; Pollacco, D; Thrane, E; Aukkaravittayapun, S; Awiphan, S; Burhanudin, U; Chote, P; Chrimes, A; Daw, E; Duffy, C; Eyles-Ferris, R; Gompertz, B; Heikkilä, T; Irawati, P; Kennedy, M R; Killestein, T; Kuncarayakti, H; Levan, A J; Littlefair, S; Makrygianni, L; Marsh, T; Mata-Sanchez, D; Mattila, S; Maund, J; McCormac, J; Mkrtichian, D; Mullaney, J; Noysena, K; Patel, M; Rol, E; Sawangwit, U; Stanway, E R; Starling, R; Strøm, P; Tooke, S; West, R; White, D J; Wiersema, K (April 2022). "The Gravitational-wave Optical Transient Observer (GOTO): prototype performance and prospects for transient science". Monthly Notices of the Royal Astronomical Society. 511 (2): 2405–2422. arXiv:2110.05539. doi:10.1093/mnras/stac013.
  8. ^ Brink, Henrik; Richards, Joseph W.; Poznanski, Dovi; Bloom, Joshua S.; Rice, John; Negahban, Sahand; Wainwright, Martin (2013-10-21). "Using machine learning for discovery in synoptic survey imaging data". Monthly Notices of the Royal Astronomical Society. 435 (2): 1047–1060. arXiv:1209.3775. doi:10.1093/mnras/stt1306. ISSN 1365-2966.
  9. ^ a b Killestein, T L; Lyman, J; Steeghs, D; Ackley, K; Dyer, M J; Ulaczyk, K; Cutter, R; Mong, Y-L; Galloway, D K; Dhillon, V; O'Brien, P; Ramsay, G; Poshyachinda, S; Kotak, R; Breton, R P (2021-04-09). "Transient-optimized real-bogus classification with Bayesian convolutional neural networks – sifting the GOTO candidate stream". Monthly Notices of the Royal Astronomical Society. 503 (4): 4838–4854. arXiv:2102.09892. doi:10.1093/mnras/stab633. ISSN 0035-8711.
  10. ^ Mong, Y-L; Ackley, K; Galloway, D K; Dyer, M; Cutter, R; Brown, M J I; Lyman, J; Ulaczyk, K; Steeghs, D; Dhillon, V; O’Brien, P; Ramsay, G; Noysena, K; Kotak, R; Breton, R (2021-09-07). "Searching for Fermi GRB optical counterparts with the prototype Gravitational-wave Optical Transient Observer (GOTO)". Monthly Notices of the Royal Astronomical Society. 507 (4): 5463–5476. arXiv:2108.11802. doi:10.1093/mnras/stab2499. ISSN 0035-8711.
  11. ^ "GCN - Circulars - 34652 - GRB 230911A: Fermi GBM Final Real-time Localization". gcn.nasa.gov. Retrieved 2024-08-21.
  12. ^ "AT 2023shv | Transient Name Server". www.wis-tns.org. Retrieved 2024-08-21.
  13. ^ Belkin, S.; Gompertz, B. P.; Kumar, A.; Ackley, K.; Galloway, D. K.; Jiménez-Ibarra, F.; Killestein, T. L.; O’Neill, D.; Wiersema, K.; Malesani, D. B.; Levan, A. J.; Lyman, J.; Dyer, M. J.; Ulaczyk, K.; Steeghs, D. (2024-01-04). "GRB 230911A: The First Discovery of a Fermi GRB Optical Counterpart with the Gravitational-wave Optical Transient Observer (GOTO)". Research Notes of the AAS. 8 (1): 6. Bibcode:2024RNAAS...8....6B. doi:10.3847/2515-5172/ad1876. ISSN 2515-5172.
  14. ^ Abbott, R.; Abe, H.; Acernese, F.; Ackley, K.; Adhicary, S.; Adhikari, N.; Adhikari, R. X.; Adkins, V. K.; Adya, V. B.; Affeldt, C.; Agarwal, D.; Agathos, M.; Aguiar, O. D.; Aiello, L.; Ain, A. (2023-08-01). "Open Data from the Third Observing Run of LIGO, Virgo, KAGRA, and GEO". The Astrophysical Journal Supplement Series. 267 (2): 29. arXiv:2302.03676. Bibcode:2023ApJS..267...29A. doi:10.3847/1538-4365/acdc9f. ISSN 0067-0049.
  15. ^ Gompertz, B P; Cutter, R; Steeghs, D; Galloway, D K; Lyman, J; Ulaczyk, K; Dyer, M J; Ackley, K; Dhillon, V S; O’Brien, P T; Ramsay, G; Poshyachinda, S; Kotak, R; Nuttall, L; Breton, R P (2020-09-01). "Searching for electromagnetic counterparts to gravitational-wave merger events with the prototype Gravitational-Wave Optical Transient Observer (GOTO-4)". Monthly Notices of the Royal Astronomical Society. 497 (1): 726–738. arXiv:2004.00025. doi:10.1093/mnras/staa1845. ISSN 0035-8711.
  16. ^ "Funding Approved For GOTO Expansion". GOTO Observatory. 2020-04-05. Retrieved 2024-01-25.
  17. ^ Dyer, Martin J.; Steeghs, Danny; Galloway, Duncan K.; Dhillon, Vik S.; O'Brien, Paul; Ramsay, Gavin; Noysena, Kanthanakorn; Pallé, Enric; Kotak, Rubina; Breton, Rene; Nuttall, Laura; Pollacco, Don; Ulaczyk, Krzysztof; Lyman, Joseph; Ackley, Kendall D. (2020-12-13). "The Gravitational-wave Optical Transient Observer (GOTO)". In Marshall, Heather K.; Spyromilio, Jason; Usuda, Tomonori (eds.). Ground-based and Airborne Telescopes VIII (PDF). Vol. 11445. SPIE. pp. 1355–1362. arXiv:2012.02685. Bibcode:2020SPIE11445E..7GD. doi:10.1117/12.2561008. ISBN 978-1-5106-3677-4. S2CID 216906754.
  18. ^ Ulaczyk, Krzysztof (2021-08-01). "Second GOTO system installed at Roque de Los Muchachos Observatory". goto-observatory.org. Retrieved 2024-01-25.
  19. ^ Ulaczyk, Krzysztof (2021-12-08). "Full northern node deployed!". goto-observatory.org. Retrieved 2024-01-25.
  20. ^ "GOTO-South". Australian National University. 2024-01-29. Retrieved 2024-01-29.
  21. ^ Ulaczyk, Krzysztof (2022-12-08). "New GOTO domes erected in Siding Spring Observatory". goto-observatory.org. Retrieved 2024-01-25.
  22. ^ Ulaczyk, Krzysztof (2023-05-08). "Two new arrays of telescopes installed at Siding Spring Observatory". goto-observatory.org. Retrieved 2024-01-26.
  23. ^ "TNS Transients Statistics, Skymaps and Plots | Transient Name Server". www.wis-tns.org. International Astronomical Union. Archived from the original on 11 September 2024. Retrieved 11 September 2024.
  24. ^ "AT 2023lli | Transient Name Server". www.wis-tns.org. Archived from the original on 2024-02-03. Retrieved 2024-02-03.
Retrieved from "https://en.wikipedia.org/w/index.php?title=GOTO_(telescope_array)&oldid=1258405639"