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A terrestrial planet candidate in a temperate orbit around Proxima Centauri
- Guillem Anglada-Escudé1,
- Pedro J. Amado2,
- John Barnes3,
- Zaira M. Berdiñas2,
- R. Paul Butler4,
- Gavin A. L. Coleman1,
- Ignacio de la Cueva5,
- Stefan Dreizler6,
- Michael Endl7,
- Benjamin Giesers6,
- Sandra V. Jeffers6,
- James S. Jenkins8,
- Hugh R. A. Jones9,
- Marcin Kiraga10,
- Martin Kürster11,
- Marίa J. López-González2,
- Christopher J. Marvin6,
- Nicolás Morales2,
- Julien Morin12,
- Richard P. Nelson1,
- José L. Ortiz2,
- Aviv Ofir13,
- Sijme-Jan Paardekooper1,
- Ansgar Reiners6,
- Eloy Rodríguez2,
- Cristina Rodrίguez-López2,
- Luis F. Sarmiento6,
- John P. Strachan1,
- Yiannis Tsapras14,
- Mikko Tuomi9 &
- …
- Mathias Zechmeister6
Naturevolume 536, pages437–440 (2016)Cite this article
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Abstract
At a distance of 1.295 parsecs1, the red dwarf Proxima Centauri (α Centauri C, GL 551, HIP 70890 or simply Proxima) is the Sun’s closest stellar neighbour and one of the best-studied low-mass stars. It has an effective temperature of only around 3,050 kelvin, a luminosity of 0.15 per cent of that of the Sun, a measured radius of 14 per cent of the radius of the Sun2 and a mass of about 12 per cent of the mass of the Sun. Although Proxima is considered a moderately active star, its rotation period is about 83 days (ref.3) and its quiescent activity levels and X-ray luminosity4 are comparable to those of the Sun. Here we report observations that reveal the presence of a small planet with a minimum mass of about 1.3 Earth masses orbiting Proxima with a period of approximately 11.2 days at a semi-major-axis distance of around 0.05 astronomical units. Its equilibrium temperature is within the range where water could be liquid on its surface5.
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Acknowledgements
We thank E. Gerlach, R. Street and U. Seemann for their support to the science preparations. We thank P. Micakovic, M. M. Mutter (QMUL), R. Ivison, G. Hussain, I. Saviane, O. Sandu, L. L. Christensen, R. Hook and the personnel at La Silla (ESO) for making the PRD campaign possible. The authors acknowledge support from the following funding grants: Leverhulme Trust/UK RPG-2014-281 (H.R.A.J., G.A.-E. and M.T.); MINECO/Spain AYA-2014-54348-C3-1-R (P.J.A., C.R.-L., Z.M.B. and E.R.); MINECO/Spain ESP2014-54362-P (M.J.L.-G.); MINECO/Spain AYA-2014-56637-C2-1-P (J.L.O. and N.M.); J.A./Spain 2012-FQM1776 (J.L.O. and N.M.); CATA-Basal/Chile PB06 Conicyt (J.S.J.); Fondecyt/Chile project #1161218 (J.S.J.); STFC/UK ST/M001008/1 (R.P.N., G.A.L.C. and G.A.-E.); STFC/UK ST/L000776/1 (J.B.); ERC/EU Starting Grant #279347 (A.R., L.F.S. and S.V.J.); DFG/Germany Research Grants RE 1664/9-2 (A.R.); RE 1664/12-1 (M.Z.); DFG/Germany Colloborative Research Center 963 (C.J.M. and S.D.); DFG/Germany Research Training Group 1351 (L.F.S.); and NSF/USA grant AST-1313075 (M.E.). Study based on observations made with ESO Telescopes at the La Silla Paranal Observatory under programmes 096.C-0082 and 191.C-0505. Observations were obtained with ASH2, which is supported by the Instituto de Astrofísica de Andalucía and Astroimagen. This work makes use of observations from the LCOGT network. We acknowledge the effort of the UVES/M-dwarf and the HARPS/Geneva teams, who obtained a substantial amount of the data used in this work.
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Authors and Affiliations
School of Physics and Astronomy, Queen Mary University of London, 327 Mile End Road, London, E1 4NS, UK
Guillem Anglada-Escudé, Gavin A. L. Coleman, Richard P. Nelson, Sijme-Jan Paardekooper & John P. Strachan
Instituto de Astrofísica de Andalucía – Consejo Superior de Investigaciones Científicas, Glorieta de la Astronomía S/N, Granada, E-18008, Spain
Pedro J. Amado, Zaira M. Berdiñas, Marίa J. López-González, Nicolás Morales, José L. Ortiz, Eloy Rodríguez & Cristina Rodrίguez-López
Department of Physical Sciences, Open University, Walton Hall, Milton Keynes, MK7 6AA, UK
John Barnes
Department of Terrestrial Magnetism, Carnegie Institution of Washington, 5241 Broad Branch Road, NW, 20015, Washington DC, USA
R. Paul Butler
Astroimagen, C. Abad y Lasierra, 58 Bis, Ibiza, 6-2, 07800, Spain
Ignacio de la Cueva
Institut für Astrophysik, Georg-August-Universität Göttingen, Friedrich-Hund-Platz 1, Göttingen, 37077, Germany
Stefan Dreizler, Benjamin Giesers, Sandra V. Jeffers, Christopher J. Marvin, Ansgar Reiners, Luis F. Sarmiento & Mathias Zechmeister
McDonald Observatory, the University of Texas at Austin, 2515 Speedway, C1400, Austin, 78712, Texas, USA
Michael Endl
Departamento de Astronomía, Universidad de Chile, Camino El Observatorio 1515, Las Condes, Santiago, Chile
James S. Jenkins
Centre for Astrophysics Research, Science & Technology Research Institute, University of Hertfordshire, Hatfield, AL10 9AB, UK
Hugh R. A. Jones & Mikko Tuomi
Warsaw University Observatory, Aleje Ujazdowskie 4, Warszawa, Poland
Marcin Kiraga
Max-Planck-Institut für Astronomie, Königstuhl 17, Heidelberg, 69117, Germany
Martin Kürster
Laboratoire Univers et Particules de Montpellier, Université de Montpellier, Place E. Bataillon—CC 72, Montpellier, 34095, Cédex 05, France
Julien Morin
Department of Earth and Planetary Sciences, Weizmann Institute of Science, 234 Herzl Street, Rehovot, 76100, Israel
Aviv Ofir
Astronomisches Rechen-Institut, Mönchhofstrasse 12–14, Heidelberg, 69120, Germany
Yiannis Tsapras
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Contributions
In the author list, after G.A.-E., the authors are listed in alphabetical order. G.A.-E. led the PRD campaign, observing proposals and organized the manuscript. P.J.A. led observing proposals and organized and supported the Instituto de Astrofisica de Andalucía team through research grants. M.T. obtained the early signal detections and most of the Bayesian analyses. J.S.J., J.B., Z.M.B. and H.R.A.J. participated in the analyses and obtained activity measurements. Z.M.B. also led observing proposals. H.R.A.J. funded several co-authors via research grants. M. Kuerster and M.E. provided the extracted UVES spectra, and R.P.B. re-derived radial velocity measurements. C.R.-L. coordinated photometric follow-up campaigns. E.R. led the ASH2 team and related reductions (M.J.L.-G., I.d.l.C., J.L.O. and N.M.). Y.T. led the LCOGT proposals, campaign and reductions. M.Z. obtained observations and performed analyses on HARPS and UVES spectra. A.O. analysed time series and transit searches. J.M., S.V.J. and A.R. analysed stellar activity data. A.R. funded several co-authors via research grants. R.P.N., G.A.L.C., S.-J.P., S.D. and B.G. did dynamical studies and studied the planet formation context. M. Kiraga provided early access to time series from the ASAS survey. C.J.M. and L.F.S. participated in the HARPS campaigns. All authors contributed to the preparation of observing proposals and the manuscript.
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Correspondence toGuillem Anglada-Escudé.
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Extended data figures and tables
Extended Data Figure 1 Window function.
a–c, Window function of the UVES (a), HARPS pre-2016 (b) and HARPS PRD (c) data sets. The same window function applies to the time series of Doppler and activity data. Peaks in the window function are periods at which aliases of infinite period signals would be expected. The green vertical lines mark the period of the planet candidate at 11.2 d.
Extended Data Figure 2 Signal searches on independent radial velocity data sets.
a–c, Likelihood-ratio periodograms searches on the radial velocity (RV) measurements of the UVES (a), HARPS pre-2016 (b) and HARPS PRD (c) subsets. The periodogram with all three sets combined is shown inFig. 1. The black and red lines represent the searches for the first and second signals, respectively. The green vertical lines mark the period of the planet candidate at 11.2 d.
Extended Data Figure 3 Signal searches on the photometry.
a–d, Likelihood-ratio periodograms searches for signals in each photometric ASH2 photometric band (a,b) and LCOGT bands (c,d). The two sinusoid fits to the ASH2 Sii series (P1 = 84 d,P2 = 39.1 d) are used later to construct theFF′ model to test for correlations of the photometry with the radial velocity data. The black, red and blue lines represent the search for the first, second and third signal respectively. The green vertical lines mark the period of the planet candidate at 11.2 d.
Extended Data Figure 4 Signal searches on the width of the spectral lines.
a,b, Likelihood-ratio periodogram searches on the width of the mean spectral line as measured bym2 for the HARPS pre-2016 (a) and HARPS PRD data (b). The signals in the HARPS pre-2016 data are comparable to the photometric period reported in the literature and the variability in the HARPS PRD run compares quite well to the photometric variability. The black, red and blue lines represent the search for the first, second and third signal, respectively. The green vertical lines mark the period of the planet candidate at 11.2 d.
Extended Data Figure 5 Signal searches on the asymmetry of the spectral lines.
a,b, Likelihood-ratio periodogram searches on the line asymmetry as measured bym3 from the HARPS pre-2016 (a) and HARPS PRD (b) data sets. Signal beating at around 1 yr and 0.5 yr is detected in the HARPS pre-2016 data, which is possibly related to instrumental systematic effects or telluric contamination. No signals are detected above the 1% threshold in the HARPS PRD campaign. The black and red lines represent the search for the first and second signals respectively. The green vertical lines mark the period of the planet candidate at 11.2 d.
Extended Data Figure 6 Signal searches on the chromosphericS-index.
a,b, Likelihood-ratio periodogram of theS-index from the HARPS pre-2016 (a) and HARPS PRD (b) campaigns. No signals were detected above the 1% threshold. The green vertical lines mark the period of the planet candidate at 11.2 d.
Extended Data Figure 7 Signal searches on the spectroscopic Hα index.
a–c, Likelihood-ratio periodogram searches of Hα intensity from the UVES (a), HARPS pre-2016 (b) and HARPS PRD (c) campaigns. No signals were detected above the 1% threshold. The green vertical lines mark the period of the planet candidate at 11.2 d.
Extended Data Figure 8 Radial velocities and chromospheric emission during a flare.
a–d, Radial velocities (a) and equivalent width measurements of the Hα (b), Na doublet lines (c) and theS-index (d) as a function of time during a flare that occurred the night of 5 May 2013. The time axis is days sincejd = 245417.0 d. No trace of the flare is observed in the radial velocities. Error bars in the radial velocities correspond to 1σ errors. The formal 1σ errors in the equivalent width measurements are comparable to the size of the points.
Extended Data Figure 9 Probability distributions for the activity coefficients versus the signal amplitude.
a–n, Marginalized posterior densities of the activity coefficients versus the semi-amplitude of the signal for UVES (a), HARPS pre-2016 (b–f), HARPS PRD campaign (g–k) and the photometricFF′ indices for the PRD campaign only (l–n). Each panel shows equiprobability contours containing 50%, 95% and 99% of the probability density around the mean estimate, and the corresponding standard deviation of the marginalized distribution (1σ) in red. The blue bar shows the zero value of each activity coefficient. OnlyCF′ is found to be substantially different from zero.
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This zipped file contains the time-series used in the paper. All time-series are given as plain ASCII/CSV files (columns separated by commas) and follow the same format. See the README file within the zip folder for details. (ZIP 62 kb)
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Anglada-Escudé, G., Amado, P., Barnes, J.et al. A terrestrial planet candidate in a temperate orbit around Proxima Centauri.Nature536, 437–440 (2016). https://doi.org/10.1038/nature19106
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Guillem Anglada
The authors would like to acknowledge useful discussions and quantitative feedback provided by Dr. Javier Pascual Granado and Prof. Rafael Garrido at IAA/CSIC on the mathematical properties of time-series under the section "Methods. Further tests on the signal" during the preparation of the manus cript.


