Barnard’s star is a red dwarf, and has the largest proper motion (apparent motion across the sky) of all known stars. At a distance of 1.8 parsecs1, it is the closest single star to the Sun; only the three stars in the α Centauri system are closer. Barnard’s star is also among the least magnetically active red dwarfs known2,3 and has an estimated age older than the Solar System. Its properties make it a prime target for planetary searches; various techniques with different sensitivity limits have been used previously, including radial-velocity imaging4,5,6, astrometry7,8 and direct imaging9, but all ultimately led to negative or null results. Here we combine numerous measurements from high-precision radial-velocity instruments, revealing the presence of a low-amplitude periodic signal with a period of 233 days. Independent photometric and spectroscopic monitoring, as well as an analysis of instrumental systematic effects, suggest that this signal is best explained as arising from a planetary companion. The candidate planet around Barnard’s star is a cold super-Earth, with a minimum mass of 3.2 times that of Earth, orbiting near its snow line (the minimum distance from the star at which volatile compounds could condense). The combination of all radial-velocity datasets spanning 20 years of measurements additionally reveals a long-term modulation that could arise from a stellar magnetic-activity cycle or from a more distant planetary object. Because of its proximity to the Sun, the candidate planet has a maximum angular separation of 220 milliarcseconds from Barnard’s star, making it an excellent target for direct imaging and astrometric observations in the future.
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The public high-resolution spectroscopic raw data used in the study can be freely downloaded from the corresponding facility archives: HIRES, http://koa.ipac.caltech.edu; UVES, HARPSpre and HARPSpost, http://archive.eso.org; HARPS-N, http://archives.ia2.inaf.it/tng; APF, https://mthamilton.ucolick.org/data). Proprietary raw data are available from the corresponding author on reasonable request. The nightly averaged, fully calibrated radial velocities, spectroscopic indices and photometric measurements are available as Supplementary Data.
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The results are based on observations made with the CARMENES instrument at the 3.5-m telescope of the Centro Astronómico Hispano-Alemán de Calar Alto (CAHA, Almería, Spain), funded by the German Max-Planck-Gesellschaft (MPG), the Spanish Consejo Superior de Investigaciones Científicas (CSIC), the European Union and the CARMENES Consortium members; the 90-cm telescope at the Sierra Nevada Observatory (Granada, Spain) and the 40-cm robotic telescope at the SPACEOBS observatory (San Pedro de Atacama, Chile), both operated by the Instituto de Astrofísica de Andalucía (IAA); and the 80-cm Joan Oró Telescope (TJO) of the Montsec Astronomical Observatory (OAdM), owned by the Generalitat de Catalunya and operated by the Institute of Space Studies of Catalonia (IEEC). This research was supported by the following institutions, grants and fellowships: Spanish MINECO ESP2016-80435-C2-1-R, ESP2016-80435-C2-2-R, AYA2016-79425-C3-1-P, AYA2016-79245-C3-2-P, AYA2016-79425-C3-3-P, AYA2015-69350-C3-2-P, ESP2014-54362-P, AYA2014-56359-P, RYC-2013-14875; Generalitat de Catalunya/CERCA programme; Fondo Europeo de Desarrollo Regional (FEDER); German Science Foundation (DFG) Research Unit FOR2544, project JE 701/3-1; STFC Consolidated Grants ST/P000584/1, ST/P000592/1, ST/M001008/1; NSF AST-0307493; Queen Mary University of London Scholarship; Perren foundation grant; CONICYT-FONDECYT 1161218, 3180405; Swiss National Science Foundation (SNSF); Koshland Foundation and McDonald-Leapman grant; and NASA Hubble Fellowship grant HST-HF2-51399.001. J.T. is a Hubble Fellow.
Nature thanks I. Snellen and the other anonymous reviewer(s) for their contribution to the peer review of this work.
The authors declare no competing interests.
Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Extended data figures and tables
a, Magnitude of the window function |w| of the combined datasets. b–d, Likelihood periodogram of the radial-velocity measurements considering the first signal search (b), the residuals after modelling a long-period (6,600 days) signal (c) and the residuals after modelling long-period and 233-day periodicities (d). No high-significance signals remain in d, in particular in the 10–40-day region, corresponding to the conservative habitable zone. The region below 10 days is not shown for clarity, but it is also devoid of significant periodic signals down to the Nyquist frequency of the dataset (2 days). Two different scales for the horizontal axis are used to improve the visibility of the low-frequency range. The red dotted line marks the 0.1% FAP threshold.
The top panel shows the PSD56 of a stacked periodogram57,58 and the bottom panel depicts a cumulative measurement of the semi-amplitude K of the signal, with the grey lines showing 1σ error bars. The horizontal red dotted line, green dashed line and blue solid lines show the 10%, 1% and 0.1% FAP thresholds. The evolution of the significance is stable with time and the variations in the amplitude over the last nine years of observations are smaller than 5% of the measured amplitude. The steady increase in signal significance and the stable amplitude are both consistent with the expected evolution of the evidence for a signal of Keplerian origin.
a, Spurious radial-velocity effect ΔRV that would be caused by offsets with respect to the catalogue coordinates (black and red) and proper motions (green and blue). b, Illustration of the radial-velocity effect caused by an offset in the parallax with respect to the catalogue value. The uncertainties of the astrometric parameters for Barnard’s star from the Hipparcos catalogue were used in the barycentric corrections, and are approximately 10 times smaller than the values used in this plot (15 mas in position, 1.5 mas yr−1 in proper motion and 1.5 mas in parallax), implying that catalogue errors introduce undetectable signals.
Blue squares represent the improvement in the log-likelihood using a Gaussian process to model the correlated noise when trying to detect a first signal. The same procedure is applied to simulated observations generated with white noise and a sinusoidal signal consistent with the parameters of the candidate planet (red circles). Even in absence of true correlated noise, the Gaussian process absorbs a substantial amount of significance (ΔlnL ≈ 30 for this selection of kernel parameters). The adopted kernel is a damped SHO, with a damping timescale of τ = Plife = 100 days, and each point corresponds to different values for the oscillator frequency ν (x axis). The PSD of an SHO kernel with ν = 140−1 d−1 and τ = 100 days is depicted as a black line. The greatest reduction in significance occurs when the trial frequency approaches that of the oscillator, but this reduction in significance extends out to a broad range of frequencies, therefore acting as a filter. The period of the candidate planet is marked with a vertical dashed line, and the likely rotation period derived from stellar activity is marked with a vertical dotted line.
Extended Data Fig. 5 Distribution of empirical false alarms from synthetic observations with correlated noise.
These simulations were obtained by generating synthetic observations following kernels derived from the observations, and then fitted to moving-average models. The resulting distribution of false alarms shows a clear excess around the measured rotation period of the star (vertical dashed blue line) and at low frequencies (long periods), owing to the use of the free offsets in the model (left of the rotation period). The empirical FAP was computed by counting the number of false alarms in the interval ΔlnL ∈ [32, ∞) and frequency ∈ [0, 1/230] (left of the green line and above the red line) and dividing by total number of false alarms in the same frequency interval (left of the green line). Empirical FAP thresholds of 10%, 1% and 0.1% are shown for reference. The candidate signal under discussion is shown as a red square and has an empirical FAP of about 0.8%. The orange histogram at the bottom shows the distribution of false alarms in frequency (arbitrary normalization).
This file contains Supplementary Data 1: Time-series measurements of radial velocity. Individual files for each of the instruments used (APF, CARMENES, HARPSN, HARPSpost, HARPSpre, HIRES, PFS, UVES) are provided in plain ASCII format with space delimiters arranged in three columns with headers: • Column 1: Barycentric Julian Date of the mid-time of the observation (BJD) • Column 2: Radial velocity (RV) in units of m s-1 • Column 3: 1-sigma uncertainty in the radial velocity (sigma_RV) in units of m s-1
This file contains Supplementary Data 2: Time-series measurements of the Hα index. Individual files for each of the instruments used (APF, CARMENES, HARPSN, HARPSpost, HARPSpre, HIRES, PFS, UVES) are provided in plain ASCII format with space delimiters arranged in three columns with headers: • Column 1:Barycentric Julian Date of the mid-time of the observation (BJD) • Column 2:Hα index (Halphindex; dimensionless) • Column 3: 1-sigma uncertainty in the Hα index (sigma_Halpindex; dimensionless)
This file contains Supplementary Data 3: Time-series measurement of the S index of the Ca II H&K chromospheric lines. Individual files for each of the instruments with coverage in the relevant wavelength range (APF, HARPSN, HARPSpost, HARPSpre, HIRES) are provided in plain ASCII format with space delimiters arranged in three columns with headers: • Column 1: Barycentric Julian Date of the mid-time of the observation (BJD) • Column 2: S index (Sindex; dimensionless) • Column 3: 1-sigma uncertainty in the S index (sigma_Sindex; dimensionless)
This file contains Supplementary Data 4: Time-series photometric measurements. Individual files for each of the instruments used (AAVSO, APT, ASAS, MEarth, OAdM, RCT, SNO) are provided in plain ASCII format with space delimiters arranged in three columns with headers: • Column 1: Barycentric Julian Date of the mid-time of the observation (BJD) • Column 2: Differential magnitude (Delta_mag) • Column 3: 1-sigma uncertainty in the differential magnitudes (sigma_Deltamag). The photometric filters used are: AAVSO: Johnson V; APT: Johnson V; ASAS: Johnson V; MEarth: RG715nm; OAdM: Cousins R; RCT: Johnson V; SNO: Johnson V
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Ribas, I., Tuomi, M., Reiners, A. et al. A candidate super-Earth planet orbiting near the snow line of Barnard’s star. Nature 563, 365–368 (2018). https://doi.org/10.1038/s41586-018-0677-y
- Planet Candidates
- Long-term Modulation
- Stellar Rotation Period
- American Association Of Variable Star Observers (AAVSO)
- Zero-point Offsets
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