2025PASP..137i4503R


Query : 2025PASP..137i4503R

2025PASP..137i4503R - Publ. Astron. Soc. Pac., 137, part no 9, 4503 (2025/September-0)

The Rayleigh Criterion: Resolution Limits of Astronomical Periodograms.

RAMIREZ DELGADO V., CAICEDO VIVAS J.S., DODSON-ROBINSON S. and HALEY C.

Abstract (from CDS):

The Rayleigh criterion determines the resolution limit of a periodogram, which is the minimum frequency separation required to barely resolve two sinusoids. Failing to consider the Rayleigh criterion may result in incorrect interpretations of long-period signals or spurious claims that two closely spaced periodogram peaks represent two distinct physical processes. Resolution considerations can help astronomers decide which periodogram peaks truly represent oscillatory signals, a question that is of great importance for exoplanet detection. We demonstrate how applying the Rayleigh criterion can help observers avoid false positive detections caused by uneven observing cadence or insufficient observing time baseline. We present three synthetic data sets that showcase the importance of the Rayleigh criterion in interpreting the generalized Lomb-Scargle and Bayesian periodograms. Our synthetic data sets illustrate (1) a single oscillation with a split Lomb-Scargle periodogram peak resulting from uneven observing cadence can be mistaken for two oscillations if the Rayleigh criterion is neglected, (2) oversampling a periodogram's frequency grid does not improve resolution, and (3) observing time baseline requirements for resolving two closely spaced oscillations. We use the Rayleigh criterion to revisit detections of planets, stellar activity, and differential rotation from four published data sets. We show that the frequency separation between planet 55 Cnc d and the activity cycle is too small to distinguish the two phenomena based on published radial velocities (RVs) alone. Likewise, the contested 4970 days planet orbiting HD 99492 cannot be statistically separated from zero frequency. We determine that a cubic polynomial better explains the long-term RV variability of Barnard's star than a sinusoid model. Finally, our re-analysis of Kepler observations of two active stars shows that the signals previously attributed to differential rotation can be modeled by a Gaussian process with a single quasiperiodicity. This work demonstrates the importance of considering Rayleigh resolution when constructing a time-domain model.

Abstract Copyright: © 2025. The Astronomical Society of the Pacific. All rights, including for text and data mining, AI training, and similar technologies, are reserved.

Journal keyword(s): Exoplanet detection methods - Light curves - Period search - Lomb-Scargle periodogram - Time series analysis

Simbad objects: 31

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Number of rows : 31
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 * eps Eri BY* 03 32 55.8444911587 -09 27 29.739493865 5.19 4.61 3.73 3.00 2.54 K2V 2073 1
2 CoRoT-7b Pl 06 43 49.4690164104 -01 03 46.826642700           ~ 422 1
3 CoRoT-7c Pl 06 43 49.4690164104 -01 03 46.826642700           ~ 50 1
4 HD 50499c Pl 06 52 02.0241958872 -33 54 56.019365496           ~ 10 0
5 HD 50499 PM* 06 52 02.0241958872 -33 54 56.019365496   7.82 7.20     G0/2V 131 1
6 * rho01 Cnc c Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 154 1
7 * rho01 Cnc e Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 682 1
8 * rho01 Cnc f Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 72 1
9 * rho01 Cnc d Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 163 1
10 * rho01 Cnc b Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 267 1
11 * rho01 Cnc PM* 08 52 35.8111044043 +28 19 50.954994470 7.45 6.82   5.4   K0IV-V 1223 1
12 HD 89744 PM* 10 22 10.5618854376 +41 13 46.309698444   6.25 5.72     F7V 360 1
13 HD 89744c Pl? 10 22 10.5618854376 +41 13 46.309698444           ~ 8 0
14 HD 92788 PM* 10 42 48.5278074048 -02 11 01.525313004   8.01 7.30     G6V 260 1
15 HD 92788c Pl 10 42 48.5278074048 -02 11 01.525313004           ~ 11 0
16 * 47 UMa d Pl 10 59 27.9727514012 +40 25 48.920572724           ~ 33 1
17 * 47 UMa PM* 10 59 27.9727514012 +40 25 48.920572724   5.66   4.7   G1-VFe-0.5 824 1
18 * 83 Leo A PM* 11 26 45.3217299671 +03 00 47.156637705 7.78 7.28 6.46 6.0   G9IV-V 259 0
19 * 83 Leo Bb Pl 11 26 46.2783265113 +03 00 22.756723728           ~ 45 1
20 * 83 Leo B PM* 11 26 46.2783265113 +03 00 22.756723728 9.467 8.554 7.530 6.97 6.508 K3 226 1
21 * 83 Leo Bc Pl 11 26 46.2783265113 +03 00 22.756723728           ~ 13 1
22 HD 120066 PM* 13 46 57.1225636378 +06 21 01.346102072   6.96   5.9   G0V 168 0
23 NAME Barnard's star BY* 17 57 48.4984700685 +04 41 36.113879676 12.497 11.24 9.511 8.298 6.741 M4V 907 2
24 NAME Barnard's Star c Pl 17 57 48.4984700685 +04 41 36.113879676           ~ 3 0
25 NAME Barnard's Star d Pl 17 57 48.4984700685 +04 41 36.113879676           ~ 3 0
26 NAME Barnard's Star e Pl 17 57 48.4984700685 +04 41 36.113879676           ~ 3 0
27 NAME Barnard's Star b Pl 17 57 48.4984700685 +04 41 36.113879676           ~ 34 0
28 2MASS J19234997+3641118 * 19 23 49.9684285608 +36 41 11.822562240           ~ 9 0
29 2MASS J19270897+3723411 * 19 27 08.9766541560 +37 23 41.111976192           ~ 10 0
30 HD 213472 PM* 22 30 49.9737483912 +40 43 19.400636388       7.8   G5 58 0
31 HD 213472b Pl 22 30 49.9737483912 +40 43 19.400636388           ~ 3 0

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