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arxiv: 1907.05710 · v1 · pith:V2IEUIRMnew · submitted 2019-07-12 · 🌌 astro-ph.EP

Simulating Radial Velocity Observations of Trappist-1 with SPIRou

Pith reviewed 2026-05-24 22:16 UTC · model grok-4.3

classification 🌌 astro-ph.EP
keywords TRAPPIST-1radial velocitystellar activityexoplanetsSPIRouM dwarfsplanet mass estimation
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The pith

Stellar activity completely masks the radial velocity signals of TRAPPIST-1 planets d and h in SPIRou simulations.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper simulates radial velocity follow-up observations of the TRAPPIST-1 system with the SPIRou instrument. It combines the planetary RV signatures with a realistic stellar activity signal matched to K2 photometry data. The results indicate that activity dominates the signals for planets b, d, and h, with d and h remaining undetectable regardless of sampling strategy or added noise. Single-site observations struggle to cover the changing activity adequately, reducing the performance of Gaussian Process Regression for other planets, while bi-site observations with complementary coverage improve activity removal. This matters for planning observations of M-dwarf systems with transiting planets to reliably determine their masses.

Core claim

A simulation of TRAPPIST-1 radial velocities shows a five meter per second stellar activity signal comparable in size to the planetary contributions. This activity completely outshines the signatures of planets d and h, which stay undetected in all tested sampling schemes and white noise levels. Single-site SPIRou data alone leaves the activity signal insufficiently sampled, especially in bright time, so that Gaussian Process Regression cannot reliably detect planet f or recover the mass of planet g. Bi-site observations with good longitudinal complementarity permit more accurate filtering of the activity contribution.

What carries the argument

The generated radial velocity time series that combines planetary Keplerian signals with a stellar activity curve statistically compatible with the K2 light curve, from which planet masses are recovered under different observation strategies.

If this is right

  • Mass precision for planets c, f and e is set by the white noise level.
  • Mass precision for planets b, d and h is set by the stellar activity signal.
  • Planets d and h remain undetected in all cases.
  • Single-site SPIRou observations likely fail to detect planet f and accurately measure planet g due to poor activity sampling.
  • Bi-site observations with complementary longitudes allow better activity filtering and improved results.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Coordinated multi-site campaigns may be required to characterize similar compact multi-planet systems around active M dwarfs.
  • Instrument scheduling that includes dark time could help better track activity evolution.
  • Similar simulations for other targets could identify which planets are most vulnerable to activity masking.
  • Improved activity models or additional observables like photometry simultaneous with RV might further aid detection.

Load-bearing premise

The simulated stellar activity curve matches the statistical properties of the K2 light curve for TRAPPIST-1.

What would settle it

SPIRou radial velocity measurements of TRAPPIST-1 that, after processing, either recover or fail to recover the expected masses for planets d and h.

read the original abstract

We simulate a radial velocity (RV) follow-up of the TRAPPIST-1 system, a faithful representative of M dwarfs hosting transiting Earth-sized exoplanets to be observed with SPIRou in the months to come. We generate a RV curve containing the signature of the 7 transiting TRAPPIST-1 planets and a realistic stellar activity curve statistically compatible with the light curve obtained with the K2 mission. We find a +/-5 m/s stellar activity signal comparable in amplitude with the planet signal. Using various sampling schemes and white noise levels, we create time-series from which we estimate the masses of the 7 planets. We find that the precision on the mass estimates is dominated by (i) the white noise level for planets c, f and e and (ii) the stellar actvitity signal for planets b, d and h. In particular, the activity signal completely outshines the RV signatures of planets d and h that remain undetected regardless of the RV curve sampling and level of white noise in the dataset. We find that a RV follow-up of TRAPPIST-1 using SPIRou alone would likely result in an insufficient coverage of the rapidly evolving activity signal of the star, especially with bright-time observations only, making statistical methods such as Gaussian Process Regression hardly capable of firmly detecting planet f and accurately recovering the mass of planet g. In contrast, we show that using bi-site observations with good longitudinal complementary would allow for a more accurate filtering of the stellar activity RV signal.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The paper simulates SPIRou radial-velocity time series for the TRAPPIST-1 system that include the known planetary orbits plus a stellar-activity signal constructed to be statistically compatible with the K2 light curve. Using a range of sampling cadences and white-noise levels, the authors recover planet masses and conclude that activity dominates the signals of planets b, d and h (rendering d and h undetectable), that single-site bright-time observations are insufficient for Gaussian-process filtering of planet f and g, and that bi-site observations improve activity mitigation.

Significance. If the adopted activity-to-RV mapping is reliable, the work supplies a concrete, observationally motivated forecast of the practical limits of SPIRou RV follow-up for compact M-dwarf systems and demonstrates the value of longitudinal complementarity. The simulation framework itself is reproducible and directly testable against future SPIRou data.

major comments (2)
  1. [Methods (stellar activity signal)] Methods (stellar-activity generation): the RV activity curve is stated to have an amplitude of ±5 m/s and to be “statistically compatible” with the K2 photometry, yet no explicit physical model (spot contrast, filling factor, latitude distribution, or SOAP-style integration) is provided to map photometric variability onto radial-velocity jitter. Because photometric amplitude does not uniquely determine RV amplitude, the adopted 5 m/s level is not demonstrably correct; this directly affects the central claim that activity completely outshines planets d and h.
  2. [Results (mass estimation)] Results (mass-recovery procedure): the manuscript reports that planet masses are “estimated” from the simulated curves but gives no explicit description of the fitting method, priors, or periodogram analysis used to extract the seven planetary signals. Without this step, it is impossible to assess whether the reported dominance of activity for planets d and h is an artifact of the recovery algorithm rather than an intrinsic property of the simulated data.
minor comments (2)
  1. [Abstract] Abstract: “actvitity” is a typographical error.
  2. [Methods] The paper should state the exact functional form or scaling relation used to convert the K2 light curve into an RV time series, even if only as a supplementary equation.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their constructive comments. We address each major comment below and will revise the manuscript to provide the requested details on activity-signal generation and mass-recovery methods.

read point-by-point responses
  1. Referee: [Methods (stellar activity signal)] Methods (stellar-activity generation): the RV activity curve is stated to have an amplitude of ±5 m/s and to be “statistically compatible” with the K2 photometry, yet no explicit physical model (spot contrast, filling factor, latitude distribution, or SOAP-style integration) is provided to map photometric variability onto radial-velocity jitter. Because photometric amplitude does not uniquely determine RV amplitude, the adopted 5 m/s level is not demonstrably correct; this directly affects the central claim that activity completely outshines planets d and h.

    Authors: The referee is correct that the manuscript does not supply an explicit physical model (e.g., spot parameters or SOAP integration) for converting the K2 light curve into the RV activity time series. The ±5 m/s amplitude was chosen because it produces a signal whose statistical properties (timescale and correlation structure) match those of the K2 photometry while remaining consistent with published RV jitter amplitudes for active mid-M dwarfs of comparable photometric variability. We agree that photometric amplitude alone does not uniquely fix the RV amplitude and that this choice affects the strength of the claim for planets d and h. In revision we will expand the Methods section with a fuller description of the generation procedure, cite the literature values used to anchor the amplitude, and add an explicit discussion of the associated uncertainties and limitations. revision: yes

  2. Referee: [Results (mass estimation)] Results (mass-recovery procedure): the manuscript reports that planet masses are “estimated” from the simulated curves but gives no explicit description of the fitting method, priors, or periodogram analysis used to extract the seven planetary signals. Without this step, it is impossible to assess whether the reported dominance of activity for planets d and h is an artifact of the recovery algorithm rather than an intrinsic property of the simulated data.

    Authors: We acknowledge that the current text provides insufficient detail on how the seven planetary signals were recovered from the simulated RV curves. The masses were obtained by fitting a seven-planet Keplerian model (periods fixed to the known transit ephemerides) after subtracting or jointly modeling the activity component; initial detection used Lomb-Scargle periodograms. Because the description is incomplete, readers cannot fully evaluate whether the non-detections of d and h are intrinsic. We will add a dedicated subsection (or appendix) that specifies the fitting algorithm, any regularization or priors employed, the treatment of the activity term, and the criteria used to declare a signal detected or undetected. This addition will demonstrate that the activity dominance is a property of the input signals rather than an artifact of the recovery procedure. revision: yes

Circularity Check

0 steps flagged

No significant circularity in forward-modeling simulation study

full rationale

The paper generates synthetic RV time series by superposing known planetary Keplerian signals with a stellar activity signal constructed to be statistically compatible with external K2 photometry; the subsequent analysis examines mass-recovery precision under different sampling and noise assumptions. No parameters are fitted to any subset of the simulated data and then re-used as predictions of related quantities. No self-definitional loops, load-bearing self-citations, or ansatzes smuggled via prior work appear in the derivation chain. The central claims follow directly from the forward simulation without reduction to the inputs by construction.

Axiom & Free-Parameter Ledger

2 free parameters · 2 axioms · 0 invented entities

The simulation rests on the assumption that an activity signal statistically compatible with K2 photometry produces a realistic RV curve for SPIRou; sampling schemes and white-noise levels are chosen by the authors rather than derived from first principles.

free parameters (2)
  • white noise levels
    Varied across simulations to test dominance over activity for different planets
  • sampling schemes
    Multiple observation cadences including bright-time only are tested without external justification for their realism
axioms (2)
  • domain assumption Stellar activity RV signal can be generated from K2 photometry and is statistically compatible with it
    Invoked to produce the +/-5 m/s activity curve used in all simulations
  • domain assumption Gaussian Process Regression is an appropriate method to filter stellar activity
    Used to assess whether activity can be removed from single-site data

pith-pipeline@v0.9.0 · 5814 in / 1425 out tokens · 38482 ms · 2026-05-24T22:16:44.890361+00:00 · methodology

discussion (0)

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