FAQ - PLATO
FAQ
This section provides a summary of Frequently Asked Questions (FAQ) and their respective answers. Clicking on any of the questions below allows readers to expand and collapse the relevant entries.
CfP Update
- Proposing observations (within 120 arcsec) of Prime sample targets do not pass the CfP checks in any configuration.
- Proposing observations (within 108 arcsec) of the P1 sample may pass the CfP checks if requesting F-CAMs. However, any such requests continue to also be flagged to the SOC. This will allow the associated science case to be checked by the SOC and, if necessary, by the TAC.
- Proposing observations (within 108 arcsec) of the P4/P5 sample may pass the CfP checks if requesting N-CAMs imagettes or F-CAMs. However, any such requests continue to also be flagged to the SOC. This will allow the associated science case to be checked by the SOC and, if necessary, by the TAC.
- Proposing observations (within 108 arcsec) of the fgPIC sample (excluding scvPIC targets) may pass the CfP checks if requesting N-CAMs imagettes or light curves. However, any such requests continue to also be flagged to the SOC to check for compliance with the duplication policy.
- Proposing observations (within 108 arcsec) of the scvPIC sample is allowed if the user requests N-CAMs imagettes or F-CAMs. However, any such requests continue to also be flagged to the SOC to check for compliance with the duplication policy.
- Prevent the observation of Prime Sample targets as required by the Science Management Plan.
- Avoid duplication with other PIC observations readily providing public data.
- Serve as general instruction to prevent blending with PIC targets in most cases, which would compromise on-board light curve extraction and scientific value. This general instruction is necessary as it is not operationally feasible for the SOC to evaluate blended targets one-by-one at the level of detail of arcsecs vs. magnitudes for all proposals received.
- Ensure operational efficiency through a set of clear, consistently applicable rules.
Policy Questions
Technical Questions
| PROCESSING TYPE | PRODUCTS |
|---|---|
| F_IMA | imagette |
| S_FX/L_FX | short- or long-cadence flux using nominal mask |
| S_FX_DFX/L_FX_DFX | as S_FX/L_FX, plus the difference in flux between the extended and nominal masks |
| S_FX_NCOB/L_FX_NCOB | as S_FX/L_FX, plus the corresponding centroids |
| S_FX_DFX_NCOB_ECOB/L_FX_DFX_NCOB_ECOB | as S_FX_DFX/L_FX_DFX, plus the centroids corresponding to the nominal and extended masks |
- 1 quarter = 3 months = 90 days
- 3 quarters = 9 months = 270 days
- 2 years = 8 quarters = 24 months = 720 days
Recent work by the mission team (e.g. Cabrera et al., 2026) notes that model uncertainties increase significantly beyond Pmag ≳ 17. Simulations presented in Jannsen et al. (in preparation; see our "recipes" webpage) explore targets as faint as Pmag ≈ 19, but the noise predictions at these levels are highly uncertain. That study suggests that Pmag ≈ 18–19 may represent PLATO’s ultimate detection limit, though all results at this faint end should be treated with caution.
In summary, while detections of a full loss-of-light or a drastic brightness increase due to a long superflare may be possible down to Pmag ≈ 18–19 in idealised cases (and likely requiring imagette stacking), robust science is more realistically expected for targets brighter than Pmag ≈ 17, depending on the observing strategy and science requirements. Observations of faint sources will also likely require using imagettes, where temporal stacking can be applied if high time or spatial resolution is not required. In some cases, such an approach may make it possible to push to Pmag ≈ 18 mag or even fainter. By contrast, on board photometry is less well suited for very faint sources. It relies on pixel summation over a mask, basic on board processing, and time averaging over 50 s or 600 s, with additional outlier rejection. If a faint source intermittently disappears, this may trigger outlier rejection, making on board photometry unreliable for such targets.
On another note: if your target is brighter than Pmag=17, and the light disappears during the transit leaving only mainly instrumental noise, there may be a problem when subtracting the background by resulting in, for example, fluxes with negative values. These errors in the background correction will be flagged in the light curve. Therefore, it is also recommended here to use imagettes to ensure a proper light curve derivation.