| Observations |
Status
|
Last Update |
|---|---|---|
Eclipse 1
|
PASS |
2025
05
Aug
|
Visit 7 STIS/G140M
|
FAIL |
2025
08
Aug
|
Visit 8 STIS/G140M
|
PASS |
2025
05
Aug
|
Eclipse 2
|
PASS |
2025
05
Aug
|
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Because of uncertainties in orbital parameters, the timing of secondary eclipses can be off by minutes to hours. Instead of covering wide time windows for every eclipse—which is inefficient—we use a two-checkpoint strategy to optimize observations:
After a small number of eclipses (enough to detect an eclipse assuming a bare-rock planet, which produces one of the deepest possible signals), we evaluate the data under the first checkpoint.
After more eclipses, we arrive at a second checkpoint.
This adaptive strategy ensures efficient use of telescope time while maintaining scientific rigor.
Conservative Noise Model
Initial eclipse count estimates were based on JWST ETC noise predictions, which are optimistic and do not fully account for real-world correlated noise.
We now apply a 1.25 × multiplier to ETC noise estimates, based on empirical results from Cycles 1-3. This ensures more realistic eclipse depth predictions and often increases the number of required eclipses.
Model Comparison: Bare Rock vs. CO₂ Atmosphere
Earlier strategies took a conservative view, comparing a high-temperature bare-rock planet with a generic atmosphere capable of redistributing heat.
With JWST/MIRI 15 μm photometry, we are most sensitive to CO₂-rich atmospheres, so we now directly compare the bare-rock case to the CO₂-rich case. This physically motivated model comparison often reduces the number of eclipses needed to distinguish between scenarios.
Pre-slewing Experiment
Fortune et al. (2025)
reported tentative evidence that the amplitude of the time-
series detector settling ramp (∼30-60 min) at 15 µm shows a somewhat repeatable and
small amplitude when the filter wheel is in the MIRI LRS P750L position
prior to swapping to the F1500W (15 µm) MIRI filter.
The setup of the pre-slew experiment is as follows:
1 finish previous visit, 2 setup instrument, wait for earliest start time, 3 slew to RW target, acquire guide star, 4 acquire target and perform science observations.
Other factors that may affect the settling slope are the stellar magnitude itself as explained in Connors et al. (2025)
We note that including the pre-slewing filter adds an additional 229 seconds to our observations.