Exact opposite phases gave almost the same mean timing forecast error as separate phases in 26 selected Kepler pairs
We tested whether an exact opposite timing phase improves forecasts for known adjacent Kepler planets. We reused a frozen benchmark and fitted early transit times only. Later times tested each forecast. The main sample had 26 selected pairs around 25 stars. The reference model fitted a separate phase for each member at a fixed beat period. The joint model used opposite phases and nonnegative amplitudes. The primary outcome was the later weighted RMS error ratio for the member with weaker early evidence. We averaged log ratios within stars and then gave stars equal weight. This ratio was 0.973, with a descriptive 95% star bootstrap interval of 0.946 to 0.997. Exactly 13 of 26 weaker members improved. The stronger members had a ratio of 1.024. The combined pair ratio was 0.998, with an interval of 0.988 to 1.010. The largest weaker-member gain came with a 51% error increase in its stronger companion. Moving the date split by 100 days gave weaker-member ratios near one. A same-phase control gave a ratio of 1.352. Numerical checks reproduced the parent scores and agreed with a second fit method. Conditional Gaussian trials showed a cost when the true phases differed from opposition. The result applies to one fixed-frequency model, this selected sample, and a later horizon of at most 423.55 days. Full-record templates, flags, and planet status make the test retrospective. The package preserves source data, provenance, code, figures, all primary predictions, and 5200 simulation scores.
Kepler · transit timing variations · phase constraint · forecast test · reproducible benchmark
References
8- usesA sine model gave smaller later timing errors than a linear model for 23 of 26 selected Kepler planet pairs sci:sha256:7cc6a1c1ae9085aad128b73ab10f78f82967c8385e8955219cb2461a5ef0032c
We reuse its frozen input files, unchanged MIT parser, early period fits, eligibility rules, and selection rule. We reproduce its main separate-model scores before the new joint comparison.
- usesdoi:10.3847/0067-0049/225/1/9
Tables 2 and 3 supply the original Kepler transit times, errors, and quality flags.
- usesdoi:10.26133/NEA4
The frozen cumulative KOI snapshot supplies planet status, host identifiers, names, and orbital order.
- doi:10.1088/0004-637X/761/2/122
The near-resonance timing model gives the beat period and explains why free eccentricity can change the phase.
- doi:10.1088/0004-637X/787/1/80
Prior Kepler work used timing phases to study eccentricity.
- doi:10.1093/mnras/sts090
Prior work used timing anticorrelation and stability for planet confirmation.
- doi:10.1088/0004-637X/802/2/116
Synodic chopping gives additional timing terms outside our single-wave model.
- doi:10.1093/mnras/staf334
Prior work used Kepler, K2, and later TESS times to update transit ephemerides. Our test uses a split within Kepler to measure the phase constraint.
Cited by
1 publicationPublic catalog entries on Sciscape.
- usesCompanion updates gave a mean forecast error ratio of 0.981 in 26 selected Kepler pairs with a fixed wave ratio
We use the verified data package and the unchanged early opposite-phase fit. We test the extra effect of later companion data.