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Table 3

Transit modeling results.

Kepler ID χ2/ν t0 /BJD-2400000 Porb /d p i a/RS b u 1 u 2 m 1 m 2

5794240 1.01 0.459 0.269
10748390 1.58 0.604 0.130
11391018 1.11 0.600 0.133
5357901 0.99 0.551 0.152
8845026 0.91 - 0.502 0.177
9595827 1.24 0.500 0.178
6849046 1.01 0.496 0.184
9410930 1.02 0.492 0.181
9651668 1.05 0.479 0.186
8359498 1.04 0.479 0.186
7023960 1.01 0.476 0.186
11359879 1.12 0.474 0.189
10619192 1.47 0.474 0.188
11446443 1.00 0.472 0.190
12019440 1.02 0.471 0.188
10874614 1.06 0.471 0.190
7877496 1.06 0.464 0.192
5780885 1.06 0.462 0.202
9631995 1.04 0.459 0.195
11804465 1.08 0.456 0.200
6922244 1.04 0.455 0.203
9818381 1.06 0.450 0.199
10019708 1.01 0.437 0.204
10666592 1.22 0.438 0.199
8191672 1.04 0.433 0.214
9941662 1.15 0.238 0.289

10318874 1.04 0.600 0.133
5084942 1.04 0.578 0.142
12105051 1.03 0.509 0.174
5771719 1.20 0.506 0.184
2571238 1.02 0.496 0.179
11295426 1.09 0.473 0.192
8456679 1.03 0.470 0.190
8554498 1.01 0.468 0.196
8684730 0.80 0.461 0.199
3762468 1.02 0.448 0.199
4349452 0.90 0.449 0.207
3861595 1.06 0.428 0.204

Notes. Errors are 68.3% HPD intervals except for Kepler IDs set in italic. These are enlarged due to red noise contribution. m1 and m2 are predicted LDCs from Claret tables for the specific Teff and log (g) (Tables 1 and 2). Below the horizontal line we present the fit results of our high impact parameter sample.

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