Table 7.

PCE CBP Semimajor Axis and Eccentricity for α_M = 1.0 M_Sun yr⁻¹ and for Primary CE

α_CE	Tides	a_CBP,PCE (au)			e_CBP,PCE			Notes
α_CE	Tides	Mode	Median	Range	Mode	Median	Range	Notes
Kepler-38								[a_CBP,0 = 0.46]
0.5	NTCP	${0.6}_{- 0.01}^{+ 0.2}$	0.8	0.58–1.7	${0.15}_{- 0.07}^{+ 0.12}$	0.26	0.05–0.67	…
0.5^a	TCP	${0.5}_{- 0.01}^{+ 0.4}$	0.6	0.49–0.9	${0.4}_{- 0.35}^{+ 0.01}$	0.2	0.03–0.42	…
1/3/5/10	NTCP	${1.3}_{- 0.2}^{+ 0.1}$	1.3	0.9–3.8	${0.38}_{- 0.01}^{+ 0.16}$	0.42	0.02–0.82	…
1/3/5/10	TCP	${1.4}_{- 0.2}^{+ 0.01}$	1.4	1.1–1.7	${0.46}_{- 0.08}^{+ 0.01}$	0.42	0.28–0.56	…
Kepler-47
0.5, P1^b	NTCP	${0.31}_{- 0.01}^{+ 0.09}$	0.34	0.3–0.44	${0.12}_{- 0.03}^{+ 0.04}$	0.14	0.06–0.27	[a_CBP,0 = 0.29]
0.5, P2^b	NTCP	${0.66}_{- 0.01}^{+ 0.42}$	0.88	0.61–1.67	${0.14}_{- 0.05}^{+ 0.35}$	0.22	0.06–0.56	[a_CBP,0 = 0.70]
0.5, P3^b	NTCP	${0.9}_{- 0.01}^{+ 0.61}$	1.2	0.8–2.87	${0.17}_{- 0.05}^{+ 0.29}$	0.23	0.09–0.66	[a_CBP,0 = 0.96]
0.5^a, P1^b	TCP	${0.32}_{- 0.01}^{+ 0.07}$	0.34	0.31–0.39	${0.1}_{- 0.02}^{+ 0.08}$	0.1	0.07–0.18	…
0.5^a, P2^b	TCP	${0.7}_{- 0.01}^{+ 0.5}$	0.87	0.67–1.24	${0.08}_{- 0.01}^{+ 0.32}$	0.21	0.06–0.42	…
0.5^a, P3^b	TCP	${0.93}_{- 0.01}^{+ 0.91}$	1.18	0.88–1.89	${0.11}_{- 0.01}^{+ 0.35}$	0.22	0.09–0.48	…
1.0, P1^b	NTCP	${0.49}_{- 0.02}^{+ 0.01}$	0.49	0.47–0.5	${0.08}_{- 0.04}^{+ 0.05}$	0.08	0.04–0.13	…
1.0, P2^b	NTCP	${1.33}_{- 0.17}^{+ 0.17}$	1.41	1.12–1.97	${0.42}_{- 0.14}^{+ 0.11}$	0.4	0.22–0.58	…
1.0, P3^b	NTCP	${1.65}_{- 0.01}^{+ 0.53}$	2.13	1.52–4.15	${0.5}_{- 0.14}^{+ 0.18}$	0.51	0.29–0.75	…
1.0^a, P1	TCP	${0.38}_{- 0.01}^{+ 0.03}$	0.39	0.37–0.41	${0.11}_{- 0.1}^{+ 0.01}$	0.07	0.01–0.12	…
1.0^a, P2	TCP	${0.91}_{- 0.01}^{+ 0.29}$	1.03	0.89–1.22	${0.36}_{- 0.21}^{+ 0.01}$	0.26	0.14–0.38	…
1.0^a, P3	TCP	${1.23}_{- 0.01}^{+ 0.47}$	1.46	1.2–1.83	${0.44}_{- 0.26}^{+ 0.01}$	0.32	0.17–0.45	…
3/5/10, P1^d	NTCP	${0.67}_{- 0.01}^{+ 0.01}$	0.67	0.66–0.68	${0.11}_{- 0.01}^{+ 0.03}$	0.11	0.04–0.17	…
3/5/10, P2^d	NTCP	${3.23}_{- 0.01}^{+ 0.57}$	3.4	2.23–7.95	${0.71}_{- 0.06}^{+ 0.1}$	0.73	0.57–0.89	…
3/5/10, P3^d	NTCP	${7.64}_{- 2.71}^{+ 7.21}$	9.97	4.48–22.52	${0.92}_{- 0.02}^{+ 0.02}$	0.89	0.74–0.95^c	46% ejected
3/5/10, P1^d	TCP	${0.69}_{- 0.01}^{+ 0.01}$	0.69	0.68–0.7	${0.1}_{- 0.01}^{+ 0.03}$	0.11	0.08–0.14	…
3/5/10, P2^d	TCP	${3.68}_{- 0.23}^{+ 0.91}$	4.18	3.34–5.62	${0.75}_{- 0.01}^{+ 0.07}$	0.78	0.72–0.83	…
3/5/10, P3^d	TCP	${15.69}_{- 0.01}^{+ 6.16}$	19.7	15.3–23.01	${0.93}_{- 0.01}^{+ 0.02}$	0.94	0.93–0.95^c	81% ejected

Notes. The modes are shown with their respective 68% range. We caution that most of the probability distribution functions (PDFs) are notably nonnormal, often with two dominant peaks at the range limits.

Sinusoidal distributions in phase versus final a_CBP/e_CBP (see, e.g., Figure 5), typically with double-peaked PDFs.

P1/P2/P3 have 40%/15%/75% probability to become dynamically unstable within 1 Myr after the CE phase.

Given the large parameter space and the associated uncertainties, we consider e_CBP > 0.95 as ejection.

P1/P2/P3 have 60%/15%/85% probability to become dynamically unstable within 1 Myr after the CE phase.