_version_ 1866917288892956672
author Fairnington, Tyler R.
Dong, Jiayin
Huang, Chelsea X.
Nabbie, Emma
Zhou, George
Wright, Duncan
Collins, Karen A.
Ciardi, David
Jenkins, Jon M.
Latham, David W.
Ricker, George
Quinn, Samuel N.
Seager, Sara
Shporer, Avi
Vanderspek, Roland
Winn, Joshua N.
Barkaoui, Khalid
Bieryla, Allyson
Buchhave, Lars
Cheryasov, Dmitry
Christiansen, Jessie
Dressing, Courtney
Fukui, Akihiko
Garmash, Alexey
Giacalone, Steven
Hintz, Eric G.
Howell, Steve B.
Isogai, Keisuke
de Leon, Jerome
Lillo-Box, Jorge
Murgas, Felipe
Narita, Norio
Nielsen, Louise D.
Palle, Enric
Rabus, Markus
Rackham, Benjamin V.
Schwarz, Richard P.
Srdoc, Gregor
Stephens, Denise C.
Wang, Gavin
Watanabe, Noriharu
Wilkin, Francis P.
Williams, Joe
author_facet Fairnington, Tyler R.
Dong, Jiayin
Huang, Chelsea X.
Nabbie, Emma
Zhou, George
Wright, Duncan
Collins, Karen A.
Ciardi, David
Jenkins, Jon M.
Latham, David W.
Ricker, George
Quinn, Samuel N.
Seager, Sara
Shporer, Avi
Vanderspek, Roland
Winn, Joshua N.
Barkaoui, Khalid
Bieryla, Allyson
Buchhave, Lars
Cheryasov, Dmitry
Christiansen, Jessie
Dressing, Courtney
Fukui, Akihiko
Garmash, Alexey
Giacalone, Steven
Hintz, Eric G.
Howell, Steve B.
Isogai, Keisuke
de Leon, Jerome
Lillo-Box, Jorge
Murgas, Felipe
Narita, Norio
Nielsen, Louise D.
Palle, Enric
Rabus, Markus
Rackham, Benjamin V.
Schwarz, Richard P.
Srdoc, Gregor
Stephens, Denise C.
Wang, Gavin
Watanabe, Noriharu
Wilkin, Francis P.
Williams, Joe
contents We characterize the radius-dependent eccentricity distribution of 347 warm (P = 8-200 days) systems with only one transiting planetary candidate identified during Sectors 1-69 of the TESS mission. Using the ``photoeccentric effect'' in a hierarchical Bayesian framework, we first model the population using discrete planetary size bins (sub-Neptunes, sub-Saturns, and Jovians). We then develop a continuous mixture model with weights governed by a logistic sigmoid function of radius. We find that the warm-single population is best described by two components: a dominant low-eccentricity mode ( <e_low> = 0.070-0.068+0.026) and a secondary dynamically excited mode (<e_high> = 0.616-0.075+0.091). The fraction of planets belonging to this high-eccentricity component increases strongly with planet radius, characterized by a transition at a break radius of R_br = 9.8-1.1+1.4 R_e. This trend places warm sub-Saturns predominantly on the same low-eccentricity track as sub-Neptunes. In contrast, warm Jovians (8--16 R_e) are frequently eccentric, with 59+-13% of the population in the high eccentricity mode. We detect this bimodality at >4sigma, providing statistically significant evidence that warm gas giants are sculpted by two distinct pathways, or a single mechanism with subsequent eccentricity excitation. Finally, we identify a non-negligible tail of highly eccentric sub-Neptunes (1--4 R_e), which comprise 14.9-6.5+5.1% of the population, consistent with excitation by non-transiting external companions.
format Preprint
id arxiv_https___arxiv_org_abs_2602_20015
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle The Orbital Eccentricity--Radius Distribution for Warm, Single Planets in TESS
Fairnington, Tyler R.
Dong, Jiayin
Huang, Chelsea X.
Nabbie, Emma
Zhou, George
Wright, Duncan
Collins, Karen A.
Ciardi, David
Jenkins, Jon M.
Latham, David W.
Ricker, George
Quinn, Samuel N.
Seager, Sara
Shporer, Avi
Vanderspek, Roland
Winn, Joshua N.
Barkaoui, Khalid
Bieryla, Allyson
Buchhave, Lars
Cheryasov, Dmitry
Christiansen, Jessie
Dressing, Courtney
Fukui, Akihiko
Garmash, Alexey
Giacalone, Steven
Hintz, Eric G.
Howell, Steve B.
Isogai, Keisuke
de Leon, Jerome
Lillo-Box, Jorge
Murgas, Felipe
Narita, Norio
Nielsen, Louise D.
Palle, Enric
Rabus, Markus
Rackham, Benjamin V.
Schwarz, Richard P.
Srdoc, Gregor
Stephens, Denise C.
Wang, Gavin
Watanabe, Noriharu
Wilkin, Francis P.
Williams, Joe
Earth and Planetary Astrophysics
We characterize the radius-dependent eccentricity distribution of 347 warm (P = 8-200 days) systems with only one transiting planetary candidate identified during Sectors 1-69 of the TESS mission. Using the ``photoeccentric effect'' in a hierarchical Bayesian framework, we first model the population using discrete planetary size bins (sub-Neptunes, sub-Saturns, and Jovians). We then develop a continuous mixture model with weights governed by a logistic sigmoid function of radius. We find that the warm-single population is best described by two components: a dominant low-eccentricity mode ( <e_low> = 0.070-0.068+0.026) and a secondary dynamically excited mode (<e_high> = 0.616-0.075+0.091). The fraction of planets belonging to this high-eccentricity component increases strongly with planet radius, characterized by a transition at a break radius of R_br = 9.8-1.1+1.4 R_e. This trend places warm sub-Saturns predominantly on the same low-eccentricity track as sub-Neptunes. In contrast, warm Jovians (8--16 R_e) are frequently eccentric, with 59+-13% of the population in the high eccentricity mode. We detect this bimodality at >4sigma, providing statistically significant evidence that warm gas giants are sculpted by two distinct pathways, or a single mechanism with subsequent eccentricity excitation. Finally, we identify a non-negligible tail of highly eccentric sub-Neptunes (1--4 R_e), which comprise 14.9-6.5+5.1% of the population, consistent with excitation by non-transiting external companions.
title The Orbital Eccentricity--Radius Distribution for Warm, Single Planets in TESS
topic Earth and Planetary Astrophysics
url https://arxiv.org/abs/2602.20015