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Detection of four cold Jupiters through combined analyses of radial velocity and astrometry data

Published 16 Jan 2026 in astro-ph.EP | (2601.11280v1)

Abstract: Cold Jupiters play a crucial role in planet formation and dynamical evolution. Since their initial discovery around 47 UMa, they have attracted significant interest, yet their formation mechanisms remain uncertain, underscoring the need to expand the known population. In this work, we combine RV data with Gaia astrometry using Hipparcos-Gaia proper-motion anomalies over a 25-year baseline. By jointly modeling both datasets with the MCMC framework, we constrain planetary masses, orbital inclinations, and three-dimensional orbital architectures. This reduces RV degeneracies and improves mass determinations. Four cold Jupiters are reported: HD 68475 b and HD 100508 b are each the first confirmed planet in their systems, with orbital periods $7832_{-323}{+463}$ d and $5681\pm42$ d and dynamical masses of $5.16_{-0.47}{+0.53} M_{\text{Jup}}$ and $1.2_{-0.18}{+0.30} M_{\text{Jup}}$, respectively. In multi-planet systems, HD 48265 c has a period of $10418_{-1400}{+2400}$ d and a mass of $3.71_{-0.43}{+0.68} M_{\text{Jup}}$, while HD 114386 c orbits at $444.00_{-0.88}{+0.93}$ d with a minimum mass of $0.37 \pm 0.03 M_{\text{Jup}}$. The two planets in the HD 48265 system may exhibit a significant mutual inclination, making it a target for testing the von-Zeipel-Kozai-Lidov mechanism. HD 68475 b is a promising candidate for future direct imaging with ELT/METIS. We identified a Jupiter analog with the longest known orbital period among planets with masses between 0.5 and 2 $M_{\text{Jup}}$, implying that a substantial population of cold Jupiters likely awaits discovery by Gaia. This study expands the sample of cold Jupiters with constrained orbits and dynamical masses, demonstrating the value of combining radial velocity and astrometry in exoplanet research.

Summary

  • The paper presents robust dynamical mass measurements and full three-dimensional orbital solutions for four cold Jupiters.
  • It employs a novel combination of multi-instrument radial velocity data and long-baseline astrometry to break the Mp sin i degeneracy.
  • The findings reveal diverse planetary architectures, including high eccentricities and significant mutual inclinations that inform planet formation models.

Detection and Characterization of Four Cold Jupiters via Combined Radial Velocity and Astrometric Constraints

Introduction

The architecture and dynamical evolution of cold Jupiter-mass exoplanets provide key empirical constraints on planet formation, migration mechanisms, and long-term system stability. The principal limitation of the radial velocity (RV) technique—obtaining only the product MpsiniM_p\sin i—precludes true mass and three-dimensional orbital orientation inference for most known giant planets, especially those on long-period orbits. This paper reports a systematic effort to overcome the MpsiniM_p\sin i degeneracy by jointly fitting multi-instrument RV data and time-resolved astrometry from both Hipparcos and multi-epoch Gaia data releases, leveraging a \sim25-year baseline to robustly detect and characterize four cold Jupiters in diverse stellar environments (2601.11280).

Methodology and Data Synthesis

The analysis is built on heterogeneous, high-cadence RV observations from major spectrographs (CORALIE, HARPS, MIKE, PFS) and astrometric constraints using Hipparcos, Gaia DR2, and DR3 catalog measurements, including barycentric motion and proper-motion anomalies. Orbital parameters are constrained via state-of-the-art parallel-tempered MCMC sampling, marginalizing over instrumental zero-point offsets and stellar jitter. For each system, non-linear three-dimensional orbital motion is modeled, and companion masses, inclinations, and nodal longitudes are directly extracted. Cross-validation with activity indicators (GLS periodograms, Pearson correlation analysis) demonstrates RV coherence with planetary, not stellar, origins.

Results for Individual Systems

HD 48265: Mutual Inclination and High-Eccentricity Dynamics

The HD 48265 system is shown to host two massive planets: HD 48265 b (P=790P=790 d, Mb=7.43.9+3.7MJupM_b = 7.4^{+3.7}_{-3.9}\,M_{\mathrm{Jup}}, highly uncertain astrometric inclination) and the newly characterized HD 48265 c (P=28.53.9+6.7P=28.5^{+6.7}_{-3.9} yr, Mc=4.450.37+0.75MJupM_c = 4.45^{+0.75}_{-0.37}\,M_{\mathrm{Jup}}, ec0.41e_c\approx0.41). The inclination posteriors indicate a bimodal prograde/retrograde degeneracy for b, while c's spatial orbit is well-constrained. The mutual inclination distribution centers on 100\sim 100^\circ with zero degrees strongly excluded (>2σ\sigma), marking HD 48265 as a system with significant nondynamical coplanarity. Figure 1

Figure 1: (a) Radial velocity curve for HD 48265; (b) RV residuals; (c)–(d) RV signatures for planets b and c individually.

Figure 2

Figure 2: Boxplot comparison of Gaia DR2/3 astrometric offsets with the HD 48265 joint model, demonstrating tight astrometric constraints.

Figure 3

Figure 3: Posterior distributions for the mutual inclination Φ\Phi (left) and i2i1|i_2 - i_1| (right) for HD 48265, evidencing significant orbital misalignment.

This configuration is dynamically consistent with outcomes of violent planet–planet scattering or von Zeipel–Kozai–Lidov cycles, as illustrated by secular integrations evidencing periodic exchange between inclination and eccentricity. Figure 4

Figure 4: Secular evolution of inner planet eccentricity and inclination in the HD 48265 system, showing KL-type cycling.

HD 68475: Long-Period High-Eccentricity Candidate for Direct Imaging

HD 68475 is found to host a cold Jupiter with a notably long period (P=21.40.9+1.3P=21.4^{+1.3}_{-0.9} yr), high eccentricity (eb=0.62±0.02e_b=0.62\pm0.02), mass (Mb=5.160.47+0.53MJupM_b=5.16^{+0.53}_{-0.47}\,M_{\mathrm{Jup}}), and well-constrained inclination (ib88i_b\approx88^\circ). At a semimajor axis of $7.3$ AU, the planet's predicted on-sky separation and brightness contrast (in mid-IR) make it an excellent candidate for thermal emission imaging with ELT/METIS, though it is not accessible to JWST/MIRI due to both IWA and contrast limitations. Figure 5

Figure 5: RV curve for HD 68475, revealing a strong, long-term planet-induced signal.

Figure 6

Figure 6: Gaia astrometric residuals and model boxplots for HD 68475, supporting the three-dimensional orbit.

Figure 7

Figure 7: Predicted astrometric positions for HD 68475 b (2025 epoch), including 13σ1-3\sigma uncertainty contours, validating direct imaging feasibility.

HD 114386: Low-Eccentricity, Two-Planet Architectures

HD 114386 is modeled as a two-planet system, with planet b (P=1049P=1049 d, Mb=1.460.22+0.37MJupM_b=1.46^{+0.37}_{-0.22}\,M_{\mathrm{Jup}}, nearly circular orbit eb=0.02±0.01e_b=0.02\pm0.01) and inner planet c (P=444P=444 d, Mcsini=0.37±0.03MJupM_c\sin i=0.37\pm0.03\,M_{\mathrm{Jup}}, ec=0.10±0.03e_c=0.10\pm0.03). Bayesian evidence disfavors modeling an astrometric signature for the inner planet given the current data, but provides precise dynamical mass and inclination for b. The circularity and inferred migration history indicate efficient eccentricity damping, consistent with Type II migration and dynamical friction during gas disk phases. Figure 8

Figure 8: RV curve for HD 114386, showing well-separated signals from two planets.

Figure 9

Figure 9: Gaia DR2/3 astrometric boxplots vs. model for HD 114386 b, confirming the orbital geometry.

HD 100508: Jupiter Analog at the Long-Period End

HD 100508 hosts a single cold Jupiter (P=15.56P=15.56 yr, Mb=1.200.18+0.30MJup,a=6.1M_b=1.20^{+0.30}_{-0.18}\,M_{\mathrm{Jup}},\, a=6.1 AU, e=0.42e=0.42). The inclination solution retains the characteristic RV + two-epoch Gaia astrometric degeneracy (i=62i=62^\circ or 124124^\circ), but mass, semimajor axis, and eccentricity are all robustly constrained. The existence of such a long-period, low-eccentricity object within the accessible RV, Gaia, and Hipparcos baseline strongly suggests that a substantial hidden population of cold Jupiters resides at large separations, undiscovered by present-day Doppler systems but within Gaia's reach. Figure 10

Figure 10: RV curve fitting for HD 100508, showing coherence with the long-period planet solution.

Figure 11

Figure 11: Gaia astrometric boxplot diagnostics for HD 100508 with residual scatter possibly indicating the presence of an additional, longer-period companion.

Population Comparison and Dynamical Implications

The period–mass and period–eccentricity distributions for the new planet sample are set against the ensemble of confirmed exoplanets with inclinations, revealing that HD 100508 b and HD 68475 b populate the extreme long-period region and HD 68475 b, in particular, exhibits exceptionally high eccentricity for its mass and period. Figure 12

Figure 12: Top: Period–mass distribution showing new detections (yellow stars) probing the long-period, Jupiter-mass regime. Bottom: Period–eccentricity distribution shows high eccentricities for some sources.

The mutual inclination analysis for HD 48265, with a median value near 100100^\circ and a 2σ2\sigma exclusion of coplanarity, provides a direct test of planet–planet scattering vs. disk-driven architecture formation scenarios. The inner/outer planet eccentricity–inclination secular exchange realized in this system, observed in REBOUND integrations, is classic for high-Φ\Phi Kozai domains. For HD 114386, the nearly circular orbits of both planets are consistent with strong disk damping and slow migration.

Astrometric Model Validations and Systematics

Multi-epoch Gaia data allow differential astrometric solutions with error propagation that break the MsiniM\sin i barrier and, for well-constrained datasets, disfavors stellar activity false positives (as validated by GLS and Pearson tests). Figure 13

Figure 13: GLS periodograms of RVs and stellar activity indices for all four targets demonstrate that RV periodic signals are not correlated with stellar activity.

Figure 14

Figure 14: Pearson correlation analysis between RV and S-index for all systems, r<0.3|r|< 0.3 in all cases, confirming planetary, not stellar, origins of the RV signals.

Completeness and Future Prospects

Injection–recovery completeness tests confirm sensitivity to Jupiter analogs across the MpsiniM_p\sin iaa parameter space of interest, but also indicate that a large population of cold Jupiters with even longer periods or higher inclinations remains to be characterized. Figure 15

Figure 15: Injection–recovery completeness simulation showing system sensitivity to Jupiter analogs as a function of MsiniM\sin i and aa.

Looking forward, the authors emphasize that Gaia DR4—anticipated with full epoch astrometry and improved baselines—will significantly enhance detection power for the next generation of cold Jupiters. Direct imaging via high-contrast, mid-IR instrumentation such as ELT/METIS will empirically probe atmospheric and physical properties of the coldest, widest-separation gas giants. Dynamically misaligned architectures such as HD 48265 will be pivotal test cases for discriminating among competing formation and migration paradigms.

Conclusion

This work provides precise dynamical characterization for four long-period cold Jupiters using full 3D orbits derived from combined RV and multi-epoch astrometry. Key results include the robust identification of a strongly mutually inclined planetary pair (HD 48265), a high-eccentricity, directly imageable planet (HD 68475 b), a Jupiter analog at unprecedented orbital period (HD 100508 b), and a system manifesting efficient disk-driven eccentricity damping (HD 114386). The presented methodology demonstrates the critical value of multi-year astrometric series when integrated with legacy and new-generation Doppler surveys, both for breaking classical RV limitations and for uncovering complex planetary architectures otherwise beyond reach. The results foreshadow a major expansion in the observable parameter space for cold Jupiters with next-generation astrometric and imaging surveys (2601.11280).

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