Centauri Dreams recently discussed the planets around HD 73526, as described in detail on astronomer Gregory Laughlin’s Systemic site. HD 73526c seemed attractive as a venue for life-bearing moons — a gas giant, it orbits well within its parent star’s habitable zone. The post inspired questions from readers on whether the chances for life on any large moons of such a planet would be minimized by Jupiter-style radiation fields. And given the unusual orbital resonance between the two planets, questions also arose about how these gas giants might have formed. Laughlin (University of California, Santa Cruz) was kind enough to answer these queries. His responses follow, with my inserted comments in italics.
The radiation environments around both HD 73526 b and c are probably more intense than in the vicinity of Jupiter. This increase would mainly be the result of the planets having larger masses than Jupiter, which gives them more vigorous interior convection and hence stronger magnetic fields. The planets also receive a larger flux of stellar wind particles as a result of orbiting closer to the parent star. The auroral displays on these planets are likely an awesome sight.
The fierce radiation environment also compromises the habitability of any moons in orbit around HD 73526 c. The moons would need to have strong magnetic fields of their own in order to stave off atmospheric erosion.
Image: HD 73526, a Sun-like star with a gas giant in the habitable zone. Credit: Space Telescope Science Institute (STScI).
Those ‘water worlds’ I speculated on yesterday in a comment on the original post may not be such comfy environments for life after all. And what about how these planets formed? Laughlin again:
Regarding the formation of the two gas giants orbiting HD 73526, I can
think of three (somewhat related) hypotheses. In decreasing order of
plausibility these are:
(1) The inner planet grew to its current large mass through the standard core-accretion process. It likely migrated inward to a distance of ~2AU after starting at the snowline of the protostellar disk (~5AU). The outer planet then formed and also began to migrate inward. When it reached a 2:1 orbital commensurability with the inner planet, the pair captured each other into resonance. Once in resonance, they both would have been forced to migrate inward together. As they migrated, their eccentricities were pumped up to the current fairly large values. This scenario does an excellent job of explaining the 2:1 resonant pair orbiting GJ 876. It is more problematic for HD 73526, however, because of the detailed dynamics of the observed resonance. In order for the scenario to work for HD 73526, the migration would have had to have been faster than expected, or the planets may have possessed an initial mutual inclination.
(2) The planets could have formed more-or-less where they are now, and captured each other into resonance as they became massive enough. I have seen core-accretion simulations which show that this scenario can work. The difficulty, however, is with growing the planetary cores fast enough in a region that is inside the protostellar snowline.
(3) The system could be the result of a catastrophic interaction between three planets whose orbits became dynamically unstable. In this scenario, one planet was ejected, and the other two were left in the observed, dynamically active, 2:1 resonant state. This sort of thing has been observed in simulations, but it is quite rare. In fact, if there had been a catastrophic event, one would expect the eccentricities of b and c to be even higher than observed.
For more on this unusual planetary system, see Laughlin’s recent post, and note that he has plugged the radial velocity data for HD 73526 into the Systemic Console for analysis. The console is a Java applet that allows users to manipulate such data and contribute to fine-tuning our tools for exoplanet detection. Laughlin’s Systemic research collaboration will ultimately work with a catalog of 100,000 stars, a fine case of applied distributed science.
This has captured my interest. I can’t seem to find exact data but my impression is that with a Jupiter equivalent gas giant a moon would need to be at least at a distance of ~1 million kilometer (Ganymede) with a strong magnet field to have a chance for surface life (assuming a liquid water enviroment). Mention of Callisto at ~1.7 million kilometers seemed to indicate that while high, with no appreciable magnetic field for the moon, radiation was not lethal.
As you pointed out the way that c evolved would make the difference. The more liquid metallic hydrogen the greater the magnetic field and of course the radiation belts (I never could find any satisfying examples of how much the metallic hydrogen ratios “supercharge” a magnetic field). After some thought I still think outer moons of c might be viable given orbital radius and possibly a lower percentage of free hydrogen due to the higher metallacity of HD 73526.
Are retrograde resonances possible in multi-planet systems?
Authors: Julie Gayon, Eric Bois (Nice Sophia-Antipolis University, CNRS, Observatoire de la Cote d’Azur, Laboratoire Cassiopee, France)
(Submitted on 7 Jan 2008)
Abstract: Most of multi-planetary systems detected until now are characterized by hot-Jupiters close to their central star and moving on eccentric orbits. Hence, from a dynamical point of view, compact multi-planetary systems form a particular class of the general N-body problem (with N greater than 3). Moreover, extrasolar planets are up to now found in prograde orbital motions about their host star and often in mean motion resonances (MMR).
In the present paper, we investigate theoretically in a first step a new stabilizing mechanism particularly suitable for compact two-planet systems. Such a mechanism involves counter-revolving orbits forming a retrograde MMR. In a second step, we study the feasibility of planetary systems to host counter-revolving planets. In order to characterize dynamical behaviors of multi-dimensional planetary systems in the vicinity of observations, we apply our technique of global dynamics analysis based on the MEGNO indicator (Mean Exponential Growth factor of Nearby Orbits) that provides the fine structure of the phase space. We also fit a few examples involving counter-revolving configurations by using the Pikaia genetic algorithm.
Studying and fitting a particular case, namely the HD73526 planetary system, we find that counter-revolving configurations may be consistent with the observational data. We also point up the novel fine and characteristic structure of retrograde MMRs. We show that retrograde resonances and their resources open a family of stabilizing mechanisms involving new behaviors of apsidal precessions. Considering two possible mechanisms of formation (free-floating planets and the Slingshot model), we may conclude that counter-revolving configurations may be considered as feasible.
Comments: 8 pages, 2 tables, 7 figures, accepted to A&A (January 7, 2008)
Subjects: Astrophysics (astro-ph)
Cite as: arXiv:0801.1089v1 [astro-ph]
Submission history
From: Eric Bois [view email]
[v1] Mon, 7 Jan 2008 18:22:55 GMT (786kb)
http://arxiv.org/abs/0801.1089