Tidal dissipation and eccentricity pumping: Implications for the depth of the secondary eclipse of 55 Cancri e
^{1} Univ. Bordeaux, LAB, UMR 5804, 33270 Floirac, France
email: emeline.bolmont@obs.ubordeaux1.fr
^{2} CNRS, LAB, UMR 5804, 33270 Floirac, France
^{3} Laboratoire de Météorologie Dynamique, Institut Pierre Simon Laplace, CZ Paris, France
Received: 3 December 2012
Accepted: 1 April 2013
Aims. We use the super Earth 55 Cnc e as a case study to address an observable effect of tidal heating. This transiting shortperiod planet belongs to a compact multiple system with massive planets. We investigate whether planetplanet interactions can force the eccentricity of this planet to a level affecting the eclipse depth observed with Spitzer.
Methods. Using the constant time lag tidal model, we first calculate the observed planet flux as a function of albedo and eccentricity, for different tidal dissipation constants and for two extreme cases: a planet with no heat redistribution and a planet with full heat redistribution. We derive the values of albedo and eccentricity that match the observed transit depth. We then perform Nbody simulations of the planetary system including tides and general relativity to follow the evolution of the eccentricity of planet e. We compare the range of eccentricities given by the simulations with the eccentricities required to alter the eclipse depth.
Results. Using our nominal value for the dissipation constant and the most recent estimates of the orbital elements and masses of the 55 Cnc planets, we find that the eccentricity of planet e can be large enough to contribute at a measurable level to the thermal emission measured with Spitzer. This affects the constraints on the albedo of the planet, which can be as high as 0.9 (instead of 0.55 when ignoring tidal heating). We also derive a maximum value for the eccentricity of planet e directly from the eclipse depth: e < 0.015 assuming Earth’s dissipation constant.
Conclusions. Transiting exoplanets in multiple planet systems – like 55 Cancri – are exceptional targets for testing tidal models because their tidal luminosity may be observable. Future multiwavelengths observations of eclipse depth and phase curves (for instance with EChO and JWST) should allow us to better resolve the temperature map of these planets and break the degeneracy between albedo and tidal heating that remains for single band observations. In addition, an accurate determination of the eccentricity will make it possible to constrain the dissipation rate of the planet and to probe its internal structure.
Key words: planets and satellites: fundamental parameters / planets and satellites: dynamical evolution and stability / planetstar interactions
© ESO, 2013
1. Introduction
The bright star 55 Cancri hosts at least five planets (Fischer et al. 2008) including the closein 8 M_{⊕}, 2.17 R_{⊕} planet e that is on a transiting orbit (Demory et al. 2011; Winn et al. 2011; Gillon et al. 2012). Table 1 shows the parameters of the star and planet e. Planets 55 Cnc e and Kepler 10 b are the only lowmass planets (M < 10 M_{⊕}) whose secondary eclipse has been observed, respectively by Demory et al. (2012, hereafter D12) and Batalha et al. (2011). In the case of Kepler 10 b, the planetary signal responsible for the eclipse depth is dominated by reflected light due to the spectral window of Kepler (400−900 nm). For this planet, a high albedo (A > 0.5) is required to fit the observation (Batalha et al. 2011; Rouan et al. 2011). The secondary eclipse of 55 Cnc e has been measured by D12 using the 4–5 μm IRAC2 channel of Spitzer. At these wavelengths, the thermal emission dominates the planetary flux. The observation implies an upper limit on the albedo (A < 0.55) as well as an inefficient heat transport towards the night side of the planet. Even with a null albedo, a planet with a uniform temperature would have an insufficient dayside emission to produce the observed drop of flux during the secondary eclipse (D12). The required albedo depends of course strongly on the radius of the planet but Gillon et al. (2012) have put tight constraints on the radius of 55 Cnc e by combining primary transit data from both MOST and Spitzer. The parameters of the bright host star 55 Cnc have been accurately characterized using various techniques (including interferometric measurements) by von Braun et al. (2011).
Stellar properties and minimum mass, radius, and semimajor axis of planet 55 Cnc e.
Planets Kepler 10b and 55 Cnc e share a lot of similarities but their surface albedo derived from secondary eclipse seem to differ. The composition of the two planets can of course be different. In particular, 55 Cnc e has a surprisingly low density that implies a significant volatile content (and therefore a gaseous envelope), as suggested by D12, or a carbonrich composition (ceramics being less dense than silicates) as suggested by Madhusudhan et al. (2012). In the present study, we investigate a scenario that could change the albedo determination, in which the thermal emission of 55 Cnc e is enhanced by the tidal dissipation resulting from a low eccentricity maintained by the other planets of the system. With a method similar to the one Barnes et al. (2010) used to infer the eccentricity of Corot7 b and its tidal heating, we used Nbody simulations that include tidal interactions and general relativity to study the evolution of the system and of 55 Cnc e in particular. We find that the orbit of 55 Cnc e cannot be fully circularized and keeps a low eccentricity subjected to important variations. Using the planets’ orbital elements derived from radial velocity data, we find that the eccentricity of planet e can reach values close to 0.01, which is below the upper limit from observations (e = 0.06, D12) but enough for dissipation to produce an internal heat flux comparable to the stellar heating. In this case, the tidal dissipation affects the observed secondary eclipse depth, which can be compatible with a high albedo.
In a first section we study the influence of tidal dissipation on the thermal emission of the planet and derive the minimum eccentricities required to affect the thermal phase curve and secondary eclipse of 55 Cnc e, for two extreme cases: a planet with no heat redistribution – no atmosphere – and a planet with a full redistribution of the stellar heating. In a second section, we simulate the dynamical evolution of the 55 Cnc system in order to constraint the range of possible eccentricities for planet e.
2. Effect of eccentricity on the secondary transit depth
2.1. Modeling the planet flux
In order to bracket the range of possible situations we consider two different cases: a synchronouslyrotating planet with no atmosphere and a planet with a uniform temperature due to a fully efficient redistribution of the stellar heating by an atmosphere.
The bolometric stellar flux φ_{⋆} and the spectral flux density φ_{⋆ ,λ} received at a distance d are given by given by where σ is the StefanBoltzmann constant, T_{eff} and R_{⋆} are the effective temperature and radius of the star, and where F_{⋆ ,λ} is the spectral flux density at the surface of the star and is computed with the stellar atmosphere code Phoenix (Allard et al. 2012) for the T_{eff}, gravity (log (g)) and metallicity of 55 Cnc (see Table 1). This synthetic spectrum agrees well with available observations (Crossfield, priv. comm.), which are numerous for such a bright star (e.g. IRAS, IRTF, AKARI, Spitzer, Wise).
The planet spectrum is a combination of its thermal emission and the reflected light. To derive the thermal component we first need to calculate the surface temperature map, which depends on both the absorbed stellar flux and the internal heat flux. Note that we consider an eccentricity that remains small enough so that its effect on the irradiation remains negligible. To calculate the stellar heating, we can thus assume a circular orbit and a synchronous rotation. In those circumstances, the irradiation at a given point of the planet does not vary with time. We checked with a more detailed thermophysical model that accounting for the small librations of the planet and the thermal inertia of the surface does not change our results.
If we assume no redistribution of the incident flux (no atmosphere), then the stellar flux absorbed by the planetary surface is a function of the zenith angle θ and the Bond albedo A_{B} and is given by a being the semimajor axis of the orbit. As we set the origin of the geographic coordinates at the substellar point, the zenith angle is given by cosθ = cos(latitude)cos(longitude). We also include an internal heat flow due to tidal dissipation. Other sources of internal heat like radioactivity or remnant of accretion/differentiation can dominate when dissipation is negligible but in this case the resulting surface warming would be too low to affect the observed emission. For instance, the mean heat flow of the Earth corresponds to a surface temperature of only 30 K. Significantly higher values would imply a very young planet, a case we do not consider here given von Braun et al. (2011)’s estimation of the age of 55 Cnc: 10.2 Gyr. Locally, the flux emitted by the surface is equal to the sum of the absorbed stellar flux and the internal heat flow φ_{tides} resulting from tidal dissipation, which we assume uniform over the whole planetary surface. On the dayside, the surface temperature is thus given by while on the night side we have In the case of a full redistribution of the absorbed stellar energy the temperature is uniform over the whole planet and simply given by where T_{eq} is the equilibrium temperature of the planet: The surface of the planet is divided into a longitudelatitude grid. Each cell j of the grid has a surface temperature T_{j} and an area S_{j}. The flux spectral density received by a distant observer at a distance d is given by where α_{j} is the angle between the normal to the cell and the direction toward the observer and I_{j} is the specific intensity of the cell given by where B_{λ} is the Planck function, ϵ_{λ} is the surface emissivity, and A_{λ} is the surface spectral albedo. In this study, we use ϵ_{λ} = 1 and A_{λ} = A_{B} = A. In practice, cosα_{j} is calculated as the dot product of the directions vectors attached to the center of the planet and pointing towards the observer and the center of the j cell. Only locations visible to the observer (cosα_{j} > 0) contribute to φ_{P,λ}.
In the previous formula, the star is considered as a point source but this approximation can become inadequate in the case of extremely close planets. Seen from 55 Cnc e, the angular radius of the stellar disk is 15°. This has two main consequences. First, it affects the distribution of the stellar flux over the planetary surface and thus the temperature map. The terminator that delimits the dayside and the nightside is replaced by a penumbra region, as described by Léger et al. (2011). This effect, however, has a negligible impact on the observed flux even in the case of 55 Cnc e because the affected regions of the planet emit/reflect an insignificant fraction of the total spatiallyunresolved planetary flux. We simulated numerically an extended star by spreading the stellar luminosity over a number of fainter punctual sources distributed over the stellar disk. We found that, for phase angles smaller than 120°, the planetary flux calculated with a point source star and with an extended star differ by less than 1%. There is a second, more significant, effect: phase angles smaller than 15° cannot be observed as they are eclipsed by the star. The outoftransit photometric reference used by D12 actually covers a broad range of phase angles: 68–15° before the eclipse and 15−43° after, while the eclipse itself lasts about one tenth of the orbit. With our model, we can calculate the planetary flux from an airless planet for any phase angle (i.e. subobserver longitude). Therefore, we can either produce the light curve for the whole range of observed phase angles (as in Figs. 1 to 2) or for a phase angle of 35°, which is the averaged value of the outoftransit observations by D12 (as in Figs. 3 to 4).
To compare the computed planetary flux with the measured transit depth of 131 ± 28 ppm derived by D12, we calculate the planet to star contrast ratio R as follows: where D = 12.34 pc is the distance of the 55 Cnc system, w_{λ} is the spectral response of the IRAC2 detector (as given in Fig. 2.4 of the IRAC Instrument Handbook), and Δλ is the IRAC2 band (3.9–5.1 μm).
Fig. 1
Effect of albedo and eccentricity on the light curve. This graph shows the planet/star contrast ratio as a function of the orbital phase for different values of (e,A). All these models give the same flux (131 ppm) for a phase angle of 35°, which is the average value for the outofeclipse Spitzer observations by D12. Calculations are done with the nominal value σ_{p} and the orbital parameters and planetary mass from Endl et al. (2012). The shortdashed and full lines are for a uniform temperature (perfect redistribution of heat) while there is no redistribution in the three other cases. 

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Fig. 2
Same as Fig. 1 but the modeled light curves are superimposed to the actual photometric observations with Spitzer as published by D12. Only 3 of the cases from in Fig. 1, with the same line styles and color, are shown here. 

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Fig. 3
Contraints on albedo and eccentricity from the secondary eclipse depth, in the case of an airless planets. The light green shaded areas are in agreement with the 131 ± 28 ppm depth measured with Spitzer/IRAC2 by D12. The right hand side plot is for an Earthlike dissipation constant σ_{p}; the left and middle plots are for 10^{3} × σ_{p} and 10^{2} × σ_{p}, respectively. The dotted (resp. dashed) lines indicate where reflection (resp. tidal dissipation) accounts for 10 and 50% of the planetary flux (reflection + thermal reemission + tides = 100%). The long dashed pink vertical line represents the observational constraint on the eccentricity given by D12. Horizontal grey bars below the graphs indicate the range of eccentricities found with the dynamical simulations described in Sect. 3.2. The upper and lower bars correspond to initial orbital elements from Endl et al. (2012) and Dawson & Fabrycky (2010), respectively. The maximum and mean values of the eccentricity are indicated, as well as the minimum when larger than 5 × 10^{4}. The blue areas are in agreement with the transit depth, the condition that tides accounts for more than 10% of the planetary flux and compatible with an eccentricity within the range found with the dynamical simulations. For 10^{3} × σ_{p} and 10^{2} × σ_{p} the agreement is met for simulations of Dawson & Fabrycky (2010) while for 1 × σ_{p} the agreement is met for Endl et al. (2012). 

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Fig. 4
Same as in Fig. 3 but for an isothermal planetary surface. 

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2.1.1. Tidal heating
The average surface heat flux φ_{tides} is given by where Ė_{tides} is the rate of tidal dissipation. We use here the constant time lag model to compute Ė_{tides}. For a planet of mass M_{p} in pseudosynchronous rotation orbiting a star of mass M_{⋆} at a semimajor axis a and with a null obliquity (formula 13 from Leconte et al. 2010), the rate of tidal dissipation is given by: (1)where the dissipation timescale T_{p} is defined as (2)and depends on the mass of the planet M_{p}, its dissipation factor σ_{p} (as defined by Hansen 2010) and of the mass of the star M_{⋆}. Na1(e), Na2(e) and Ω(e) are eccentricitydependent factors: The difference in the rate of tidal dissipation assuming synchronization or pseudosynchronization for planet 55 Cnc e is 3.5% for e = 0.06 (the upper limit of eccentricity from D12) and only 0.1% for e = 0.01.
The characteristics of planet e can be seen in Table 1. We used for this study the latest estimation for the radius of 55 Cnc e from Gillon et al. (2012). Both Dawson & Fabrycky (2010) and Endl et al. (2012) give comparable masses for 55 Cnc e.
As in Bolmont et al. (2011, 2012) in order to be consistent with the Earth dissipation inferred from D245 astrometric data (Neron de Surgy & Laskar 1997), our nominal value of σ_{p} is 1.877 × 10^{51} g^{1} cm^{2} s^{1}. This value will be referred thereafter as 55 Cnc e nominal dissipation factor.
The uncertainty on the dissipation factor is, however, considerable. The composition of the planet and its internal structure are unknown while they affect, and are affected by, the dissipation. For instance, if we assume that a melted planet dissipates less than a solid one, an initially solid planet can start to melt due to tidal heating, which in turn lowers its dissipation and the internal heating. For a given eccentricity, this feedback may result in a steady state, in which the internal structure and mineral phases are consistent with the tidal heating. A selfconsistent treatment would thus include a feedback between the dissipation rate and the dissipation factor, but that is beyond the scope of this study. (Such modeling has been done by Henning et al. 2009; Běhounková et al. 2011.) Nonetheless, there is no reason that 55 Cnc e’s dissipation factor should be the same as Earth’s. To take into account this uncertainty we performed simulations over 7 decades of dissipation factors from 10^{5} to 10^{2} × σ_{p}.
Fig. 5
Map representing contours of the average surface heat flux φ_{tides}, as a function of eccentricity and planetary dissipation factor. From left to right the full lines correspond to a flux of 10^{6}, 10^{4}, 10^{2} 1, 10^{2}, 10^{4}, 10^{6}, 10^{8}, 10^{10} W m^{2}. The long dashed lines correspond to a temperature of 10, 10^{2}, 10^{3} and 10^{4} K. The observed value of φ_{tides} on Io, 2.4–4.8 W m^{2} (Spencer et al. 2000), is indicated in black for its estimated eccentricity value of 4.3 × 10^{3} (Murray & Dermott 1999). 

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Figure 5 shows the contours of the average surface heat flux φ_{tides}, as a function of eccentricity and dissipation factor. To affect the observation, φ_{tides} must be extremely high and comparable to the insolation flux. Such values exceed by orders of magnitude the tidal heat flux measured at the surface of Io, which is the largest in the Solar System. The highest values on Fig. 5 certainly imply a melted surface and interior, as well as an extremely efficient vertical heat transfer, which may not be consistent with the assumed strong dissipation, as discussed above. Note, however, that a melted surface does not contradict the airless assumption as melted refractory materials have very low vapor pressures: Léger et al. (2011) calculated that the equilibrium pressure above a substellar magma ocean on Corot 7 b would not exceed a few Pa, with a negligible effect on the opacity and horizontal heat transport.
2.2. Model vs. observations
Besides parameters that are constrained by observations other than secondary eclipse (M_{⋆},M_{P},R_{P},a), φ_{tides} depends on the eccentricity and on the internal dissipation constant σ_{p}, while the albedo A determines the ratio between reflected and absorbed stellar fluxes. At low eccentricities yielding negligible dissipation, the planetary flux depends only on the albedo (and on the heat redistribution assumption). For higher eccentricities, the resulting dissipation can increase the temperature and the flux depends on two additional parameters: e and σ_{p}.
Figures 3 and 4 show contours of the eclipse depth in the Spitzer/IRAC2 band as a function of eccentricity and albedo, and for three values of the dissipation constant: 10^{3} × σ_{p}, 10^{2} × σ_{p} and 1 × σ_{p}. Figure 3 is for a planet with no atmosphere while Fig. 4 is for an isothermal photosphere (full redistribution of the stellar heating). The shaded area gives the A − e domain compatible with the observation by D12 (131 ± 28 ppm). The eclipse depth is calculated for a phase angle of 35° corresponding to the average phase angle during the outofeclipse observations by D12. Isothermal cases cannot match the observation even for A = 0 (as noted by D12) because the dayside would be too cold and would produce an eclipse that is too shallow unless there is an internal source of heat. This isothermal case may not, however, be realistic for such a closein planet, even in the presence of a thick atmosphere. Indeed, the radiative cooling timescale, which varies as T^{3}, is likely to be shorter than the dynamical one due to the high equilibrium temperature of this planet (~1600 K, for an albedo of 0.5). Even a moderate daynight temperature contrasts would make the dayside emission significantly stronger than the nightside one. Note also that a phase modulation exists even in the isothermal case due to the reflected light (unless A = 0).
The cases with no heat redistribution match the observation with either an albedo lower than 0.55 and no eccentricity (in agreement with D12) or with a higher albedo (up to A = 1) and an eccentric orbit. When increasing (resp. decreasing) the dissipation constant, lower (resp. higher) values of the eccentricity are required to modify the eclipse depth by a same factor. In Figs. 3 and 4 the blue shaded area corresponds to cases for which the following three conditions are met: the resulting transit depth is within the observational range, the tides account for more than 10% of the planetary flux and the eccentricity is within the range of eccentricities found by the dynamical simulations of the system. For dissipations of 10^{3} × σ_{p} and 10^{2} × σ_{p}, the range of eccentricity comes from a simulation of the system of Dawson & Fabrycky (2010) and for a dissipation of 1 × σ_{p}, it comes from a simulation of the system of Endl et al. (2012). For example, assuming that tides represent more than 10% of the planetary flux, the observations would be in agreement with a planet of albedo between 0.25 and 0.75 assuming a dissipation of 10^{3} × σ_{p}. As we do not know the dissipation of the planet nor its precise eccentricity the observations would not allow to determine the albedo of the planet. However, D12 gave an observational constraint on the eccentricity of 55 Cnc e, it should not be higher than 0.06. It allows to rule out some of the solutions found. For a dissipation of 10^{3} × σ_{p}, there would no longer be agreement with Dawson & Fabrycky (2010) because the eccentricity is too high. For a dissipation of 10^{2} × σ_{p}, there would be an agreement with Dawson & Fabrycky (2010) for a planet of albedo between 0.35 and 0.7. For a dissipation of 1 × σ_{p}, there would still be an agreement with Endl et al. (2012) for a planet of albedo lower than 0.95.
We define here the critical eccentricity as the eccentricity above which tides affect the transit depth by more than 10% and for which the transit depth is of 103 ppm. This critical eccentricity depends on the dissipation and is given in Table 5 for the range of dissipation factors considered here. In Figs. 3 and 4, the critical eccentricity corresponds to the eccentricity of the intersection of the dashed line corresponding to “tides = 10%” and the upper line of the shaded area. The maximum eclipse depth that we find without dissipation is 134 ppm with no atmosphere and 98 ppm in the isothermal case (to be compared with the 131 ± 28 ppm found by D12).
Whatever the redistribution efficiency, the albedo, and for a dissipation constant of 1 × σ_{p}, eccentricities higher than 0.015 produce too large a planet flux and can be ruled out. However, D12 constrained the eccentricity of 55 Cnc e to be less than 0.06, which allows us to rule out some of the solutions we found.
Figures 3 and 4 also show the range of eccentricities found with Nbody simulations that are described in the next section. These Nbody simulations use two different sets of orbital elements and masses derived from radial velocities, one from Dawson & Fabrycky (2010) and the other from Endl et al. (2012). In particular, the value for the orbital distance of planet e slightly differs between these two sets (see Table 3). The effect on the transit depth calculation is, however, very small and would hardly be seen on these plots. Therefore, Figs. 3 and 4 only present the results obtained with a = 0.01544 AU, the value from Endl et al. (2012).
As shown in Fig. 1, orbital photometry (i.e. phase curve measurement) could break the degeneracy between the different sets of albedo and eccentricity. Cases with strong tidal heating and high albedo exhibit much flatter phase curves than cases with negligible tidal heating and low albedo. Distinguishing between these cases at 4.5 μm would require a photometric precision of the order of 10 ppm, which is not achieved yet as seen in Fig. 2. The space telescope EChO (Tinetti et al. 2012) should reach the required precision and could also observe at wavelengths as long as 11 μm and possibly 15 μm. At these wavelengths the planet/star contrast ratio would increase significantly (200 ppm at 11 μm). Also by measuring the eclipse depth and/or the phase curve at different wavelengths simultaneously, EChO could get a much better constraint on the temperature map of the planet and thus on the albedo vs eccentricity.
With no other constraints on the eccentricity, our results show that all values of the albedos between 0 and 1 are possible for 55 Cnc e if its dissipation factor is of 10^{2} × σ_{p}. The goal of the next section is to estimate the maximum eccentricity of planet e using Nbody simulations of the 55 Cnc system.
3. The eccentricity of 55 Cnc e: damping vs. forcing
In a system with one planet, the eccentricity of such a closein planet would be damped to zero very quickly, however 55 Cnc e is part of a compact fiveplanet system. Planetplanet interactions can maintain an eccentricity, which would be an equilibrium between the tidal damping and the excitation by the other planets.
3.1. Eccentricity evolution assuming a single planet system
The model used for the study of the evolution of one planet around its host star is a a rederivation of the equilibrium tide model of Hut (1981) as in Eggleton et al. (1998). We consider both the tide raised by the star on the planet and by the planet on the star. We apply the constant time lag model (Leconte et al. 2010) and use Hansen’s (2010) estimation of the internal dissipation constant of giant exoplanets and their host stars for planet “b” and 55 Cnc. For consistency, we use for planet e the same dissipation constant as in the tidal heating model (see Sect. 2.1.1).
The secular evolution of the eccentricity of the planet is given by Hansen (2010): (3)where Ω_{p} is the planet rotation frequency, and n is the mean orbital angular frequency. The stellar parameters are obtained by switching the p and ⋆ indices. Ne1(e) and Ne2(e) are given by: The integration of the tidal equations was performed using a fourth order RungeKutta integrator with an adaptive timestep routine (Press et al. 1992). The precision of the calculations was chosen such that the final semimajor axis of each integrated system was robust to numerical error at a level of at most one part in 10^{3}.
The characteristics of the star and the inner planet of the 55 Cnc system are listed in Table 1.
We use for the star 55 Cnc the value of stellar dissipation derived by Hansen (2010): σ_{⋆} = 4.992 × 10^{66} g^{1} cm^{2} s^{1}. We compute the tidal evolution of 55 Cnc e with the dissipation factor given in Sect. 2.1.1 and we also compute separately the tidal evolution of 55 Cnc b. This planet is thought to be a gas giant, so Hansen’s value for gas giants is used: σ_{b} = 2.006 × 10^{60} g^{1} cm^{2} s^{1}. The radius of 55 Cnc b is calculated assuming a Jupiter density.
Because the planetary spin synchronization timescale is short compared to the other timescales considered here (Leconte et al. 2010; Heller et al. 2011), each planet rotation period is fixed to the pseudosynchronization value at every calculation timestep. Note that for the low eccentricities found for planet e, the difference in the dissipation rates calculated assuming pseudosynchronization and sychronization is negligible. If the obliquity of planet e is determined by planetary tides, it reaches zero on very short timescales. The obliquity of planet “b” should not evolve tidally on less than Gyr timescales. For simplicity, we assume both obliquities to be zero.
If the obliquity of 55 Cnc e were nonzero it would affect our results by increasing the planet’s dissipation rate and tidal heat flux. Neglecting the obliquity of 55 Cnc e therefore gives us a lower limit on the possible tidal flux. We calculated the tidal flux for two different obliquities of planet e. Figure 6 shows the ratio of the planetary tidal to total flux in the Spitzer band for different obliquities, for dissipation factors and albedos. As expected, the lower the dissipation factor, the higher the eccentricity needed to reach the ratio of 10% of the planet tidal flux over its total flux. For a dissipation of 10^{3} × σ_{p}, the eccentricity needed to reach 10% is of about 0.1 for a planet with an albedo of 0 and this eccentricity is of 0.04 if the albedo is of 1. In the IRAC2 Spitzer band, the thermal emission dominates over the reflected light so increasing the albedo has an effect of decreasing the non tidal part of the flux emitted by the planet. Thus, a smaller eccentricity is needed for the tidal flux to reach 10% of the planet total flux.
The right panel of Fig. 6 shows a case for which planet e’s obliquity of 2 degrees may have been excited by forcing from the other planets. Had this planet been alone, tides would have reduced this obliquity in very short timescales. The major difference with the left panel is that for small eccentricities, the ratio F_{p,tides}/F_{p,tot} is non zero. The obliquity contributes to the tidal dissipation in a strong way. If the planetary dissipation is more than 10^{2} × σ_{p}, the ratio is always bigger than 10% whatever the value of the planet’s albedo. For eccentricities bigger than 0.1, the tidal dissipation due to the eccentricity becomes dominant again.
The study of the effect of obliquities of the inner planets on the Nbody evolution of the system will be conducted in the future.
Fig. 6
Ratio of 55 Cnc e tidal flux over its total flux as a function of eccentricity for two different obliquities (0° and 2°). The purple curve corresponds to a dissipation factor of 10^{3} × σ_{p}, the blue one to 10^{2} × σ_{p}, the green one to 10^{1} × σ_{p} and the orange one to 10^{1} × σ_{p}. The full line corresponds to a Bond albedo of the planet of 0, the small dashed line to an albedo of 0.5, the dashed dotted line to an albedo of 0.8 and the long dashed one to an albedo of 1. The black horizontal dashed line represents a ratio of 10%. 

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The tidal evolution of a single planet around a star is determined by the tide raised by the planet on the star – the stellar tide – and the tide raised by the star on the planet – the planetary tide. The eccentricity damping timescale τ_{ecc}_{plan} due to the planetary tide is given by .
For 55 Cnc e, τ_{ecc}_{plan} ~ 4600 yrs, and the eccentricity damping timescale due to the stellar tide is τ_{ecc}_{star} ~ 1.4 × 10^{10} yrs. The evolution of the eccentricity of 55 Cnc e will therefore be dominated by the planetary tide. Let us define the eccentricity damping timescale as τ_{ecc} = τ_{ecc}_{plan}. In Fig. 7, the evolutionary tracks of 55 Cnc e are represented in purple dasheddotted lines for a nominal dissipation factor σ_{p}. If this planet was alone in the system, the eccentricity would be damped in about 10 × τ_{ecc}_{plan}.
For 55 Cnc b, τ_{ecc}_{plan} and τ_{ecc}_{star} are longer than the age of the system. The eccentricity of 55 Cnc b will remain at its present values on more than Gyrs timescales. In Fig. 7, the evolutionary tracks of 55 Cnc b are represented in blue dasheddotted lines. If this planet was alone in the system, its semimajor axis and eccentricity would remain the same for more than one billion years.
However, to accurately describe the evolution of 55 Cnc e, it is crucial to take into account the fact that these planets are interacting and are part of a fiveplanet system.
Fig. 7
Evolution of semimajor axis and eccentricity for the five planets of 55 Cnc assuming the “nominal” tidal dissipation for 55 Cnc e and the initial conditions come from Dawson & Fabrycky (2010). Top panel: the semimajor axis is plotted in thick colored lines, the colored dashed lines represent the distance of aphelion and perihelion for each planet. The corotation radius is indicated by a black dashed line and the thick red dashed line is the stellar radius. Bottom panel: the colored full lines represent the eccentricities of the five planets, the dashed dotted lines represent the secular evolution 55 Cnc e (purple) and 55 Cnc b (blue) would experience if alone in the system. The thick red dashed line represent the critical eccentricity of planet e above which its secondary transit depth is increased by more than 10% by tidal heating. 

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3.2. Eccentricity evolution assuming the fiveplanet system
3.2.1. Tides in multiple planets systems
To compute the tidal interactions we used the tidal force as expressed in Hut (1981) for the constant time lag model. We added the force in the Nbody code Mercury (Chambers 1999). Kaib et al. (2011) showed that the system is expected to be nearly coplanar (all the orbits remain within 5° in their simulations). Ehrenreich et al. (2012) claim that they have observed the signature of an extended hydrogen atmosphere of planet b, grazing the stellar disk, implying a very low mutual inclination between planets e and “b”. Because planet e is transiting, assuming coplanarity implies that all the minimum masses inferred from radial velocity are close to the true masses. Kaib et al. (2011) predicted that the plane of the orbits should be misaligned with the star due to the influence of the binary companion 55 Cnc B. In this study, however, we assume a zero inclination of the system and neglect the gravitational influence of 55 Cnc B. Furthermore, we consider that the planets have zero obliquity. We consider the tidal forces between the star and the planets but we neglect the tidal interaction between planets. In this formalism, the total tidal force exerted by the star on the ith planet gives an acceleration for the planet of: (4)where R_{i} is the radius of the ith planet, M_{i} its mass, σ_{i} its dissipation factor, k_{2,i} its potential Love number of degree 2. r_{i} is the distance between the center of star and the ith planet and its derivative. is the derivative of the ith planet’s true anomaly θ_{i} (the instantaneous orbital angular velocity). The radial vector e_{r,i} links the center of the star S to the center of the ith planet P_{i}, . The orthoradial vector e_{θ,i} is such that , where is the orbital angular momentum of the ith planet, here in heliocentric coordinates.
Here, we consider that only the two inner planets feel the effects of tides. This assumption is justified by the order of magnitude calculation made in Sect. 3.1. Both planets are assumed to be in pseudosynchronous rotation.
We also add the orbital acceleration due to general relativity (Kidder 1995; Mardling & Lin 2002). Adding this force causes a change in the period of the eccentricity oscillations but does not change much the equilibrium eccentricity of planet e.
We performed different simulations with two sets of initial conditions. For each set of initial conditions, we varied the planetary dissipation from 10^{5} × σ_{p} to 100 × σ_{p}.
The first set of initial conditions is from Dawson & Fabrycky (2010) and the second one is from Endl et al. (2012). Tables 2 and 3 show the initial conditions for Dawson & Fabrycky (2010) and Endl et al. (2012) respectively.
Minimum mass, and orbital elements of the three outer planets of the 55 Cnc system.
Minimum mass, and orbital elements of the five planets of the 55 Cnc system.
3.2.2. Results
Orbits and masses from Dawson & Fabrycky (2010 )
Figure 7 shows the 1 Myr evolution of the 5planet system starting from the orbits from Table 2 and for a dissipation factor of 1 × σ_{p} for 55 Cnc e. For the first few 10^{4} yrs, the eccentricity of 55 Cnc e (initially set to 0.17) decreases as expected by the secular evolution calculations (dasheddotted purple line), as if it were alone in the system, save a few oscillations. But after this initial decay, the eccentricity stops decreasing and oscillates around a few 10^{3}, due to the simultaneous influence of tidal damping and eccentricity pumping by the other planets.
Over 1 Myr, the semimajor axis of 55 Cnc e does not vary significantly. It decreases from 1.560 × 10^{2} AU to 1.515 × 10^{2} AU in the first few 10^{4} yrs while the eccentricity is still high and then decreases to reach 1.512 × 10^{2} AU at 1 Myr. As expected from the order of magnitude timescale, the eccentricity of 55 Cnc b does not decrease over the integration time. However due to the presence of other planets exciting its orbit, 55 Cnc b’s eccentricity oscillates around 0.016.
We tested if assuming pseudosynchronization for 55 Cnc e and 55 Cnc b is correct when their eccentricities oscillate around their mean value. When 55 Cnc e has the maximum eccentricity its pseudosynchronization period is of 17.949016 h, and when it has the minimum eccentricity, it is of 17.950161 h. The difference between these two values is of ≲0.01%, which is negligible for dissipation. So the pseudosynchronization remains a good assumption. For 55 Cnc b tidal interaction is weak so it keeps its initial rotation period throughout the evolution. We chose here to assume pseudosynchronization.
To validate our version of the Nbody code Mercury with tides, we verified it could reproduce the tidal evolution of single planet systems simulated with the code used in Bolmont et al. (2011) and Bolmont et al. (2012), which solves the tidal secular equations for the semimajor axis, eccentricity (Eq. (3) of this paper) and rotation spin evolution of planet and star. We tested the general relativity effects with Mardling (2007)’s calculations for the secular evolution of twoplanet systems. However as they use the constant phase lag model to compute the tidal force, we cannot compare their tidal evolution calculations with our simulations, which are based on the constant time lag model. The recent literature has debated the applicability of the constant time lag and constant phase lag models. The constant phase lag model has been shown to be mathematically inconsistent (Efroimsky & Makarov 2013). On the other hand, Greenberg (2009) showed that the response of a viscoelastic fluid reduces exactly to the constant time lag approach in the limit where the forcing frequency is smaller than the natural frequency of the system and where damping is weak (see his equations 8b and c in these limits). A real planet’s response is certainly much more complex than the one of a viscoelastic fluid, meaning that the constant time lag approach must also be used with care. The constant time lag model is a linear theory but taking into account nonlinear terms can result in noticeable changes (Weinberg et al. 2012). However, we choose this model because we believe that it stands on more robust mathematical grounds than the constant phase lag model.
As the dissipation factor of planets is not well known, we decided to cover a wide dissipation factor range, from 10^{5} × σ_{p} to 100 × σ_{p}. As seen in Sect. 2, the dissipation factor affects the tidal heating and change the value of the eccentricity required to affect the depth of the secondary eclipse. In addition, changing the dissipation in 55 Cnc e has two effects on its orbital evolution. First, it has an effect on how fast its eccentricity decreases. For a dissipation factor of 0.1 × σ_{p}, the eccentricity reaches the “equilibrium” in ~ 3 × 10^{5} yrs, while for a nominal dissipation factor, it does so in ~ 3 × 10^{4} yrs, and ~ 3 × 10^{3} yrs for 10 × σ_{p}. This is in agreement with the order of magnitude calculation of Sect. 3.1. In fact, the eccentricity damping timescale τ_{ecc} scales as T_{p} so as , so if the dissipation factor is twice the fiducial value τ_{ecc} is half the value calculated for the nominal dissipation factor.
Thus for dissipations below 10^{2} × σ_{p} the “equilibrium” eccentricity is not reached in less than 1 Myr because the system is still in the circularization period. For dissipation lower than 10^{2} × σ_{p}, the minimum, average and maximum values of the eccentricity of Table 5 are calculated for the whole evolution. For dissipation bigger than 10^{1} × σ_{p}, the “equilibrium” eccentricity is reached in less than 1 Myr. The minimum, average and maximum values of the eccentricity are then calculated when the eccentricity has reached the “equilibrium”.
The evolution of the system assuming 55 Cnc e has a dissipation factor of 10^{2} × σ_{p} can be seen in Fig. 8. The eccentricity of 55 Cnc e remains higher than the critical eccentricity for ~6 × 10^{5} yrs. For a dissipation of 100 × σ_{p}, the planet 55 Cnc e falls on its star in ~1.2 × 10^{5} yrs. It is therefore likely that the planet dissipates less than this value because the probability of observing the system in this configuration is low.
Changing the dissipation factor of 55 Cnc e has also an effect on the forcing of its eccentricity by the other planets. The “equilibrium” eccentricity oscillates between a minimum and a maximum value, which are given in Table 5 for the different planetary dissipation factors.
Fig. 8
As Fig. 7 but assuming a dissipation factor of 10^{2} × σ_{p} for 55 Cnc e. 

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As expected, when the planetary dissipation is higher the forced eccentricity is lower. In Fig. 7, we plot the critical eccentricity above which the tidal heating has an effect of more than 10% on the depth of the secondary transit. This value evolves with the dissipation. If the planet has a large dissipation factor, the eccentricity needed to have a strong tidal dissipation is lower. In Sect. 4, we discuss the configurations that produce the strongest tidal signature in the transit depth.
Minimum, maximum and mean value of the eccentricity of 55 Cnc e obtained in the simulation of the system proposed by Dawson & Fabrycky (2010) for different dissipation factor for 55 Cnc e.
Minimum, maximum and mean value of the eccentricity of 55 Cnc e obtained in the simulation of the system proposed by Endl et al. (2012) for different dissipation factor for 55 Cnc e.
Fig. 9
As Fig. 7, but the initial conditions come from Endl et al. (2012). 

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Figure 7 shows that the eccentricity of 55 Cnc e determined by Dawson & Fabrycky (2010), e = 0.17, is not stable as it is damped to values of a few 10^{3} in less than 10^{5} yrs. Table 5 also shows that the eccentricity of 55 Cnc e never becomes high enough to cause a notable increase in the IR emission of the planet. In the absence of significant tidal heating, inefficient redistribution of heat and an albedo lower than 0.55 are required.
Orbits and masses from Endl et al. (2012 )
Using the orbital distances, masses and exact arguments of pericenter proposed by Endl et al. (2012) lead to a destabilization of the system. We simulated the system with the Nbody code Mercury without the tidal forces and without general relativity and the outcome is the ejection of a planet. We also simulated the system without tides but with general relativity and the outcome is also the ejection of a planet. However, if we simulate the system with the orbital distances and masses from Endl et al. (2012) but using random arguments of pericenter (knowing that the values they provide are affected by significant uncertainties), we usually find that the system is stable on 10^{7} yrs timescales.
Figure 9 shows the simulation using orbital elements and masses from Endl et al. (2012). The important differences between Endl et al. (2012) and Dawson & Fabrycky (2010) for the dynamical evolution of the system mainly lie in the values of the eccentricities of b and c. In Dawson & Fabrycky (2010), b and c have small eccentricities: 0.01 for b and 0.005 for c, while in Endl et al. (2012) b has a small eccentricity: 0.004 but c has a high eccentricity: 0.07. In Dawson & Fabrycky (2010) after the damping of its initially high value, the eccentricity of e depends mainly on the eccentricity of b and in a weaker way on the eccentricity of c. However for Endl et al. (2012), we observe that c excites b from the initial value of 0.004 to the mean value of ~ 0.02. So e is excited by a more eccentric planet b than was the case for Dawson & Fabrycky (2010), and in a weaker way by a more eccentric planet c.
The eccentricity of 55 Cnc e cannot be zero because of the presence of the other planets, it oscillates around 4.98 × 10^{3}. The eccentricity of b also increases to oscillate around 2.20 × 10^{2}. However, during the evolution of the five planets, the system frequently passes within the error bars of the current configuration derived by (Endl et al. 2012). For these configurations, the eccentricity of 55 Cnc e is higher than the critical eccentricity for tidal heating. This simulation therefore provides dynamical evolution snapshots that are simultaneously consistent with the system properties derived from radial velocities, the secondary eclipse depth observed with Spitzer and an observable tidal heating.
As seen in Table 5 and Fig. 9, the mean eccentricity of 55 Cnc e is also higher than the critical value. For 10 × σ_{p}, the maximum value of the eccentricity is above the critical eccentricity while for 0.1 × σ_{p} the eccentricity always remain below the critical value.
In Fig. 3 (airless case) we can see that the upper limit on the albedo is 0.75 for the mean eccentricity from this simulation. For the maximum eccentricity, this upper limit is as high as 0.85. Interestingly, these high values of the albedo match those inferred for the exoplanet Kepler 10 b.
In the isothermal case (Fig. 4) the upper limit on the albedo is 0.1 for the mean eccentricity from this simulation. For the maximum eccentricity, this upper limit is 0.7. No solutions are found for 0.1 × σ_{p} and a marginal match is found with 10 × σ_{p} with A < 0.05.
4. Tidal dissipation, transit depth and eccentricity
Figure 10 sums up what has been discussed so far. It shows the range of simulated eccentricities of 55 Cnc e for an evolution of 1 Myr superimposed with the albedodependent region in the eccentricityplanetary dissipation parameters space corresponding to the two following conditions: (5)The first condition is that the tidal flux is more than 10% the total flux of the planet. The second condition corresponds to the observability constrain of a transit depth of 131 ± 28 ppm, where F_{⋆} is the flux of the star calculated – as the flux of the planet – at a distance of 12.34 pc (D12) in the Spitzer band.
Fig. 10
Eccentricity vs dissipation. The thick colored lines corresponds to the minimum, average and maximum eccentricity – bottom full line, middle dashed line and top full line – of 55 Cnc e obtained with the simulations of Dawson & Fabrycky (2010) in purple, and Endl et al. (2012) in blue. The horizontal black dashed line corresponds to the upper limit from observations (e = 0.06, D12). The color bands correspond to the region where the two conditions of Eq. (5) are met: where the tides contribute to more than 10% of the planet’s flux and where the resulting transit depth is between the observational constraints. The light orange band corresponds to an albedo of 0 and the red one to an albedo of 1. The orange dashed dotted lines delimit the band corresponding to an albedo of 0.65. 

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The configurations for which the two conditions are met are therefore where the thick colored curves representing the output of our Mercury code intersect the shaded areas. For Dawson & Fabrycky (2010), the overlap occurs from a dissipation of a few ~ 10^{4} × σ_{p} to a dissipation of a few 10^{2} × σ_{p}. However, as the eccentricity of the planet has been constrained by observations (D12) to be smaller than 0.06, the lower limit of the dissipation we can infer is about 8 × 10^{3} σ_{p} – where the dashed dotted orange line intersects the horizontal black dashed line. For dissipations lower than 10^{2} × σ_{p}, the eccentricity of 55 Cnc e has not reached the “equilibrium” eccentricity, and the planet is still in its circularization period after 1 Myr. The eccentricity decreases slowly with small oscillations as seen in Fig. 8. So for dissipations lower than 10^{2} × σ_{p}, the minimum eccentricity plotted in Fig. 10 is the eccentricity of 55 Cnc e at t = 1 Myr and the maximum eccentricity is the high initial one 0.17. It means that for these configurations, the two conditions of equation 5 are met for a short period of time only. For example, for a dissipation of 10^{2} × σ_{p}, the two conditions are met for ~ 6 × 10^{5} yrs after the proposed present configuration (Dawson & Fabrycky 2010). We do not know the previous state of the system, but it is likely that with such low dissipation the ancient eccentricity was significantly higher than its present value.
The most favorable configuration is for a planet with A ~ 0.65 as can be seen in Fig. 3. This albedo corresponds to the band delimited by orange dashed dotted lines in Fig. 10. Figure 3 shows that if the tides contribute to more than 10% to the planet’s flux, and the eccentricity of the planet is less than 0.06 and the transit depth is in agreement with the observations, the albedo of the planet would be between ~0.5 and 0.7.
For Endl et al. (2012), a consistency between the two conditions and the eccentricity range obtained with Mercury simulations is found for dissipations around 1 × σ_{p}. Depending on the dissipation, the two conditions are in agreement with the whole range of albedo. Contrary to the case of Dawson & Fabrycky (2010), the eccentricity oscillates around the “equilibrium” eccentricity for all the dissipation range values. So over time the system will be periodically in configurations for which the two conditions are met. Over an oscillation of the eccentricity, the two conditions are met when the eccentricity is the higher. For example, as can be seen in Fig. 10, for a dissipation of 10 × σ_{p}, the only configuration which would be in agreement with the two conditions is when 55 Cnc e reaches the maximum value of the eccentricity oscillations, and it would mean that the planet has an albedo of 0.65.
5. Discussion
This work shows that the albedo cannot be constrained directly from the eclipse depth due to the influence of tidal heating on the radiative budget. For a given dissipation constant there is, therefore, a degeneracy between albedo, eccentricity and the assumed heat redistribution scenario. This degeneracy can partially be broken by using precise orbital photometry, as shown in Fig. 1. A measure of the eclipse depth and/or the phase curve a different wavelengths would provide an additional constraint on the temperature map (as shown for instance by Maurin et al. 2012) and thus on the heat redistribution as well as on the relative contributions of tidal and radiative heating. A measure of the secondary eclipse and/or the phase curve at visible wavelengths that are not affected by thermal emission would provide a direct measurement of the albedo and would also help breaking this degeneracy. The ratio between the dayside emission of the planet and the star is however very small: A × 17.5 ppm and should be measured over a broad wavelength range in order to infer the Bond albedo. The photometric survey of 55 Cnc with MOST (Winn et al. 2011) reveals a modulation of the luminosity of the system (in the 350–700 nm window), at the orbital period of the planet and whose phase is consistent with a phase modulation. However, the amplitude of this modulation, ~170 ppm is nearly 10 times larger than what could be attributed to the planet. In addition the light curve does not exhibit a significant drop when the secondary eclipse occurs. This points to a modulation of the stellar luminosity itself. Winn et al. (2011) suggest that that part of the stellar hemisphere facing the planet could be slightly fainter than the rest of the star due to magnetic interaction between the planet and star. Such a stellar modulation would also make extremely challenging the extraction of the planetary phase modulation. How better is the situation in the infrared still has to be evaluated.
Our calculations assume that the internal heat flux is released uniformly over the planet. The existence of one or a few hot spots could significantly change the results. As an extreme case, if all the heat is released in the dark hemisphere, it has no effect on the dayside emission and thus a weak effect on the secondary eclipse depth. This would however have a strong signature on the orbital photometry.
In this study, we modeled the orbital photometric signature of planet e as if it was alone in the system. Kane et al. (2011) showed that, at visible wavelengths, the modulation due to planet “b” may not be negligible compared with that of planet e, depending of course on the respective albedos of planets e and “b”. Characterizing the properties of planet e by orbital photometry thus requires the ability to distinguish between the two components, which is an additional challenge. At thermal wavelengths, the situation should be different because planet “b” is a Jovian planet and atmospheric circulation tends to attenuate the day/night temperature contrast and thus the amplitude of thermal phase curve. To estimate this temperature contrast we can compare radiative and dynamical timescales. The radiative cooling timescale is given by where c_{P} is the specific heat of H_{2}, P is the pressure at the considered level and T is the bolometric brightness temperature. Assuming a superrotating atmosphere (as that of Venus or as predicted for strongly irradiated atmospheres (see for instance Showman et al. 2009; and Selsis et al. 2011), a relevant dynamical timescale is given by τ_{D} = R/v where R is the planetary radius and v is the average of the zonal wind. Let us use P = 0.1 bar (a typical photosphere for infrared radiation), T = 700 K (the equilibrium temperature of the planet for A = 0), R = R_{Jup}. Using 3D hydrocodes, Selsis et al. (2011) found v ~ 200 m/s for the mean zonal wind speed for a 10 bar CO_{2} atmosphere and an equilibrium temperature of 390 K, while Showman et al. (2009) found one order of magnitude faster winds for HD 189733b (T_{eq} = 1200 K). Assuming 200 < v < 2000 m/s yields 1 < τ_{R}/τ_{D} < 10, which implies an efficient heat redistribution between the day and night hemisphere and thus a rather flat phase curve. The change of equilibrium temperature between periastron and apoastron is less than 5 K, a difference that should be completely averaged out by the inertia of the atmosphere. The contribution of planet “b” to the photometric variations of the system should thus be negligible at thermal wavelengths.
Observations in several infrared bands will be necessary to establish the radiative budget of the planet and demonstrate the existence of an excess of luminosity due to tidal heating. In particular, in the presence of an atmosphere, the measured brightness temperature can correspond to the physical temperature at any atmospheric level. This temperature can locally exceed the highest temperature that can be found on an airless planet with a null albedo. This can happen in two cases. First, if there is a strong greenhouse warming and if the observed band corresponds to an atmospheric window that probes the surface of the planet. This situation can be illustrated by the thermal phase curves modeled by Selsis et al. (2011) for CO_{2}rich atmospheres. In their Fig. 6, for instance, one can see that the 8.7 μm band (an atmospheric window) exhibits fluxes that are higher in the presence of an atmosphere. However, expected components of a planetary atmosphere, like CO_{2}, CO, SO_{2}, H_{2}S, CS_{2}, have strong absorption bands in the IRAC2 spectral window, making unlikely for this band to probe the deep and hot atmospheric layers heated by greenhouse effect. An “excess” of brightness temperatures can also be observed in an opaque band probing high stratospheric layers subjected to a strong thermal inversion. In the present case this would imply that the atmosphere is sufficiently opaque over the whole 4 to 5 μm for the emission to come from very low pressure layers. Indeed, on the dayside of a synchronously rotating planet, the convective plume powered by the stellar irradiation is drafted to very high altitudes and an inversion appears possible only in the upper atmosphere.
In a recent work, Maurin et al. (2012) proposed to use multiwavelengths orbital photometry to derive the albedo, radius and inclination of rocky planets on circular nontransiting shortperiod orbits. The present study shows that applying this technique requires to insure that tidal heating is not affecting the radiative budget of the planet. Planets subjected to the influence of a massive and eccentric companion could have a small nonmeasurable eccentricity sufficient to produce a significant tidal heating.
In our simulations, we assume the pseudosynchronization of the planet spin. For rocky planets, the very existence of such state has been recently contested by Makarov & Efroimsky (2013), who suggest that the only likely rotation configurations are spinorbit resonances. Taking into account a more realistic rheology for the rocky planets, they show that the seemingly lowestenergy state of pseudosynchronization is actually unstable. In the present study, the eccentricities remain small enough so that the difference between the 1:1 spinorbit resonance and pseudosynchronization has a negligible effect on dissipation, at least after a few 10^{4} yrs. The evolution during the first few 10^{4} yrs of the simulation of the Dawson & Fabrycky (2010) system would, however, be different. Using the constant time lag model, Rodriguez et al. (2012) showed that even though spinorbit resonances are possible for large eccentricities, planets could be in pseudosynchronization for eccentricities smaller than 0.1. This study takes into account the oblateness of the planet in a most accurate way than in our model but does not incorporate a realistic rheology for the terrestrial planets such as in Makarov & Efroimsky (2013).
The initial conditions of our simulations are the present values of semimajor axis and eccentricity of the planets. However, planet e must have formed farther out and migrated in due to tidal evolution. Tides are a dissipative process so it is delicate to integrate the evolution back in time, the solution diverges quickly to a huge semimajor axis and an eccentricity close to 1. To investigate a possible formation distance from the star would require to explore a range of semimajor axis initial conditions to try reproduce present values. Our simulations are time demanding, so exploring a huge parameters space – including the planetary dissipation– in order to find a appropriate configuration would require a lot of time. So, we chose here not to treat past evolution, but investigate the present dynamics of the system.
In this paper, we show the influence of the eccentricity of the outer planets on the eccentricity of the inner planet. In the case of Endl et al. (2012), the presence of the eccentric planet “c” can increase the eccentricity of e from the supposed observational value of 0 to 5 × 10^{3}. The presence of the other planets also influences the eccentricity of the inner planet, so the values of the inner planet equilibrium eccentricity could change if more planets exist in the system as might be the case according to Raymond et al. (2008).
6. Conclusions
Our study shows that the orbit of exoplanet 55 Cancri e cannot be fully circularized due to the influence of the other planets in the system. The forced eccentricity depends on the unknown dissipation constant and on the detailed set of orbital elements for the system. Using an Earthlike dissipation and orbital parameters from Endl et al. (2012), we find an eccentricity that oscillate around a mean value 5 × 10^{3}, up to 8.5 × 10^{3}. The resulting tidal heating is sufficient to affect the thermal emission that has been observed at secondary eclipse with Spitzer/IRAC2 by Demory et al. (2012).
With e = 0 (and thus no internal heating) we find the same constraints on the planetary albedo as Demory et al. (2012): A < 0.55 in the absence of heat redistribution and no match in the case of a uniform temperature. Including tidal heating the upper limit on the albedo becomes 0.9 and 0.7 without heat redistribution and in the uniform case, respectively. With these new constraints, both 55 Cnc e and Kepler 10 b can have a high albedo (A > 0.5).
Assuming an Earthlike dissipation allows us to use the Spitzer measurement to put an upper limit on the eccentricity: e < 0.015, which is significantly lower than the observational constraint from D12 (e < 0.06). The actual dissipation is unknown but future observations (in particular mutiwavelength orbital photometry) will have the ability to better constraint the contribution of tidal dissipation and thus the eccentricity. Alternatively, a more accurate measurement of the eccentricity and of the inclination of the system would allow us to constrain the dissipation.
This shows the importance tidal heating on the radiative budget of closein exoplanets, in particular in compact systems that include eccentric planets. This case illustrates how the dynamics of a whole planetary system can influence the retrieval of the intrinsic properties of one particular planet (here, for instance, the surface albedo).
Acknowledgments
F.S. acknowledges support from the European Research Council (Starting Grant 209622: E_{3}ARTHs). E.B. and S.N.R. thank the CNRS’s PNP program. We thank the referee Rory Barnes for helpful comments that improved the paper.
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 Rodriguez, A., Callegari, N., Michtchenko, T. A., & Hussmann, H. 2012, MNRAS, 427, 2239 [NASA ADS] [CrossRef] (In the text)
 Rouan, D., Deeg, H. J., Demangeon, O., et al. 2011, ApJ, 741, L30 [NASA ADS] [CrossRef] (In the text)
 Selsis, F., Wordsworth, R. D., & Forget, F. 2011, A&A, 532, A1 [NASA ADS] [CrossRef] [EDP Sciences] (In the text)
 Showman, A. P., Fortney, J. J., Lian, Y., et al. 2009, ApJ, 699, 564 [NASA ADS] [CrossRef] (In the text)
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 Winn, J. N., Matthews, J. M., Dawson, R. I., et al. 2011, ApJ, 737, L18 [NASA ADS] [CrossRef] (In the text)
All Tables
Stellar properties and minimum mass, radius, and semimajor axis of planet 55 Cnc e.
Minimum mass, and orbital elements of the three outer planets of the 55 Cnc system.
Minimum, maximum and mean value of the eccentricity of 55 Cnc e obtained in the simulation of the system proposed by Dawson & Fabrycky (2010) for different dissipation factor for 55 Cnc e.
Minimum, maximum and mean value of the eccentricity of 55 Cnc e obtained in the simulation of the system proposed by Endl et al. (2012) for different dissipation factor for 55 Cnc e.
All Figures
Fig. 1
Effect of albedo and eccentricity on the light curve. This graph shows the planet/star contrast ratio as a function of the orbital phase for different values of (e,A). All these models give the same flux (131 ppm) for a phase angle of 35°, which is the average value for the outofeclipse Spitzer observations by D12. Calculations are done with the nominal value σ_{p} and the orbital parameters and planetary mass from Endl et al. (2012). The shortdashed and full lines are for a uniform temperature (perfect redistribution of heat) while there is no redistribution in the three other cases. 

Open with DEXTER  
In the text 
Fig. 2
Same as Fig. 1 but the modeled light curves are superimposed to the actual photometric observations with Spitzer as published by D12. Only 3 of the cases from in Fig. 1, with the same line styles and color, are shown here. 

Open with DEXTER  
In the text 
Fig. 3
Contraints on albedo and eccentricity from the secondary eclipse depth, in the case of an airless planets. The light green shaded areas are in agreement with the 131 ± 28 ppm depth measured with Spitzer/IRAC2 by D12. The right hand side plot is for an Earthlike dissipation constant σ_{p}; the left and middle plots are for 10^{3} × σ_{p} and 10^{2} × σ_{p}, respectively. The dotted (resp. dashed) lines indicate where reflection (resp. tidal dissipation) accounts for 10 and 50% of the planetary flux (reflection + thermal reemission + tides = 100%). The long dashed pink vertical line represents the observational constraint on the eccentricity given by D12. Horizontal grey bars below the graphs indicate the range of eccentricities found with the dynamical simulations described in Sect. 3.2. The upper and lower bars correspond to initial orbital elements from Endl et al. (2012) and Dawson & Fabrycky (2010), respectively. The maximum and mean values of the eccentricity are indicated, as well as the minimum when larger than 5 × 10^{4}. The blue areas are in agreement with the transit depth, the condition that tides accounts for more than 10% of the planetary flux and compatible with an eccentricity within the range found with the dynamical simulations. For 10^{3} × σ_{p} and 10^{2} × σ_{p} the agreement is met for simulations of Dawson & Fabrycky (2010) while for 1 × σ_{p} the agreement is met for Endl et al. (2012). 

Open with DEXTER  
In the text 
Fig. 4
Same as in Fig. 3 but for an isothermal planetary surface. 

Open with DEXTER  
In the text 
Fig. 5
Map representing contours of the average surface heat flux φ_{tides}, as a function of eccentricity and planetary dissipation factor. From left to right the full lines correspond to a flux of 10^{6}, 10^{4}, 10^{2} 1, 10^{2}, 10^{4}, 10^{6}, 10^{8}, 10^{10} W m^{2}. The long dashed lines correspond to a temperature of 10, 10^{2}, 10^{3} and 10^{4} K. The observed value of φ_{tides} on Io, 2.4–4.8 W m^{2} (Spencer et al. 2000), is indicated in black for its estimated eccentricity value of 4.3 × 10^{3} (Murray & Dermott 1999). 

Open with DEXTER  
In the text 
Fig. 6
Ratio of 55 Cnc e tidal flux over its total flux as a function of eccentricity for two different obliquities (0° and 2°). The purple curve corresponds to a dissipation factor of 10^{3} × σ_{p}, the blue one to 10^{2} × σ_{p}, the green one to 10^{1} × σ_{p} and the orange one to 10^{1} × σ_{p}. The full line corresponds to a Bond albedo of the planet of 0, the small dashed line to an albedo of 0.5, the dashed dotted line to an albedo of 0.8 and the long dashed one to an albedo of 1. The black horizontal dashed line represents a ratio of 10%. 

Open with DEXTER  
In the text 
Fig. 7
Evolution of semimajor axis and eccentricity for the five planets of 55 Cnc assuming the “nominal” tidal dissipation for 55 Cnc e and the initial conditions come from Dawson & Fabrycky (2010). Top panel: the semimajor axis is plotted in thick colored lines, the colored dashed lines represent the distance of aphelion and perihelion for each planet. The corotation radius is indicated by a black dashed line and the thick red dashed line is the stellar radius. Bottom panel: the colored full lines represent the eccentricities of the five planets, the dashed dotted lines represent the secular evolution 55 Cnc e (purple) and 55 Cnc b (blue) would experience if alone in the system. The thick red dashed line represent the critical eccentricity of planet e above which its secondary transit depth is increased by more than 10% by tidal heating. 

Open with DEXTER  
In the text 
Fig. 8
As Fig. 7 but assuming a dissipation factor of 10^{2} × σ_{p} for 55 Cnc e. 

Open with DEXTER  
In the text 
Fig. 9
As Fig. 7, but the initial conditions come from Endl et al. (2012). 

Open with DEXTER  
In the text 
Fig. 10
Eccentricity vs dissipation. The thick colored lines corresponds to the minimum, average and maximum eccentricity – bottom full line, middle dashed line and top full line – of 55 Cnc e obtained with the simulations of Dawson & Fabrycky (2010) in purple, and Endl et al. (2012) in blue. The horizontal black dashed line corresponds to the upper limit from observations (e = 0.06, D12). The color bands correspond to the region where the two conditions of Eq. (5) are met: where the tides contribute to more than 10% of the planet’s flux and where the resulting transit depth is between the observational constraints. The light orange band corresponds to an albedo of 0 and the red one to an albedo of 1. The orange dashed dotted lines delimit the band corresponding to an albedo of 0.65. 

Open with DEXTER  
In the text 