# The ARIEL mission reference sample

Tiziano Zingales, Giovanna Tinetti, Ignazio Pillitteri, J. Leconte, Giuseppina Micela, Subhajit Sarkar

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Tiziano Zingales, Giovanna Tinetti, Ignazio Pillitteri, J. Leconte, Giuseppina Micela, et al. The ARIEL mission reference sample. Experimental Astronomy, 2018, pp. Online First 2018. 10.1007/s10686-018-9572-7. hal-01730265

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# The ARIEL mission reference sample

Tiziano Zingales<fnref n="1" />,<fnref n="2" /> ID · Giovanna Tinetti<fnref n="1" /> ·

Ignazio Pillitteri<fnref n="2" /> · Jérémy Leconte<fnref n="3" /> ·

Giuseppina Micela<fnref n="2" /> · Subhajit Sarkar<fnref n="4" />

Received: 28 April 2017 / Accepted: 9 January 2018 / Published online: 28 February 2018

© The Author(s) 2018. This article is an open access publication

**Abstract** The ARIEL (Atmospheric Remote-sensing Exoplanet Large-survey) mission concept is one of the three M4 mission candidates selected by the European Space Agency (ESA) for a Phase A study, competing for a launch in 2026. ARIEL has been designed to study the physical and chemical properties of a large and diverse sample of exoplanets and, through those, understand how planets form and evolve in our galaxy. Here we describe the assumptions made to estimate an optimal sample of exoplanets – including already known exoplanets and expected ones yet to be discovered – observable by ARIEL and define a realistic mission scenario. To achieve the mission objectives, the sample should include gaseous and rocky planets with a range of temperatures around stars of different spectral type and metallicity. The current ARIEL design enables the observation of ~1000 planets, covering a broad range of planetary and stellar parameters, during its four year mission lifetime. This nominal list of planets is expected to evolve over the years depending on the new exoplanet discoveries.

**Keywords** Exoplanets · ARIEL space mission · Planetary population

<figure><img src="image_2.png" /></figure>

<footnote>Tiziano Zingales
tiziano.zingales.15@ucl.ac.uk</footnote>

<footnote n="1">¹ University College London, Gower St, Bloomsbury, London WC1E 6BT, UK</footnote>

<footnote n="2">² INAF - Osservatorio Astronomico di Palermo, London, UK</footnote>

<footnote n="3">³ Laboratoire d'Astrophysique de Bordeaux, CNRS, Université de Bordeaux, Bordeaux, Nouvelle-Aquitaine, France</footnote>

<footnote n="4">⁴ Cardiff University, Cardiff, UK</footnote>
# 1 Introduction

## 1.1 Mission overview

Today we know over 3700 exoplanets of which more than one third are transiting (http://exoplanets.eu/). These include Earths, super-Earths, Neptunes and Giant planets around a variety of stellar types. The Kepler space mission has discovered alone more than 1000 new transiting exoplanets between 2009 and 2015 and more than 3000 still unconfirmed planetary candidates.

The number of known exoplanets is expected to increase in the next decade thanks to current and future space missions (K2, GAIA, TESS, CHEOPS, PLATO) and a long list of ground-based surveys (e.g. HAT-NET, HARPS, WASP, MEarth, NGTS, TRAPPIST, Espresso, Carmenes). These facilities are expected to detect thousands of new transiting exoplanets.

ARIEL (Atmospheric Remote-sensing Exoplanet Large-survey) is one of the three candidate missions selected by the European Space Agency (ESA) for its next medium-class science mission due for launch in 2026. The goal of the ARIEL mission is to investigate the chemical composition of several hundred planets orbiting distant stars in order to address the fundamental questions on how planetary systems form and evolve. Key objective of the mission is to find out whether the chemical composition of exoplanetary atmospheres correlate with basic parameters such as the planetary size, density, temperature, and stellar type and metallicity. During its four-year mission, ARIEL aims at observing a statistically significant sample of exoplanets, ranging from Jupiter- and Neptune-size down to super-Earth and Earth-size in the visible and the infrared with its meter-class telescope. The analysis of ARIEL spectra and photometric data will allow to extract the chemical fingerprints of gases and condensates in the planets’ atmospheres, including the elemental composition for the most favorable targets. It will also enable the study of thermal and scattering properties of the atmosphere as the planet orbit around the star.

The main purpose of this paper is to estimate an optimal list of targets observable by ARIEL or a similar mission in the next decade and quantify a realistic mission scenario to be completed in 4 year nominal mission lifetime, including the commissioning phase.

To achieve the mission objectives, the sample should include gaseous and rocky planets with a range of temperatures around stars of different spectral type and metallicity. With this aim, it is necessary to consider both the already known exoplanets and the “expected” ones yet to be discovered. The data collected by Kepler allow to estimate the occurrence rate of exoplanets according to their size and orbital periods. Using this planetary occurrence rate and the number density of stars in the Solar neighbourhood, we can estimate the number of exoplanets expected to exist with a particular size, orbital period range and orbiting a star of a particular spectral type and metallicity. Here we describe the assumptions made to estimate an optimal sample of exoplanets observable by ARIEL and define the Mission Reference Sample (MRS). It is clear that this nominal list of planets will change over the years depending on the new exoplanetary discoveries.
In Section 2 we explain the method used to estimate the number and the parameters of the planetary systems yet to be discovered. All the potential ARIEL targets will be presented in Section 3, where we show all the planets that can be observed individually during the mission lifetime, and out of which we want to select the optimal sample. Section 4 is dedicated to the selection and description of an ARIEL MRS fulfilling the mission requirements, we compare the proposed ARIEL MRS to the sample expected to be discovered by TESS, confirming that TESS could provide a large fraction of the ARIEL targets. A sample including only planets known today is identified. In Section 5 we show a possible MRS which maximises the coverage of the planetary and stellar physical parameters.

## 1.2 Description of the models

We use the ESA Radiometric Model [13] to estimate the performances of the ARIEL mission given the planetary, stellar and orbital characteristics: namely the stellar type and brightness, the planetary size, mass, equilibrium temperature and atmospheric composition, the orbital period and eccentricity. This tool takes into account the mission instrumental parameters and planetary system characteristics to calculate:

- The SNR (Signal to Noise Ratio) that can be achieved in a single transit;

- The SNR that can be achieved in a single occultation;

- The number of transit/occultation revisits necessary to achieve a specified SNR;

- The total number and types of targets that can be included in the mission lifetime.

In this work, the list of planets considered as input to the radiometric model includes known and simulated exoplanets, as detailed in the following sections. We used the instrument parameters of the ARIEL payload as designed during the phase A study. To increase the efficiency of our simulations we used a Python tool as a wrap of the ESA Radiometric Model, so we could test different mission configurations that fulfil the mission science objectives. The results were validated with ExoSim, a time domain simulator used for the ARIEL space mission, but thanks to its modularity it can be used to study any transit spectroscopy instrument from space or ground. ExoSim has been developed by [11, 15, 16] (see Appendix A).

# 2 Simulations of planetary systems expected to be discovered in the next decade

## 2.1 Star count estimate

We used the stellar mass function as obtained from the 10-pc RECONS (REsearch Consortium On Nearby Stars) to estimate the number of stars as a function of the K magnitude. We assume mass-luminosity-K magnitude conversions from [1]. The same procedure was adopted by [14]. The number of main sequence stars with limit K-mag $m_K = 7$ used to infer the number density of stars in the Solar neighbourhood is shown in Table 1.
<table><caption>**Table 1** Star counts considering different spectral types with limiting magnitude $m_K = 7$</caption><thead><tr><th>Mass (M<sub>☉</sub>)</th><th>Spectral type</th><th>N<sub>*</sub> (K &lt; 7)</th></tr></thead><tbody><tr><td>1.25 – 1.09</td><td>F6 – F9</td><td>5646</td></tr><tr><td>1.09 – 0.87</td><td>G0 – G8</td><td>3356</td></tr><tr><td>0.87 – 0.65</td><td>K0 – K5</td><td>1167</td></tr><tr><td>0.65 – 0.41</td><td>K7 – M1</td><td>386</td></tr><tr><td>0.41 – 0.22</td><td>M2 – M3</td><td>81</td></tr><tr><td>0.22 – 0.10</td><td>M4 – late M</td><td>28</td></tr></tbody></table>

The number density (Table 2) and the number of stars are related through (1):

$$ \rho_* = \frac{N_*(K < 7)}{\frac{4}{3}\pi d^3} \qquad (1) $$

where the distance *d* has been calculated in the ARIEL Radiometric Model [13] using the relation between K magnitude *m*<sub>K</sub> and the distance *d*:

$$ m_K = -2.5 \log \frac{R_*^2 S_s (\Delta\lambda)}{d^2 S_0^K (\Delta\lambda)} \qquad (2) $$

In (2), $R_*$ is the stellar radius, $S_0^K (\Delta\lambda)$ is the zero point flux for the standard K-band filter profile, $\Delta\lambda$ is the filter band pass given in [4] and $S_s (\Delta\lambda)$ the stellar flux density evaluated over the same bandwidth. We neglect the interstellar absorption since our stars are at a relatively short distance.

## 2.2 Planetary population and occurrence rate

In this section we briefly review the current knowledge about the occurrence rate of planets, i.e. the average expected number of planets per star. Fressin et al. [5] used the Kepler statistics to publish the planetary occurrence rates around F, G, K main sequence stars ordered by orbital periods and planetary types. An accurate planetary occurrence rate is pivotal to the reliability of the estimate of the existing planets in the Solar neighbourhood. We used the planetary occurrence rate values for F,G,K stars from [5], being the most complete, i.e. covering all planetary types and stars. We have extended the same occurrence rates to M stars but, by doing that, we are

<table><caption>**Table 2** Main sequence star densities considering different spectral types with limiting magnitude $m_K = 7$</caption><thead><tr><th>Density</th><th>Star / pc<sup>3</sup></th></tr></thead><tbody><tr><td>ρ(F6–F9)</td><td>0.0039</td></tr><tr><td>ρ(G0–G8)</td><td>0.0044</td></tr><tr><td>ρ(K0–K5)</td><td>0.0049</td></tr><tr><td>ρ(K7–M1)</td><td>0.0074</td></tr><tr><td>ρ(M2–M3)</td><td>0.0059</td></tr><tr><td>ρ(M4 – late M)</td><td>0.0118</td></tr></tbody></table>
<figure><img src="image_3.png" /><figcaption>**Fig. 1** Average number of planets per star and per size bin with an orbital period shorter than 85 days orbiting around F, G, K stars. The statistics was extracted from the Q1 - Q6 Kepler data [5]</figcaption></figure>

effectively underestimating the number of planets with short period around M dwarfs in our sample (Fig. 1).

Mulders et al. [9] updated the planetary occurrence rate for planets between $0.5R_⊕$ and $4R_⊕$ and orbital period < 50 days, using a more recent list of planets discovered by the Kepler satellite. Figure 2 shows the comparison between [5, 9]. The differences between the two occurrence rates can be up to an order of magnitude. Mulders et al. [8] show that M stars have 3.5 times more small planets (1.0 – 2.8$R_⊕$) than F, G, K stars, but two times fewer Neptune-sized and larger (> 2.8$R_⊕$) planets. The fraction of M-stars considered in our work is only ~7% of the total stellar sample, so we are significantly underestimating the number of small planets around M-dwarfs, which are optimal targets for transit spectroscopy. More recent and complete occurrence rates are expected to be published in the next months. Given the discrepancy between Mulders and Fressin’s statistics we expect a substantial improvement in our estimates when the most recent Kepler statistics will become available. The recent papers by Fulton et al. [6] and Mayo et al. [7] confirm this expectations.

Fressin et al. [5] provided the following statistics for different planetary classes:

- Jupiters: $6R_⊕ < R_p \le 22R_⊕$

- Neptunes: $4R_⊕ < R_p \le 6R_⊕$

- Small Neptunes: $2R_⊕ < R_p \le 4R_⊕$

- Super Earths: $1.25R_⊕ < R_p \le 2R_⊕$

- Earths: $0.8R_⊕ < R_p \le 1.25R_⊕$

We adopted a size resolution of $1R_⊕$ in each of these classes.
<figure><img src="image_4.png" /><figcaption>**Fig. 2** Comparison of three different distributions estimating the planetary occurrence rate as a function of orbital period for planets between 0.5R<sub>⊕</sub> and 4R<sub>⊕</sub>. Blue and green lines: results from [9] for two metallicity classes. Red line: results from [5]. The [5] statistics strongly underestimates the occurrence of sub Neptune size planets compared to [9] and other more recent estimates. The reason is the large number of small planets discovered after 2013</figcaption></figure>

The number of planets can be estimated as:

$$N_p = \frac{4}{3} \pi d^3 \rho_* P_{t,p} P_{geom} \quad (3)$$

where *d* is the radius of a sphere with the Sun at the centre, *ρ*<sub>*</sub> is the number density of the stars, *P*<sub>*t*,p</sub> is the probability of having a t-type planet orbiting with an orbital period *p* (See Fig. 1). *P*<sub>geom</sub> = *R*<sub>*</sub>/<i>a</i> is the geometrical probability of a transit.

We simulated all the transiting planets in the solar neighbourhood up to *m*<sub>*K*</sub> = 14: all these planets described by *N*<sub>*p*</sub> constitute the “Mission Reference Population”.

To avoid duplications, every time we predicted a planet/star system with the same physical properties of a known one, we replaced it with the known one. In Section 3 we show that in the solar system neighbourhood there are ~ 9500 planets for which the ARIEL science requirements can be achieved in less that 6 transits or eclipses.

The equilibrium temperature (4) of the planet can be estimated assuming the incoming and outgoing radiation at the planetary surface are in equilibrium:

$$T_p = T_* \left( \frac{R_*}{2a} \right)^{\frac{1}{2}} \left( \frac{1 - A}{\varepsilon} \right)^{\frac{1}{4}} \quad (4)$$

Here *T*<sub>*</sub> and *R*<sub>*</sub> are the stellar temperature and radius, *a* the semi-major axis of the orbit, *A* is the planetary albedo and *ε* is the atmospheric emissivity.
The ARIEL space mission will focus on planets with an orbital period shorter than 50 days. As expected, shorter periods mean shorter semi-major axis and, therefore, from (4), typically warmer temperature.

## 2.3 Planetary masses and densities

To simulate a realistic planetary population we need to consider a distribution of plausible masses given a planetary radius. The planetary mass controls the surface gravity and therefore the scale height (H) of the atmosphere:

$$H = \frac{kT}{\mu g} \qquad (5)$$

Estimating the planetary mass is not a trivial task, given the range of planetary densities observed today. We used a Python tool written by [3] to estimate the mass of all the planets in our simulated sample. Chen and Kipping [3] use the currently known planets to derive the statistical distribution of the mass of a given planet when its radius is known. Thus, except for known systems, for each planet in our simulated sample the mass is randomly drawn following that distribution. In Fig. 3 we show the mass distribution for all the planets in our simulations. Moreover, as a very few planets have a radius larger than $20R_⊕$, we use that radius as an upper limit. There is

<figure><img src="image_5.png" /><figcaption>Fig. 3 Mass-Radius distribution for all the simulated planets. The mass-radius relationship has been calculated with the [3] tool</figcaption></figure>
<table><caption>**Table 3** Spectral range and spectral resolving power required for the ARIEL photometric and spectroscopic channels</caption><thead><tr><th colspan="3">ARIEL spectral coverage</th></tr><tr><th>Channel name</th><th>Wavelength (μm)</th><th>Resolving power</th></tr></thead><tbody><tr><td>VisPhot</td><td>0.5 – 0.55</td><td>Photometer</td></tr><tr><td>FGS-1</td><td>0.8 – 1.0</td><td>Photometer</td></tr><tr><td>FGS-2</td><td>1.05 – 1.2</td><td>Photometer</td></tr><tr><td>NIRSpec</td><td>1.25 – 1.95</td><td>R≥10</td></tr><tr><td>AIRS-Channel #0</td><td>1.95 – 3.9</td><td>R≥100</td></tr><tr><td>AIRS-Channel #1</td><td>3.9 – 7.8</td><td>R≥30</td></tr></tbody></table>

already a well known degeneracy in the 7 − 20R$_{⊕}$ range: objects with a radius within that range can be planets as well as very cool stars. However, this should not be too concerning, as observations have shown that very short-period, low-mass stellar companions are much less frequent than hot giant planets [12].

# 3 ARIEL science goals and mission reference population

## 3.1 The 3 tier approach

The ARIEL primary science objectives call for atmospheric spectra or photometric lightcurves of a large and diverse sample of known exoplanets covering a wide range of masses, densities, equilibrium temperatures, orbital properties and host stars. Other science objectives require, by contrast, the very deep knowledge of a select sub-sample of objects. To maximise the science return of ARIEL and take full advantage of its unique characteristics, a three-tiered approach has been considered, where three different samples are observed at optimised spectral resolutions, wavelength intervals and signal-to-noise ratios. A summary of the three-tiers and observational methods is given below in Tables 3 and 4.

In this section we present the pool of potential targets that could reach the specifications for each tier with a reasonable number of transit/eclipse events. The number of targets for the various Tiers are shown as a function of planetary radius in Figs. 4, 6 and 8 and as a function of effective temperature in 5, 7 and 9. Note that the planets shown in these figures do not represent the final sample, as it would take too

<table><caption>**Table 4** Summary of the survey tiers and the observational strategy required to accomplish them. Each tier will use a % of the nominal mission lifetime, as indicated in the left column</caption><thead><tr><th colspan="2">ARIEL 3-tiers</th></tr></thead><tbody><tr><td>Survey (~37%)</td><td>Low spectral resolution observations (R ≥ 10 across all channels) of a large sample of planets in the Vis-IR, with SNR ≥ 7.</td></tr><tr><td>Deep (~60%)</td><td>Intermediate spectral resolution observations (R > 50 in AIRS channel 0 and R > 15 in AIRS channel 1) of a sub-sample in the VIS-IR.</td></tr><tr><td>Benchmark (~3%)</td><td>Very best planets, re-observed multiple time with all techniques. Full spectral resolution.</td></tr></tbody></table>
<figure><img src="image_6.png" /><figcaption>**Fig. 4** Complete set of Tier 1 planets from the ARIEL mission reference population. The final list of Tier 1 planets will include an optimal sub-sample. Different colours indicate the number of transits/eclipses needed to reach Tier 1 performances. The planets shown here can achieve the Tier 1 requirements combining the signal of ≤ 5 transits/eclipses</figcaption></figure>

long to observe all of them. They are the pool from which the MRS can be selected to best address the scientific questions summarized below. The fact that the number of potential targets is much larger than the number that can be observed illustrates that ARIEL can choose the final sample among a great variety of observable planets, providing a lot a flexibility.

In Table 3 we show the spectral coverage and the resolving power of the ARIEL photometric and spectroscopic sensors. In Table 4 we report a summary of the three tiers and the observational strategy.

**3.2 Key science questions**

The key questions and objectives of each tier can be summarised as follows (see Tinetti et al., submitted for further details):

**Survey:**

- *What fraction of planets are covered by clouds?* – Tier 1 mode is particularly useful for discriminating between planets that are likely to have clear atmospheres, versus those that are so cloudy that no molecular absorption features are visible in transmission. Extremely cloudy planets may be identified simply

<figure><img src="image_7.png" /><figcaption>**Fig. 5** Temperature distribution for the planets illustrated in Fig. 4</figcaption></figure>
from low-resolution observations over a broad wavelength range. This preliminary information will therefore allow us to take an informed decision about whether to continue the spectral characterization of the planet at higher spectral resolution, and therefore include or not the planet in the Tier 2 sample.

- What fraction of small planets have still hydrogen and helium retained from the protoplanetary disk? – Primordial (primary atmosphere) atmospheres are expected to be mainly made of hydrogen and helium, i.e. the gaseous composition of the protoplanetary nebula. If an atmosphere is made of heavier elements, then the atmosphere has probably evolved (secondary atmosphere). An easy way to distinguish between primordial (hydrogen-rich) and evolved atmospheres (metal-rich), is to examine the transit spectra of the planet: the main atmospheric component will influence the atmospheric scale height, thus changing noticeably the amplitude of the spectral features. This question is essential to understand how super-Earths formed and evolved.

- Can we classify planets through colour-colour diagrams or colour-magnitude diagrams? – Colour-colour or colour-magnitude diagrams are a traditional way of comparing and categorising luminous objects in astronomy. Similarly to the Herzsprung-Russell diagram, which led to a breakthrough in understanding stellar formation and evolution, the compilation of similar diagrams for exoplanets might lead to similar developments [18].

- What is the bulk composition of the terrestrial exoplanets? – The planetary density may constrain the composition of the planet interior. However this measurement alone may lead to non-unique interpretations [19]. A robust determination of the composition of the upper atmosphere of transiting planets will reveal the extent of compositional segregation between the atmosphere and the interior, removing the degeneracy originating from the uncertainty in the presence and mass of their (inflated?) atmospheres.

- What is the energy balance of the planet? – Eclipse measurements in the optical and infrared can provide the bulk temperature and albedo of the planet, thereby allowing the estimation of the planetary energy balance and whether the planet has an internal heat source or not.

**Deep:**

A key objective of ARIEL is to understand whether there is a correlation between the chemistry of the planet and basic parameters such as planetary size, density, temperature and stellar type and metallicity. Spectroscopic measurements at higher resolution will allow in particular to measure:

- The main atmospheric component for small planets;

- The chemical abundances of trace gases, which is pivotal to understand the type of chemistry (equilibrum/non equilibrium).

- The atmospheric thermal structure, both vertical and horizontal;

- The cloud properties, i.e. cloud particles size and distribution,

- The elemental composition in gaseous planets. This information can be used to constrain formation scenarios [10].

**Benchmark:**
<figure><img src="image_8.png" /><figcaption>**Fig. 6** Planets from the ARIEL mission reference population in the Deep mode (Tier 2) with a small/moderate number of transits/eclipses, divided in size bins. The final list of Tier 2 planets will include an optimal sub-sample. Different colours indicate the number of transits/eclipses needed to reach Tier 2 performances</figcaption></figure>

A fraction of planets around very bright stars will be observed repeatedly through time to obtain:

- A very detailed knowledge of the planetary chemistry and dynamics;

- An understanding of the weather, and the spatial and temporal variability of the atmosphere.

Benchmark planets are the best candidates for phase-curve spectroscopic measurements.

## 3.3 Target samples

In this section we discuss a number of lists of potential targets for ARIEL: these are expected to evolve until launch and will be updated regularly to include new planet discoveries.

ARIEL Tier 1 (Survey) will analyse a large sample of exoplanets to address science questions where a statistically significant population of objects needs to be observed. ARIEL Tier 1 will also allow a rapid, broad characterisation of planets permitting a more informed selection of Tier 2 and Tier 3 planetary candidates. For

<figure><img src="image_9.png" /><figcaption>**Fig. 7** Temperature distribution for the planets illustrated in Fig. 6</figcaption></figure>
<figure><img src="image_10.png" /><figcaption>**Fig. 8** Number of planets from the mission reference population observable by ARIEL in the Benchmark mode with a < 25 number of transits/eclipses, divided in size bins. Different colours indicate the number of transits/eclipses needed to reach Tier 3 performances</figcaption></figure>

most Tier 1 planetary candidates, Tier 1 performances can be reached between 1 and 2 transits/eclipses. In Figs. 4 and 5 we show that in the solar system neighbourhood there are ~9500 observable by ARIEL for which the science requirements can be reached in less that 6 transits or eclipses.

ARIEL Tier 2 (Deep, the core of the mission) will analyse a sub-sample of Tier 1 planets with a higher spectral resolution, allowing an optimal characterisation of the atmospheres, including information on the thermal structure, abundance of trace gases, clouds and elemental composition.

In Figs. 6 and 7 we show the properties of all the planetary candidates that could be studied by ARIEL in the Deep mode with a small/moderate number of transit or eclipse events.

The third ARIEL Tier (Benchmark, the reference planets) will study the best planets (Section 4.3), i.e. the ones orbiting very bright stars which can be studied in full spectral resolution with a relatively small number of transits/eclipses. For the planets observed in benchmark mode in 1 or 2 events, it is possible to study the spatial and temporal variability (i.e. study the weather and evaluate its impact when observations are averaged over time). In Figs. 8 and 9 we show the properties of the Tier 3 planetary candidates.

<figure><img src="image_11.png" /><figcaption>**Fig. 9** Temperature distribution for the planets illustrated in Fig. 8</figcaption></figure>
<figure><img src="image_12.png" /><figcaption>**Fig. 10** Overview of the ARIEL MRS, comparing the number of planets observable in the three tiers during the mission lifetime</figcaption></figure>

# 4 A possible scenario for the ARIEL space mission

In Section 3 we presented a comprehensive list of planet candidates which could be observed with the ARIEL space mission. Here we discuss possible optimisations of the Mission Reference Sample, which ideally should include a large and diverse sample of planets, have the right balance among the three Tiers and, most importantly, must be completed during the nominal mission lifetime (4 years including the commissioning phase).

In Fig. 10 we show a possible MRS with all the three tiers nested together. This MRS is optimised to yield the maximum number of targets, taking into account the nominal mission lifetime. It has been built starting from all the targets feasible within one transit/eclipse, and adding all the targets that can be done within 2, 3, 4 and so on transits/eclipses in ascending order. This is just one of the possible configurations for the MRS, and one would expect the ARIEL MRS to evolve in response of new exoplanetary discoveries in the next decade.

## 4.1 MRS tier 1: survey

Our simulations indicate that the current ARIEL design as presented at the end of the Phase A study, allows to observe 1002 planets in Tier 1. All the planets can be

<figure><img src="image_13.png" /><figcaption>**Fig. 11** ARIEL MRS Tier 1 planets organised in size-bins. Different colours indicate the number of transits/eclipses needed to reach Tier 1 performances</figcaption></figure>
<figure><img src="image_14.png" /><figcaption>**Fig. 12** ARIEL MRS Tier 1 planets organised in temperature-bins. Different colours indicate the number of transits/eclipses needed to reach Tier 1 performances</figcaption></figure>

observed during 37% of the mission lifetime. Most giant planets and Neptunes fulfil the Tier 1 science objectives in 1 transit/eclipse, the smaller planets require up to 6 events (Figs. 11 and 12). Figures 13 and 14 illustrate how the 1002 planets are distributed in terms of planetary size, temperature, density and stellar type.

## 4.2 MRS tier 2: deep

The Deep is the core of the mission. Our simulations indicate that the current ARIEL design as presented at the end of the Phase A study, allows to observe ~500 planets in Tier 2 assuming 60% of the mission lifetime. Most Gaseous planets fulfil the Tier 2 science objectives in less than five transits/eclipses, the small planets require up to twenty events (Figs. 15 and 16). Figures 17 and 18 illustrate how the 500 planets are distributed in terms of planetary size, temperature, density and stellar type.

We included a variety of planets from cold (300 K) to very hot (2500 K) as shown in Fig. 16. We scheduled also ~50 planets that will be studied with both transit and eclipse methods, indicated by stripes in Fig. 15). These are the best candidates for

<figure><img src="image_15.png" /><figcaption>**Fig. 13** ARIEL MRS Tier 1 planets organised in size-bins. Different colours indicate differences in the simulated planetary densities</figcaption></figure>
<figure><img src="image_16.png" /><figcaption>**Fig. 14** ARIEL MRS Tier 1 planets organised in temperature-bins. Different colours indicate differences in the simulated stellar temperatures</figcaption></figure>

phase-curves observations, which can be included at the expenses of the number of
Tier 2 planets observed.

**4.3 MRS tier 3: benchmark**

In the current MRS, we have selected as Tier 3, 67 gaseous planets for weather stud-
ies. Figure 19 shows the temperature distribution covered by the Tier 3 sample. Only
3% of the mission lifetime is required to achieve the Tier 3 science objectives for this
sample.

4.4 Compliance with TESS expected yields

The Transiting Exoplanet Survey Satellite (TESS) is expected to provide a large frac-
tion of the targets observable by ARIEL. The numbers of targets envisioned in the
sample presented here are perfectly in line with the expected yield from The Transit-
ing Exoplanet Survey Satellite (TESS), as shown in Fig. 20 where we compare the
expected TESS discoveries and the ARIEL MRS. We see that the ARIEL MRS is

<figure><img src="image_17.png" /><figcaption>**Fig. 15** ARIEL MRS Tier 2 planets organised in size-bins. Different colours indicate the number of transits/eclipses needed to reach Tier 2 performances. Stripes indicate planets that will be studied with both transit and eclipse methods</figcaption></figure>
<figure><img src="image_18.png" /><figcaption>**Fig. 16** ARIEL MRS Tier 2 planets organised in temperature-bins. Different colours indicate the number of transits/eclipses needed to reach Tier 2 performances</figcaption></figure>

<figure><img src="image_19.png" /><figcaption>**Fig. 17** ARIEL MRS Tier 2 planets organised in size-bins. Different colours indicate differences in the simulated planetary densities</figcaption></figure>

<figure><img src="image_20.png" /><figcaption>**Fig. 18** ARIEL MRS Tier 2 planets organised in temperature-bins. Different colours indicate differences in the simulated stellar temperatures</figcaption></figure>

<figure><img src="image_21.png" /></figure>
<figure><img src="image_22.png" /><figcaption>**Fig. 19** Temperature distribution of the planets observable by ARIEL in the Benchmark</figcaption></figure>

<figure><img src="image_23.png" /><figcaption>**Fig. 20** Comparison between the TESS targets [17] and the ARIEL MRS (green bars)</figcaption></figure>

<figure><img src="image_24.png" /><figcaption>**Fig. 21** ARIEL MRS with currently available planets radius distribution</figcaption></figure>
<figure><img src="image_25.png" /><figcaption>**Fig. 22** ARIEL MRS with currently available planets temperature distribution</figcaption></figure>

<figure><img src="image_26.png" /><figcaption>**Fig. 23** ARIEL MRS with currently available planets density distribution</figcaption></figure>

<figure><img src="image_27.png" /><figcaption>**Fig. 24** Temperature distribution of the stellar hosts for the planets shown in Fig. 21</figcaption></figure>

<figure><img src="image_28.png" /></figure>
<figure><img src="image_29.png" /><figcaption>**Fig. 25** Metallicity distribution of the stellar hosts for the planets shown in Fig. 21</figcaption></figure>

well within the TESS sample [17]. The success of the TESS mission will allow the
characterisation of hundreds of planets by ARIEL.

**4.5 ARIEL MRS with currently known targets**

In February 2017 ~ 210 transiting planets fulfill the ARIEL previous criteria. It means
that, even if ARIEL were launched tomorrow, it would observe at least 210 relevant

<figure><img src="image_30.png" /><figcaption>**Fig. 26** Planets known today and observable by ARIEL in Deep mode, distributed in size-bins (top) and temperature bins (bottom) – 158 planets</figcaption></figure>
<figure><img src="image_31.png" /><figcaption>**Fig. 27** Planets known today and observable by ARIEL in Benchmark mode, distributed size-bins (**top**) and temperature bins (**bottom**) – 67 planets</figcaption></figure>

<figure><img src="image_32.png" /><figcaption>**Fig. 28** A plot illustrating the fraction of the year for which a given location in the sky (in equatorial coordinates) is visible to ARIEL, as seen from a representative operational orbit of ARIEL at L2. Yellow dots: planets observed in Tier 1. Red dots: planets observed in Tier 2. Green dots: planets observed in Tier 3. (Marc Ollivier, private communication)</figcaption></figure>

<figure><img src="image_33.png" /></figure>
targets. Using the planets known today, we could organise the MRS into the following three tiers:

- Survey: 210 planets using 30% of the mission lifetime (Fig. 21);

- Deep: 158 planets using 60% of the mission lifetime (Fig. 26);

- Benchmark: 67 planets using 10% of the mission lifetime (Fig. 27).

In Figs. 21, 22 and 23 we show the key physical parameters of the known planets defining the current observable MRS current MRS. In Figs. 24 and 25 we show the properties of the stellar hosts. A possible deep and benchmark mode configuration is shown, respectively, in Figs. 26 and 27. As mentioned previously, the number of known planets is expected to increase dramatically in the future.

Pictorial representation (M. Ollivier, private comm.) of the known planets sky coordinates and their sky visibility all over the year is given in Fig. 28. It shows that

<figure><img src="image_34.png" /><figcaption>**Fig. 29** Distribution of the 9545 planets in the 4D space of $T_{\text{eff}}$, [Fe/H], $R_{\text{pl}}$, $T_{\text{pl}}$. Above each panels we indicate the spectral type and metallicity. The numbers in each cell are the numbers of planets with the corresponding properties. The colour scale indicates more populated cells (darker orange/brown). Grey cells without any number indicate no objects</figcaption></figure>
objects far away from the ecliptic plane will be visible longer than the planet close to this plane.

# 5 MRS optimisation for stellar hosts

In this section we show another possible selection of the Tier 1 sample that maximises also the diversity of stellar hosts, additionally to other planet parameters. In particular, the stellar metallicity is expected to play an important role in the planet formation process and type of chemistry of the planet [20]. ARIEL will also collect important data to test the possible correlations between stellar metallicity and planetary characteristics.

## 5.1 Method

We will limit our analysis to those systems which can be studied in up to six visits for each planet (either a transit or an occultation).

We chose four physical quantities that define a 4D space to distribute the ARIEL targets. The quantities are: stellar effective temperature ($T_{eff}$), metallicity ([Fe/H]), planetary radius ($R_{pl}$) and planetary theoretical equilibrium temperature ($T_{pl}$) (Fig. 29). For the metallicity we use the values observed in the solar neighbourhood and reported by [2]. We adopt three bins for stellar $T_{eff}$, [Fe/H] and planetary $R_{pl}$, while for the $T_{pl}$ we use five bins, as detailed in Table 5. The three $T_{eff}$ bins correspond approximately to the ranges of spectral types M-Late / K stars, Early K-G stars and F-G stars, respectively, as indicated in the labels in Figs. 30, 31 and 32. Analogously, we separated the sample in low metallicity, solar metallicity and high metallicity, according to individual temperature values. The binning into 3 intervals of $T_{eff}$, [Fe/H] and $R_{pl}$ is a reasonable trade-off between a detailed representation of the sample and a simple visualization of the richness and diversity of the physical configurations of the sample. We inferred from [2] that the metallicities of stars in the solar neighbourhood are consistent with a normal distribution with mean -0.1 and standard deviation sd=0.2. Using such model distribution we simulated the values of [Fe/H] for each star in the ARIEL sample.

<table><caption>**Table 5** Bins of $T_{eff}$, [Fe/H], $R_{pl}$, $T_{pl}$ defining the 4D parameter space</caption><tr><td>Stellar Temp.: $T_{eff}$</td><td>3000 &lt; $T$ (K) &lt; 4100</td><td>4100 &lt; $T$ (K) &lt; 5800</td><td>$T$ &gt; 5800K</td></tr><tr><td>Labels</td><td>M-Late K</td><td>Early K-G</td><td>F-G</td></tr><tr><td>Metallicity: [Fe/H]</td><td>[Fe/H] &lt; -0.15</td><td>-0.15 &lt; [Fe/H] &lt; 0.15</td><td>[Fe/H] &gt; 0.15</td></tr><tr><td>Labels</td><td>Low [Fe/H]</td><td>Solar</td><td>High [Fe/H]</td></tr><tr><td>Planet Radius: $R_{pl}$</td><td>$R_{pl}$ &lt; 3R<sub>⊕</sub></td><td>3 &lt; $R_{pl}$ &lt; 8</td><td>$R_{pl}$ &gt; 8R<sub>⊕</sub></td></tr><tr><td>Labels</td><td>Earths/ Super Earths</td><td>Neptunes</td><td>Jupiters</td></tr><tr><td>Planet Temp.: $T_{pl}$</td><td>contiguous bins: [250, 500, 800, 1200, 1600, 2600] K</td><td></td><td></td></tr></table>
<figure><img src="image_35.png" /><figcaption>**Fig. 30** Same as Fig. 29 1002 planets of the Mission Reference Sample</figcaption></figure>

The 4D space of $T_{\text{eff}}$, [Fe/H], $R_{\text{pl}}$ and $T_{\text{pl}}$ is composed by a total of 3 × 3 × 3 × 5 = 135 cells. We assume that 10 systems are sufficiently reliable to determine the properties of the atmospheres of planets in each cell.

## 5.2 Results

The population of 9545 planets is distributed in the 4-D bins as in Fig. 29.

From this distribution we selected 1002 exoplanets, requiring altogether 1538 satellite visits. These 1002 planets are distributed in the 4D space as shown in Fig. 30. The 3 × 3 panel grid distributes the sample along the 3 spectral types and the metallicity ranges reported in Table 5. Each panel is a matrix with planetary radii along x-axis and (calculated) equilibrium temperatures along y-axis, as specified in Table 5 and discussed above. The numbers in each box identify the numbers of systems with the corresponding $R_{\text{pl}}$, $T_{\text{pl}}$, spectral type, and [Fe/H] values.
The 1002 systems in Fig. 30 tend to populate the cells corresponding to F-G-early and K stars orbited by Neptunes/Jupiters size planets (with a number of planets per cell $N > 20$), as these systems are the easiest to be observed with high signal to noise and, on average, with one or two visits. At the same time, planets around M or late K stars are much less represented in this distribution, especially planets smaller than Neptunes. This issue was identified in the previous sections as a result of extending the occurrence rate for F, G, K to M stars and it can be addressed by prioritising these targets over the rest of the population. We selected 908 planets and, in particular, 594 of them require only 1 visit (65.4%), 151 planets require 2 visits (16.6%), 83 planets require 3 visits (9.1%), 41 planets require 4 visits (4.5%), and 39 planets require 5 visits (4.4%). The corrected sample is shown in Fig. 31, where now ~ 19% of the population are Earths/Super Earth or Neptunes around M or K stars observable with less than 6 visits.

<figure><img src="image_36.png" /><figcaption>**Fig. 31** Same as Fig. 30 for the selected sample of 908 known and simulated planetary systems. They have been selected by filling each cell with up to 10 objects and for a budget of total satellite visits of about 1500</figcaption></figure>
Assuming a total number of visits as in the 1002 planets configuration (approximately 1500 visits), we fixed the maximum number of systems (10 planets in our choice) in each 4D space cell. This choice implies that any additional targets in an “already full” cell will be discarded. In this way we can include planets in the empty or poorly populated parts of the parameter space. The goal is to verify that we can cover with enough statistics most of the 4D parameter space. The distribution of systems selected with such criteria is shown in Fig. 31. Compared to Fig. 30, we see that we can efficiently cover most of the 4D space in planetary sizes, planetary temperatures, host temperatures and metallicities, apart from those combination of parameters corresponding to not physical or rare systems (e.g., very hot planets around very cool stars). Our selection is composed by 908 unique planets requiring a total of 1504 visits. Among already known systems, 92 of the initial 211 systems are in this new list. This selection is not unique, and depends on our choices, but our exercise shows that we have great freedom on the final choice on how to spend ARIEL observing time, as it can be easily tuned on specific needs.

<figure><img src="image_37.png" /><figcaption>**Fig. 32** Average number of visits required for the sample selected in Fig. 31. The binning is as in Figs. 30 to 31</figcaption></figure>
Figure 32 shows the average number of visits required to cover each cell of the 4D space. The number of visits needed for Jupiters and Neptunes is, typically, one or two, while Earths/Super Earths require from 3 to 5 visits each. To summarise, out of the 908 planets in our selection there are 594 planets requiring only 1 visit (65.4%), 151 planets requiring 2 visits (16.6%), 83 planets requiring 3 visits (9.1%), 41 planets requiring 4 visits (4.5%), and 39 planets requiring 5 visits (4.4%).

As a final comment, we have verified that, by increasing the maximum number of systems per 4D cell while keeping fixed the total number of visits to ~ 1500, we obtain that the number of observed planets increases (for example assuming N=15 as maximum systems per cell, we can observe up to 1000 systems), but at the same time the 4D cells of systems with cold/warm Earths/Super Earths would tend to be left empty and thus unexplored. This exercise shows the degree of flexibility offered by ARIEL in the choice of the target sample.

# 6 Conclusions

In this paper we demonstrated that the current ARIEL design enables the observation of 900-1000 planets during its four-year lifetime, depending on the physical parameters of the planet/star systems which one wants to optimise. The optimal sample of targets fulfils all the science objectives of the mission. While we currently know only ~200 transiting exoplanets which could be part of the mission reference sample, new space missions and ground-based observatories are expected to discover thousands of new planets in the next decade. NASA-TESS alone is expected to deliver most ARIEL targets.

**Acknowledgements** T. Z. is supported by the European Research Council ERC projects ExoLights (617119) and from INAF trough the “Progetti Premiali” funding scheme of the Italian Ministry of Education, University, and Research. I.P and G.M. are supported by Ariel ASI-INAF agreement No. 2015-038-R.O. We thank Enzo Pascale and Ludovig Puig for their help in setting up the ESA’s Radiometric model.

**Open Access** This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

# Appendix A: ESA Radiometric Model validation with ExoSim

We compare the out-of-transit signal and noise from ESA Radiometric Model (ERM) with that from ExoSim. An early version of ARIEL with a grating design was used for the instrument model in each. We model 55 Cancri and GJ 1214 with the same PHOENIX spectra in each simulator and include only photon noise and the noise floor, $N_{min}(\lambda)$, which is dominated by dark current noise. All the calculations are done per unit time and per spectral bin ($R = 30$ in Ch1 and $R = 100$ in Ch0). The noise variance was compared assuming an aperture mask on the final images, and the
<figure><img src="image_38.png" /><figcaption>Fig. 33 Comparison between the out-of-transit signal (left) and noise (right) simulated by ExoSim (white points) and the ESA Radiometric Model (blue points) for the star 55 Cancri. Subplots show the percent difference of the ERM from ExoSim</figcaption></figure>

noiseless signal per unit time was compared assuming no aperture. In the ERM, we use the following expression for $N_{min}$ giving the noise variance:

$$N_{min}(\lambda) = \frac{2.44 f \lambda^2}{m R \Delta_{pix}^2} I_{dc} \quad (6)$$

where $I_{dc}$ is the dark current per pixel, $m$ is the reciprocal linear dispersion of the spectrum in µm wavelength per µm distance, $R$ is the spectral resolving power and $\Delta_{pix}$ is the pixel pitch. The ExoSim noise variance results are the mean results from 50 simulations, with the standard deviations shown as error bars in the following figures. For 55 Cancri e case (Fig. 33), over all wavelength bins, the ERM signal is always within 2% of ExoSim, and the averaged noise variance within 5% of the ERM. In 94% of the bins, the ERM noise variance is within the standard deviation from ExoSim.

For GJ 1214 (Fig. 34), the ERM signal is within 4% of ExoSim over all bins and the averaged noise variance within 6% of ExoSim over all bins. The ERM noise variance is always within the standard deviation from ExoSim over all bins.

There is therefore good agreement between the two simulators.

<figure><img src="image_39.png" /><figcaption>Fig. 34 Comparison between the out-of-transit signal (left) and noise (right) simulated by ExoSim (white points) and the ESA Radiometric Model (blue points) for the star GJ 1214. Subplots show the percent difference of the ERM from ExoSim</figcaption></figure>
Appendix B: Known planets observable by ARIEL

<table><caption>**Table 6** List of known planets observable by ARIEL. The former to last column represents the number of transits/eclipses necessary to fulfil the ARIEL Tier 1 goals</caption><thead><tr><th rowspan="2">#</th><th rowspan="2">Planet</th><th colspan="4">Planetary properties</th><th colspan="2">Stellar properties</th><th rowspan="2">Observation</th></tr><tr><th>R (R<sub>⊕</sub>)</th><th>M (M<sub>⊕</sub>)</th><th>P (days)</th><th>T (K)</th><th>R (R<sub>☉</sub>)</th><th>T (K)</th><th>#</th><th>Type</th></tr></thead><tbody><tr><td>1</td><td>55 Cnc e</td><td>1.88</td><td>8.07</td><td>0.74</td><td>1891</td><td>0.95</td><td>5196</td><td>1</td><td>transit</td></tr><tr><td>2</td><td>EPIC 204129699 b</td><td>15.47</td><td>563.97</td><td>1.26</td><td>1473</td><td>0.91</td><td>5280</td><td>1</td><td>transit</td></tr><tr><td>3</td><td>WASP-52 b</td><td>13.94</td><td>146.24</td><td>1.75</td><td>1267</td><td>0.87</td><td>5000</td><td>1</td><td>transit</td></tr><tr><td>4</td><td>HD 189733 A b</td><td>12.49</td><td>361.78</td><td>2.22</td><td>1180</td><td>0.80</td><td>4980</td><td>1</td><td>transit</td></tr><tr><td>5</td><td>WASP-77 A b</td><td>13.28</td><td>559.52</td><td>1.36</td><td>1762</td><td>1.00</td><td>5500</td><td>1</td><td>transit</td></tr><tr><td>6</td><td>WASP-85 A b</td><td>16.24</td><td>387.85</td><td>2.66</td><td>1341</td><td>1.04</td><td>5685</td><td>1</td><td>transit</td></tr><tr><td>7</td><td>WASP-33 b</td><td>15.78</td><td>1459.19</td><td>1.22</td><td>2541</td><td>1.50</td><td>7200</td><td>1</td><td>occultation</td></tr><tr><td>8</td><td>WASP-19 b</td><td>15.21</td><td>371.32</td><td>0.79</td><td>1998</td><td>0.97</td><td>5500</td><td>1</td><td>occultation</td></tr><tr><td>9</td><td>WASP-95 b</td><td>13.28</td><td>359.23</td><td>2.18</td><td>1521</td><td>1.11</td><td>5630</td><td>1</td><td>transit</td></tr><tr><td>10</td><td>WASP-121 b</td><td>19.83</td><td>376.08</td><td>1.27</td><td>2295</td><td>1.35</td><td>6459</td><td>1</td><td>transit</td></tr><tr><td>11</td><td>WASP-12 b</td><td>19.05</td><td>446.34</td><td>1.09</td><td>2399</td><td>1.35</td><td>6118</td><td>1</td><td>occultation</td></tr><tr><td>12</td><td>WASP-35 b</td><td>14.48</td><td>228.89</td><td>3.16</td><td>1414</td><td>1.07</td><td>5990</td><td>1</td><td>transit</td></tr><tr><td>13</td><td>HAT-P-30 b</td><td>14.70</td><td>226.03</td><td>2.81</td><td>1594</td><td>1.24</td><td>6304</td><td>1</td><td>transit</td></tr><tr><td>14</td><td>WASP-108 b</td><td>14.09</td><td>283.57</td><td>2.68</td><td>1558</td><td>1.17</td><td>6000</td><td>2</td><td>transit</td></tr><tr><td>15</td><td>HD 209458 b</td><td>15.14</td><td>226.99</td><td>3.52</td><td>1401</td><td>1.15</td><td>6075</td><td>1</td><td>transit</td></tr><tr><td>16</td><td>WASP-122 b</td><td>21.64</td><td>436.17</td><td>1.71</td><td>1900</td><td>1.40</td><td>5720</td><td>1</td><td>transit</td></tr><tr><td>17</td><td>WASP-2 A b</td><td>12.26</td><td>290.57</td><td>2.15</td><td>1276</td><td>0.89</td><td>5255</td><td>2</td><td>transit</td></tr><tr><td>18</td><td>HAT-P-32 b</td><td>22.35</td><td>299.15</td><td>2.15</td><td>1850</td><td>1.18</td><td>6207</td><td>1</td><td>transit</td></tr><tr><td>19</td><td>WASP-43 b</td><td>11.37</td><td>646.62</td><td>0.81</td><td>1403</td><td>0.72</td><td>4520</td><td>1</td><td>occultation</td></tr><tr><td>20</td><td>WASP-123 b</td><td>14.56</td><td>292.47</td><td>2.98</td><td>1477</td><td>1.21</td><td>5740</td><td>1</td><td>transit</td></tr><tr><td>21</td><td>WASP-101 b</td><td>15.47</td><td>158.95</td><td>3.59</td><td>1518</td><td>1.34</td><td>6400</td><td>1</td><td>transit</td></tr><tr><td>22</td><td>WASP-74 b</td><td>17.12</td><td>302.01</td><td>2.14</td><td>1872</td><td>1.48</td><td>5990</td><td>1</td><td>transit</td></tr><tr><td>23</td><td>WASP-76 b</td><td>20.08</td><td>292.47</td><td>1.81</td><td>2125</td><td>1.46</td><td>6250</td><td>1</td><td>transit</td></tr><tr><td>24</td><td>WASP-1 b</td><td>16.27</td><td>271.49</td><td>2.52</td><td>1777</td><td>1.24</td><td>6160</td><td>1</td><td>occultation</td></tr><tr><td>25</td><td>KELT-10 b</td><td>15.35</td><td>215.86</td><td>4.17</td><td>1340</td><td>1.11</td><td>5948</td><td>1</td><td>transit</td></tr><tr><td>26</td><td>KELT-3 b</td><td>14.90</td><td>464.78</td><td>2.70</td><td>1774</td><td>1.28</td><td>6304</td><td>1</td><td>transit</td></tr><tr><td>27</td><td>WASP-62 b</td><td>15.25</td><td>181.21</td><td>4.41</td><td>1389</td><td>1.25</td><td>6230</td><td>1</td><td>transit</td></tr><tr><td>28</td><td>HD 149026 b</td><td>7.88</td><td>113.17</td><td>2.88</td><td>1699</td><td>1.30</td><td>6147</td><td>1</td><td>transit</td></tr><tr><td>29</td><td>WASP-97 b</td><td>12.40</td><td>419.64</td><td>2.07</td><td>1500</td><td>1.12</td><td>5640</td><td>2</td><td>occultation</td></tr><tr><td>30</td><td>WASP-94 A b</td><td>18.87</td><td>143.69</td><td>3.95</td><td>1464</td><td>1.29</td><td>6170</td><td>1</td><td>transit</td></tr><tr><td>31</td><td>HAT-P-8 b</td><td>14.50</td><td>405.33</td><td>3.08</td><td>1687</td><td>1.19</td><td>6200</td><td>1</td><td>occultation</td></tr><tr><td>32</td><td>WASP-54 b</td><td>18.14</td><td>202.19</td><td>3.69</td><td>1531</td><td>1.15</td><td>6100</td><td>1</td><td>transit</td></tr><tr><td>33</td><td>WASP-109 b</td><td>15.83</td><td>289.30</td><td>3.32</td><td>1729</td><td>0.91</td><td>6520</td><td>1</td><td>transit</td></tr><tr><td>34</td><td>HAT-P-41 b</td><td>18.49</td><td>254.33</td><td>2.69</td><td>1886</td><td>1.42</td><td>6390</td><td>1</td><td>transit</td></tr><tr><td>35</td><td>HAT-P-13 b</td><td>14.05</td><td>270.22</td><td>2.92</td><td>1600</td><td>1.22</td><td>5638</td><td>1</td><td>transit</td></tr><tr><td>36</td><td>KELT-15 b</td><td>15.83</td><td>289.30</td><td>3.33</td><td>1500</td><td>1.18</td><td>6003</td><td>2</td><td>transit</td></tr><tr><td>37</td><td>KELT-7 b</td><td>16.82</td><td>406.92</td><td>2.73</td><td>1996</td><td>1.53</td><td>6789</td><td>1</td><td>transit</td></tr></tbody></table>
<table><caption>**Table 6** (continued)</caption><thead><tr><th rowspan="2">#</th><th rowspan="2">Planet</th><th colspan="4">Planetary properties</th><th colspan="2">Stellar properties</th><th rowspan="2">Observation</th><th rowspan="2">Type</th></tr><tr><th>R (R<sub>⊕</sub>)</th><th>M (M<sub>⊕</sub>)</th><th>P (days)</th><th>T (K)</th><th>R (R<sub>☉</sub>)</th><th>T (K)</th></tr></thead><tbody><tr><td>38</td><td>HAT-P-6 b</td><td>14.59</td><td>336.03</td><td>3.85</td><td>1629</td><td>1.29</td><td>6570</td><td>2</td><td>transit</td></tr><tr><td>39</td><td>WASP-49 b</td><td>12.24</td><td>120.17</td><td>2.78</td><td>1334</td><td>0.94</td><td>5600</td><td>1</td><td>transit</td></tr><tr><td>40</td><td>WASP-15 b</td><td>15.67</td><td>172.31</td><td>3.75</td><td>1609</td><td>1.18</td><td>6300</td><td>1</td><td>transit</td></tr><tr><td>41</td><td>WASP-79 b</td><td>18.65</td><td>286.12</td><td>3.66</td><td>1709</td><td>1.56</td><td>6600</td><td>1</td><td>transit</td></tr><tr><td>42</td><td>KELT-4A b</td><td>18.64</td><td>286.75</td><td>2.99</td><td>1779</td><td>1.20</td><td>6206</td><td>1</td><td>transit</td></tr><tr><td>43</td><td>WASP-17 b</td><td>21.85</td><td>154.50</td><td>3.74</td><td>1725</td><td>1.31</td><td>6650</td><td>1</td><td>transit</td></tr><tr><td>44</td><td>WASP-3 b</td><td>15.96</td><td>654.89</td><td>1.85</td><td>1933</td><td>1.24</td><td>6400</td><td>1</td><td>occultation</td></tr><tr><td>45</td><td>WASP-7 b</td><td>14.59</td><td>305.19</td><td>4.95</td><td>1448</td><td>1.28</td><td>6400</td><td>1</td><td>transit</td></tr><tr><td>46</td><td>KELT-8 b</td><td>20.41</td><td>275.63</td><td>3.24</td><td>1633</td><td>1.21</td><td>5754</td><td>1</td><td>transit</td></tr><tr><td>47</td><td>HAT-P-22 b</td><td>11.85</td><td>682.55</td><td>3.21</td><td>1248</td><td>0.92</td><td>5302</td><td>3</td><td>transit</td></tr><tr><td>48</td><td>WASP-13 b</td><td>15.44</td><td>158.95</td><td>4.35</td><td>1494</td><td>1.19</td><td>5989</td><td>1</td><td>transit</td></tr><tr><td>49</td><td>HAT-P-33 b</td><td>20.05</td><td>242.56</td><td>3.47</td><td>1799</td><td>1.40</td><td>6446</td><td>1</td><td>transit</td></tr><tr><td>50</td><td>TrES-4 A b</td><td>20.17</td><td>157.05</td><td>3.55</td><td>1644</td><td>1.45</td><td>6295</td><td>1</td><td>transit</td></tr><tr><td>51</td><td>WASP-82 b</td><td>18.33</td><td>394.20</td><td>2.71</td><td>2127</td><td>1.63</td><td>6490</td><td>1</td><td>transit</td></tr><tr><td>52</td><td>WASP-31 b</td><td>16.87</td><td>151.96</td><td>3.41</td><td>1502</td><td>1.16</td><td>6200</td><td>1</td><td>transit</td></tr><tr><td>53</td><td>HAT-P-45 b</td><td>15.65</td><td>283.57</td><td>3.13</td><td>1605</td><td>1.26</td><td>6330</td><td>2</td><td>transit</td></tr><tr><td>54</td><td>KELT-2A b</td><td>14.33</td><td>472.41</td><td>4.11</td><td>1671</td><td>1.31</td><td>6148</td><td>1</td><td>transit</td></tr><tr><td>55</td><td>WASP-26 b</td><td>14.06</td><td>326.81</td><td>2.76</td><td>1618</td><td>1.12</td><td>5950</td><td>2</td><td>occultation</td></tr><tr><td>56</td><td>TrES-2</td><td>12.83</td><td>398.34</td><td>2.47</td><td>1458</td><td>0.98</td><td>5850</td><td>4</td><td>transit</td></tr><tr><td>57</td><td>WASP-50 b</td><td>12.62</td><td>467.32</td><td>1.96</td><td>1354</td><td>0.89</td><td>5400</td><td>5</td><td>transit</td></tr><tr><td>58</td><td>WASP-63 b</td><td>15.69</td><td>120.80</td><td>4.38</td><td>1496</td><td>1.32</td><td>5570</td><td>1</td><td>transit</td></tr><tr><td>59</td><td>XO-2N b</td><td>10.68</td><td>189.79</td><td>2.62</td><td>1312</td><td>0.97</td><td>5332</td><td>2</td><td>transit</td></tr><tr><td>60</td><td>WASP-104 b</td><td>12.48</td><td>404.38</td><td>1.76</td><td>1476</td><td>1.08</td><td>5475</td><td>3</td><td>occultation</td></tr><tr><td>61</td><td>WASP-41 b</td><td>13.28</td><td>292.47</td><td>3.05</td><td>1278</td><td>0.95</td><td>5450</td><td>2</td><td>transit</td></tr><tr><td>62</td><td>HAT-P-40 b</td><td>18.98</td><td>195.51</td><td>4.46</td><td>1719</td><td>1.51</td><td>6080</td><td>1</td><td>transit</td></tr><tr><td>63</td><td>WASP-48 b</td><td>18.33</td><td>311.55</td><td>2.14</td><td>1980</td><td>1.19</td><td>5920</td><td>1</td><td>occultation</td></tr><tr><td>64</td><td>HAT-P-4 b</td><td>13.94</td><td>216.18</td><td>3.06</td><td>1653</td><td>1.26</td><td>5890</td><td>2</td><td>transit</td></tr><tr><td>65</td><td>WASP-4 b</td><td>14.96</td><td>356.53</td><td>1.34</td><td>1818</td><td>0.93</td><td>5500</td><td>1</td><td>occultation</td></tr><tr><td>66</td><td>WASP-103 b</td><td>17.59</td><td>467.32</td><td>0.93</td><td>2430</td><td>1.20</td><td>6110</td><td>1</td><td>occultation</td></tr><tr><td>67</td><td>WASP-75 b</td><td>13.94</td><td>340.16</td><td>2.48</td><td>1660</td><td>1.14</td><td>6100</td><td>2</td><td>occultation</td></tr><tr><td>68</td><td>Qatar-1 b</td><td>12.77</td><td>422.82</td><td>1.42</td><td>1347</td><td>0.85</td><td>4910</td><td>5</td><td>occultation</td></tr><tr><td>69</td><td>WASP-20 b</td><td>16.00</td><td>99.50</td><td>4.90</td><td>1345</td><td>1.20</td><td>5950</td><td>1</td><td>transit</td></tr><tr><td>70</td><td>TrES-3 b</td><td>14.32</td><td>607.20</td><td>1.31</td><td>1654</td><td>0.88</td><td>5720</td><td>1</td><td>occultation</td></tr><tr><td>71</td><td>PTFO 8-8695 b</td><td>20.96</td><td>953.72</td><td>0.45</td><td>1884</td><td>0.34</td><td>3470</td><td>1</td><td>occultation</td></tr><tr><td>72</td><td>HAT-P-1 b</td><td>13.35</td><td>166.58</td><td>4.47</td><td>1259</td><td>1.13</td><td>5975</td><td>1</td><td>transit</td></tr><tr><td>73</td><td>WASP-90 b</td><td>17.89</td><td>200.28</td><td>3.92</td><td>1791</td><td>1.55</td><td>6430</td><td>2</td><td>transit</td></tr><tr><td>74</td><td>HAT-P-46 b</td><td>14.09</td><td>156.73</td><td>4.47</td><td>1413</td><td>1.28</td><td>6120</td><td>1</td><td>transit</td></tr><tr><td>75</td><td>WASP-111 b</td><td>15.82</td><td>581.77</td><td>2.31</td><td>2065</td><td>1.50</td><td>6400</td><td>1</td><td>occultation</td></tr></tbody></table>
<table><caption>**Table 6** (continued)</caption><thead><tr><th rowspan="2">#</th><th rowspan="2">Planet</th><th colspan="4">Planetary properties</th><th colspan="2">Stellar properties</th><th rowspan="2">Observation</th><th rowspan="2">Type</th></tr><tr><th>R (R<sub>⊕</sub>)</th><th>M (M<sub>⊕</sub>)</th><th>P (days)</th><th>T (K)</th><th>R (R<sub>☉</sub>)</th><th>T (K)</th></tr></thead><tbody><tr><td>76</td><td>XO-1 b</td><td>12.99</td><td>286.12</td><td>3.94</td><td>1216</td><td>1.00</td><td>5940</td><td>1</td><td>transit</td></tr><tr><td>77</td><td>WASP-34 b</td><td>13.39</td><td>187.57</td><td>4.32</td><td>1131</td><td>1.01</td><td>5700</td><td>1</td><td>transit</td></tr><tr><td>78</td><td>WASP-88 b</td><td>18.65</td><td>178.03</td><td>4.95</td><td>1716</td><td>1.45</td><td>6431</td><td>1</td><td>transit</td></tr><tr><td>79</td><td>HATS-3 b</td><td>18.62</td><td>361.78</td><td>3.55</td><td>1757</td><td>1.30</td><td>6351</td><td>2</td><td>occultation</td></tr><tr><td>80</td><td>WASP-100 b</td><td>18.54</td><td>645.35</td><td>2.85</td><td>2143</td><td>1.57</td><td>6900</td><td>1</td><td>occultation</td></tr><tr><td>81</td><td>WASP-68 b</td><td>13.61</td><td>302.01</td><td>5.08</td><td>1447</td><td>1.24</td><td>5911</td><td>2</td><td>transit</td></tr><tr><td>82</td><td>CoRoT-2 b</td><td>16.08</td><td>1052.27</td><td>1.74</td><td>1484</td><td>0.97</td><td>5575</td><td>1</td><td>occultation</td></tr><tr><td>83</td><td>HAT-P-49 b</td><td>15.51</td><td>549.98</td><td>2.69</td><td>2072</td><td>1.54</td><td>6820</td><td>1</td><td>occultation</td></tr><tr><td>84</td><td>HAT-P-56 b</td><td>16.09</td><td>693.04</td><td>2.79</td><td>1791</td><td>1.30</td><td>6566</td><td>1</td><td>occultation</td></tr><tr><td>85</td><td>HAT-P-7 b</td><td>16.01</td><td>543.30</td><td>2.20</td><td>2141</td><td>1.59</td><td>6310</td><td>1</td><td>occultation</td></tr><tr><td>86</td><td>WASP-21 b</td><td>12.75</td><td>87.74</td><td>4.32</td><td>1298</td><td>0.89</td><td>5800</td><td>1</td><td>transit</td></tr><tr><td>87</td><td>WASP-22 b</td><td>12.71</td><td>186.93</td><td>3.53</td><td>1383</td><td>1.10</td><td>6000</td><td>2</td><td>transit</td></tr><tr><td>88</td><td>WASP-24 b</td><td>12.11</td><td>328.08</td><td>2.34</td><td>1611</td><td>1.13</td><td>6075</td><td>4</td><td>occultation</td></tr><tr><td>89</td><td>WASP-25 b</td><td>13.83</td><td>184.39</td><td>3.76</td><td>1209</td><td>1.00</td><td>5750</td><td>1</td><td>transit</td></tr><tr><td>90</td><td>HAT-P-5 b</td><td>13.74</td><td>336.98</td><td>2.79</td><td>1477</td><td>1.16</td><td>5960</td><td>6</td><td>transit</td></tr><tr><td>91</td><td>WASP-69 b</td><td>11.60</td><td>82.66</td><td>3.87</td><td>938</td><td>0.83</td><td>4715</td><td>1</td><td>transit</td></tr><tr><td>92</td><td>WASP-87 b</td><td>15.20</td><td>693.04</td><td>1.68</td><td>2251</td><td>1.20</td><td>6450</td><td>1</td><td>occultation</td></tr><tr><td>93</td><td>HAT-P-24 b</td><td>13.63</td><td>217.77</td><td>3.36</td><td>1581</td><td>1.19</td><td>6329</td><td>4</td><td>transit</td></tr><tr><td>94</td><td>HAT-P-39 b</td><td>17.24</td><td>190.43</td><td>3.54</td><td>1705</td><td>1.40</td><td>6430</td><td>3</td><td>transit</td></tr><tr><td>95</td><td>WASP-16 b</td><td>11.06</td><td>271.81</td><td>3.12</td><td>1235</td><td>1.02</td><td>5550</td><td>4</td><td>transit</td></tr><tr><td>96</td><td>TrES-1 b</td><td>12.06</td><td>241.93</td><td>3.03</td><td>1147</td><td>0.88</td><td>5250</td><td>2</td><td>transit</td></tr><tr><td>97</td><td>WASP-64 b</td><td>13.95</td><td>404.06</td><td>1.57</td><td>1587</td><td>0.98</td><td>5400</td><td>3</td><td>occultation</td></tr><tr><td>98</td><td>WASP-6 b</td><td>13.43</td><td>159.91</td><td>3.36</td><td>1161</td><td>0.89</td><td>5450</td><td>1</td><td>transit</td></tr><tr><td>99</td><td>WASP-55 b</td><td>14.27</td><td>181.21</td><td>4.47</td><td>1236</td><td>1.01</td><td>5900</td><td>1</td><td>transit</td></tr><tr><td>100</td><td>HAT-P-36 b</td><td>13.87</td><td>582.41</td><td>1.33</td><td>1778</td><td>1.02</td><td>5580</td><td>1</td><td>occultation</td></tr><tr><td>101</td><td>HAT-P-9 b</td><td>15.36</td><td>213.00</td><td>3.92</td><td>1490</td><td>1.28</td><td>6350</td><td>4</td><td>transit</td></tr><tr><td>102</td><td>HAT-P-14 b</td><td>13.17</td><td>699.40</td><td>4.63</td><td>1525</td><td>1.39</td><td>6600</td><td>3</td><td>occultation</td></tr><tr><td>103</td><td>WASP-28 b</td><td>13.31</td><td>288.34</td><td>3.41</td><td>1429</td><td>1.02</td><td>6150</td><td>6</td><td>transit</td></tr><tr><td>104</td><td>XO-4 b</td><td>14.70</td><td>546.80</td><td>4.13</td><td>1418</td><td>1.32</td><td>5700</td><td>6</td><td>occultation</td></tr><tr><td>105</td><td>WASP-58 b</td><td>15.03</td><td>282.94</td><td>5.02</td><td>1242</td><td>0.94</td><td>5800</td><td>2</td><td>transit</td></tr><tr><td>106</td><td>HAT-P-23 b</td><td>15.01</td><td>664.43</td><td>1.21</td><td>1997</td><td>1.13</td><td>5905</td><td>1</td><td>occultation</td></tr><tr><td>107</td><td>Qatar-2 b</td><td>12.55</td><td>790.63</td><td>1.34</td><td>1256</td><td>0.74</td><td>4645</td><td>9</td><td>occultation</td></tr><tr><td>108</td><td>WASP-5 b</td><td>12.85</td><td>520.41</td><td>1.63</td><td>1693</td><td>1.00</td><td>5700</td><td>2</td><td>occultation</td></tr><tr><td>109</td><td>WASP-65 b</td><td>12.20</td><td>492.76</td><td>2.31</td><td>1446</td><td>0.93</td><td>5600</td><td>7</td><td>occultation</td></tr><tr><td>110</td><td>CoRoT-1 b</td><td>16.35</td><td>327.44</td><td>1.51</td><td>1839</td><td>0.95</td><td>6298</td><td>1</td><td>occultation</td></tr><tr><td>111</td><td>HAT-P-27 b</td><td>11.19</td><td>197.10</td><td>3.04</td><td>1161</td><td>0.92</td><td>5300</td><td>3</td><td>transit</td></tr><tr><td>112</td><td>KELT-6 b</td><td>12.95</td><td>140.51</td><td>7.85</td><td>1284</td><td>1.13</td><td>6272</td><td>1</td><td>transit</td></tr><tr><td>113</td><td>WASP-45 b</td><td>12.73</td><td>320.13</td><td>3.13</td><td>1165</td><td>0.91</td><td>5140</td><td>6</td><td>transit</td></tr></tbody></table>
<table><caption>**Table 6** (continued)</caption><thead><tr><th rowspan="2">#</th><th rowspan="2">Planet</th><th colspan="4">Planetary properties</th><th colspan="2">Stellar properties</th><th colspan="2">Observation</th></tr><tr><th>R (R<sub>⊕</sub>)</th><th>M (M<sub>⊕</sub>)</th><th>P (days)</th><th>T (K)</th><th>R (R<sub>☉</sub>)</th><th>T (K)</th><th>#</th><th>Type</th></tr></thead><tbody><tr><td>114</td><td>WASP-72 b</td><td>11.08</td><td>448.25</td><td>2.22</td><td>1819</td><td>1.23</td><td>6250</td><td>2</td><td>occultation</td></tr><tr><td>115</td><td>HATS-1 b</td><td>14.29</td><td>589.72</td><td>3.45</td><td>1332</td><td>0.99</td><td>5870</td><td>14</td><td>transit</td></tr><tr><td>116</td><td>WASP-78 b</td><td>19.20</td><td>368.77</td><td>2.18</td><td>2136</td><td>2.02</td><td>6100</td><td>1</td><td>occultation</td></tr><tr><td>117</td><td>WASP-96 b</td><td>13.17</td><td>152.60</td><td>3.43</td><td>1251</td><td>1.06</td><td>5540</td><td>3</td><td>transit</td></tr><tr><td>118</td><td>HAT-P-28 b</td><td>13.30</td><td>199.01</td><td>3.26</td><td>1345</td><td>1.02</td><td>5680</td><td>6</td><td>transit</td></tr><tr><td>119</td><td>WASP-39 b</td><td>13.94</td><td>89.01</td><td>4.06</td><td>1088</td><td>0.93</td><td>5400</td><td>1</td><td>transit</td></tr><tr><td>120</td><td>WASP-80 b</td><td>10.45</td><td>176.12</td><td>3.07</td><td>794</td><td>0.57</td><td>4145</td><td>1</td><td>transit</td></tr><tr><td>121</td><td>HATS-2 b</td><td>12.82</td><td>427.58</td><td>1.35</td><td>1528</td><td>0.88</td><td>5227</td><td>5</td><td>occultation</td></tr><tr><td>122</td><td>WASP-71 b</td><td>16.02</td><td>712.75</td><td>2.90</td><td>1987</td><td>1.56</td><td>6050</td><td>1</td><td>occultation</td></tr><tr><td>123</td><td>WASP-38 b</td><td>11.96</td><td>861.53</td><td>6.87</td><td>1218</td><td>1.23</td><td>6150</td><td>10</td><td>transit</td></tr><tr><td>124</td><td>WASP-110 b</td><td>13.58</td><td>162.13</td><td>3.78</td><td>1113</td><td>0.89</td><td>5400</td><td>1</td><td>transit</td></tr><tr><td>125</td><td>HAT-P-3 b</td><td>9.07</td><td>187.88</td><td>2.90</td><td>1115</td><td>0.92</td><td>5224</td><td>4</td><td>transit</td></tr><tr><td>126</td><td>WASP-47 b</td><td>12.84</td><td>336.98</td><td>4.16</td><td>1240</td><td>1.04</td><td>5576</td><td>8</td><td>transit</td></tr><tr><td>127</td><td>WASP-98 b</td><td>12.07</td><td>263.86</td><td>2.96</td><td>1149</td><td>0.69</td><td>5525</td><td>8</td><td>transit</td></tr><tr><td>128</td><td>WASP-46 b</td><td>14.38</td><td>667.92</td><td>1.43</td><td>1615</td><td>0.96</td><td>5620</td><td>3</td><td>occultation</td></tr><tr><td>129</td><td>HAT-P-25 b</td><td>13.06</td><td>180.22</td><td>3.65</td><td>1172</td><td>1.01</td><td>5500</td><td>3</td><td>transit</td></tr><tr><td>130</td><td>WASP-18 b</td><td>12.78</td><td>3315.77</td><td>0.94</td><td>2345</td><td>1.24</td><td>6400</td><td>1</td><td>occultation</td></tr><tr><td>131</td><td>WASP-67 b</td><td>15.36</td><td>133.52</td><td>4.61</td><td>1000</td><td>0.87</td><td>5200</td><td>1</td><td>transit</td></tr><tr><td>132</td><td>WASP-14 b</td><td>14.06</td><td>2333.75</td><td>2.24</td><td>1834</td><td>1.21</td><td>6462</td><td>1</td><td>occultation</td></tr><tr><td>133</td><td>WASP-60 b</td><td>9.44</td><td>163.40</td><td>4.31</td><td>1261</td><td>0.51</td><td>5900</td><td>6</td><td>transit</td></tr><tr><td>134</td><td>WASP-11 b</td><td>11.47</td><td>146.24</td><td>3.72</td><td>1002</td><td>0.82</td><td>4974</td><td>1</td><td>transit</td></tr><tr><td>135</td><td>HAT-P-35 b</td><td>14.62</td><td>335.07</td><td>3.65</td><td>1537</td><td>1.24</td><td>6096</td><td>12</td><td>occultation</td></tr><tr><td>136</td><td>WASP-36 b</td><td>13.93</td><td>724.51</td><td>1.54</td><td>1655</td><td>1.02</td><td>5881</td><td>3</td><td>occultation</td></tr><tr><td>137</td><td>HAT-P-50 b</td><td>14.13</td><td>429.17</td><td>3.12</td><td>1805</td><td>1.27</td><td>6280</td><td>3</td><td>occultation</td></tr><tr><td>138</td><td>WASP-99 b</td><td>12.07</td><td>883.78</td><td>5.75</td><td>1438</td><td>1.48</td><td>6180</td><td>6</td><td>occultation</td></tr><tr><td>139</td><td>HAT-P-42 b</td><td>14.01</td><td>309.96</td><td>4.64</td><td>1389</td><td>1.18</td><td>5743</td><td>13</td><td>transit</td></tr><tr><td>140</td><td>WASP-73 b</td><td>12.73</td><td>597.66</td><td>4.09</td><td>1736</td><td>1.34</td><td>6036</td><td>3</td><td>occultation</td></tr><tr><td>141</td><td>WASP-135 b</td><td>14.27</td><td>604.02</td><td>1.40</td><td>1673</td><td>0.98</td><td>5675</td><td>3</td><td>occultation</td></tr><tr><td>142</td><td>WASP-23 b</td><td>10.56</td><td>281.03</td><td>2.94</td><td>1099</td><td>0.78</td><td>5150</td><td>10</td><td>transit</td></tr><tr><td>143</td><td>TrES-5 b</td><td>13.27</td><td>565.24</td><td>1.48</td><td>1433</td><td>0.88</td><td>5171</td><td>10</td><td>occultation</td></tr><tr><td>144</td><td>HAT-P-16 b</td><td>13.06</td><td>1332.98</td><td>2.78</td><td>1527</td><td>1.22</td><td>6140</td><td>3</td><td>occultation</td></tr><tr><td>145</td><td>Kepler-12 b</td><td>19.20</td><td>136.70</td><td>4.44</td><td>1341</td><td>1.09</td><td>5953</td><td>2</td><td>transit</td></tr><tr><td>146</td><td>Kepler-7 b</td><td>17.71</td><td>137.65</td><td>4.89</td><td>1584</td><td>1.36</td><td>5933</td><td>4</td><td>transit</td></tr><tr><td>147</td><td>WASP-44 b</td><td>11.00</td><td>276.26</td><td>2.42</td><td>1275</td><td>0.92</td><td>5410</td><td>28</td><td>transit</td></tr><tr><td>148</td><td>XO-5 b</td><td>11.30</td><td>342.39</td><td>4.19</td><td>1206</td><td>0.88</td><td>5510</td><td>16</td><td>transit</td></tr><tr><td>149</td><td>HAT-P-43 b</td><td>14.08</td><td>209.82</td><td>3.33</td><td>1322</td><td>1.05</td><td>5645</td><td>12</td><td>transit</td></tr><tr><td>150</td><td>HAT-P-55 b</td><td>12.97</td><td>185.02</td><td>3.58</td><td>1278</td><td>1.01</td><td>5808</td><td>10</td><td>transit</td></tr><tr><td>151</td><td>WASP-32 b</td><td>13.06</td><td>1144.46</td><td>2.72</td><td>1507</td><td>1.10</td><td>6100</td><td>5</td><td>occultation</td></tr></tbody></table>
<table><caption>**Table 6** (continued)</caption><thead><tr><th rowspan="2">#</th><th rowspan="2">Planet</th><th colspan="3">Planetary properties</th><th colspan="2">Stellar properties</th><th colspan="2">Observation</th></tr><tr><th>R (R<sub>⊕</sub>)</th><th>M (M<sub>⊕</sub>)</th><th>P (days)</th><th>T (K)</th><th>R (R<sub>☉</sub>)</th><th>T (K)</th><th>#</th><th>Type</th></tr></thead><tbody><tr><td>152</td><td>HAT-P-29 b</td><td>12.15</td><td>247.33</td><td>5.72</td><td>1224</td><td>1.21</td><td>6087</td><td>8</td><td>transit</td></tr><tr><td>153</td><td>WASP-10 b</td><td>11.85</td><td>972.79</td><td>3.09</td><td>1009</td><td>0.71</td><td>4675</td><td>37</td><td>transit</td></tr><tr><td>154</td><td>Kepler-6 b</td><td>14.27</td><td>213.00</td><td>3.23</td><td>1354</td><td>1.05</td><td>5640</td><td>15</td><td>transit</td></tr><tr><td>155</td><td>HD219134b</td><td>1.61</td><td>4.47</td><td>3.09</td><td>934</td><td>0.78</td><td>4699</td><td>1</td><td>transit</td></tr><tr><td>156</td><td>HATS-13 b</td><td>13.30</td><td>172.62</td><td>3.04</td><td>1212</td><td>0.96</td><td>5523</td><td>10</td><td>transit</td></tr><tr><td>157</td><td>HAT-P-51 b</td><td>14.19</td><td>98.23</td><td>4.22</td><td>1159</td><td>0.98</td><td>5449</td><td>2</td><td>transit</td></tr><tr><td>158</td><td>HAT-P-34 b</td><td>13.14</td><td>1057.99</td><td>5.45</td><td>1440</td><td>1.39</td><td>6442</td><td>10</td><td>occultation</td></tr><tr><td>159</td><td>WASP-37 b</td><td>12.47</td><td>539.17</td><td>3.58</td><td>1293</td><td>0.85</td><td>5800</td><td>43</td><td>transit</td></tr><tr><td>160</td><td>WASP-56 b</td><td>11.98</td><td>181.52</td><td>4.62</td><td>1117</td><td>1.03</td><td>5600</td><td>4</td><td>transit</td></tr><tr><td>161</td><td>WASP-66 b</td><td>15.25</td><td>737.54</td><td>4.09</td><td>1754</td><td>1.30</td><td>6600</td><td>3</td><td>occultation</td></tr><tr><td>162</td><td>WASP-112 b</td><td>13.07</td><td>279.76</td><td>3.04</td><td>1349</td><td>0.81</td><td>5610</td><td>28</td><td>transit</td></tr><tr><td>163</td><td>HAT-P-44 b</td><td>14.05</td><td>124.62</td><td>4.30</td><td>1092</td><td>0.94</td><td>5295</td><td>2</td><td>transit</td></tr><tr><td>164</td><td>HAT-P-37 b</td><td>12.93</td><td>371.63</td><td>2.80</td><td>1166</td><td>0.93</td><td>5500</td><td>37</td><td>transit</td></tr><tr><td>165</td><td>Gliese 436 b</td><td>4.13</td><td>23.11</td><td>2.64</td><td>695</td><td>0.45</td><td>3684</td><td>1</td><td>transit</td></tr><tr><td>166</td><td>WASP-29 b</td><td>8.69</td><td>77.57</td><td>3.92</td><td>970</td><td>0.82</td><td>4800</td><td>1</td><td>transit</td></tr><tr><td>167</td><td>HD 219134 b</td><td>1.57</td><td>3.81</td><td>3.09</td><td>931</td><td>0.79</td><td>4699</td><td>1</td><td>transit</td></tr><tr><td>168</td><td>HAT-P-12 b</td><td>10.52</td><td>67.08</td><td>3.21</td><td>932</td><td>0.73</td><td>4650</td><td>1</td><td>transit</td></tr><tr><td>169</td><td>Kepler-13 A b</td><td>15.43</td><td>2571.87</td><td>1.76</td><td>2389</td><td>1.72</td><td>7200</td><td>1</td><td>occultation</td></tr><tr><td>170</td><td>HAT-P-19 b</td><td>12.17</td><td>92.83</td><td>4.01</td><td>982</td><td>0.84</td><td>4990</td><td>1</td><td>transit</td></tr><tr><td>171</td><td>CoRoT-11 b</td><td>15.25</td><td>791.59</td><td>2.99</td><td>1686</td><td>1.27</td><td>6440</td><td>5</td><td>occultation</td></tr><tr><td>172</td><td>Kepler-8 b</td><td>15.58</td><td>187.57</td><td>3.52</td><td>1528</td><td>1.13</td><td>6251</td><td>20</td><td>transit</td></tr><tr><td>173</td><td>HATS-10 b</td><td>10.63</td><td>167.22</td><td>3.31</td><td>1369</td><td>1.10</td><td>5880</td><td>28</td><td>transit</td></tr><tr><td>174</td><td>WTS-2 b</td><td>14.96</td><td>356.06</td><td>1.02</td><td>1495</td><td>0.82</td><td>5000</td><td>16</td><td>occultation</td></tr><tr><td>175</td><td>HAT-P-52 b</td><td>11.07</td><td>260.05</td><td>2.75</td><td>1184</td><td>0.89</td><td>5131</td><td>43</td><td>transit</td></tr><tr><td>176</td><td>HAT-P-20 b</td><td>9.51</td><td>2303.55</td><td>2.88</td><td>946</td><td>0.76</td><td>4595</td><td>97</td><td>occultation</td></tr><tr><td>177</td><td>WASP-120 b</td><td>16.62</td><td>1592.71</td><td>3.61</td><td>1842</td><td>1.45</td><td>6450</td><td>1</td><td>occultation</td></tr><tr><td>178</td><td>HATS-9 b</td><td>11.69</td><td>266.09</td><td>1.92</td><td>1769</td><td>1.03</td><td>5366</td><td>9</td><td>occultation</td></tr><tr><td>179</td><td>CoRoT-19 b</td><td>15.91</td><td>352.88</td><td>3.90</td><td>1616</td><td>1.21</td><td>6090</td><td>16</td><td>occultation</td></tr><tr><td>180</td><td>OGLE-TR-10 b</td><td>18.87</td><td>216.18</td><td>3.10</td><td>1554</td><td>1.28</td><td>6075</td><td>16</td><td>occultation</td></tr><tr><td>181</td><td>WASP-42 b</td><td>11.85</td><td>158.95</td><td>4.98</td><td>969</td><td>0.88</td><td>5200</td><td>1</td><td>transit</td></tr><tr><td>182</td><td>WASP-61 b</td><td>13.61</td><td>654.89</td><td>3.86</td><td>1509</td><td>1.22</td><td>6250</td><td>17</td><td>occultation</td></tr><tr><td>183</td><td>HAT-P-31 b</td><td>11.74</td><td>690.18</td><td>5.01</td><td>1343</td><td>1.22</td><td>6065</td><td>43</td><td>occultation</td></tr><tr><td>184</td><td>HAT-P-53 b</td><td>14.46</td><td>471.77</td><td>1.96</td><td>1624</td><td>1.09</td><td>5956</td><td>7</td><td>occultation</td></tr><tr><td>185</td><td>WASP-8 b</td><td>11.39</td><td>713.38</td><td>8.16</td><td>906</td><td>1.03</td><td>5600</td><td>6</td><td>transit</td></tr><tr><td>186</td><td>HATS-4 b</td><td>11.19</td><td>420.59</td><td>2.52</td><td>1282</td><td>1.00</td><td>5403</td><td>97</td><td>occultation</td></tr><tr><td>187</td><td>Kepler-447 b</td><td>18.11</td><td>435.53</td><td>7.79</td><td>908</td><td>0.76</td><td>5493</td><td>2</td><td>transit</td></tr><tr><td>188</td><td>Kepler-76 b</td><td>14.92</td><td>638.99</td><td>1.54</td><td>2074</td><td>1.20</td><td>6409</td><td>2</td><td>occultation</td></tr><tr><td>189</td><td>WASP-57 b</td><td>10.05</td><td>213.63</td><td>2.84</td><td>1430</td><td>1.01</td><td>5600</td><td>43</td><td>occultation</td></tr></tbody></table>
<table><caption>**Table 6** (continued)</caption><thead><tr><th rowspan="2">#</th><th rowspan="2">Planet</th><th colspan="4">Planetary properties</th><th colspan="2">Stellar properties</th><th colspan="2">Observation</th></tr><tr><th>R (R<sub>⊕</sub>)</th><th>M (M<sub>⊕</sub>)</th><th>P (days)</th><th>T (K)</th><th>R (R<sub>☉</sub>)</th><th>T (K)</th><th>#</th><th>Tpe</th></tr></thead><tbody><tr><td>190</td><td>CoRoT-5 b</td><td>15.23</td><td>148.46</td><td>4.04</td><td>1315</td><td>1.00</td><td>6100</td><td>15</td><td>transit</td></tr><tr><td>191</td><td>HD 17156 b</td><td>12.02</td><td>1014.44</td><td>21.22</td><td>816</td><td>1.27</td><td>6079</td><td>9</td><td>transit</td></tr><tr><td>192</td><td>Kepler-412 b</td><td>14.54</td><td>298.51</td><td>1.72</td><td>1780</td><td>1.17</td><td>5750</td><td>12</td><td>occultation</td></tr><tr><td>193</td><td>XO-3 b</td><td>13.35</td><td>3748.12</td><td>3.19</td><td>1665</td><td>1.21</td><td>6429</td><td>1</td><td>occultation</td></tr><tr><td>194</td><td>WASP-117 b</td><td>11.20</td><td>87.58</td><td>10.02</td><td>997</td><td>1.13</td><td>6040</td><td>1</td><td>transit</td></tr><tr><td>195</td><td>Gliese 1214 b</td><td>2.77</td><td>6.20</td><td>1.58</td><td>552</td><td>0.18</td><td>3250</td><td>1</td><td>transit</td></tr><tr><td>196</td><td>Gliese 3470 b</td><td>3.80</td><td>13.73</td><td>3.34</td><td>635</td><td>0.51</td><td>3652</td><td>1</td><td>transit</td></tr><tr><td>197</td><td>HAT-P-11 b</td><td>4.96</td><td>25.75</td><td>4.89</td><td>848</td><td>0.81</td><td>4780</td><td>1</td><td>transit</td></tr><tr><td>198</td><td>GJ 1132 b</td><td>1.16</td><td>1.62</td><td>1.63</td><td>529</td><td>0.18</td><td>3270</td><td>1</td><td>transit</td></tr><tr><td>199</td><td>Gliese 436 c</td><td>0.66</td><td>0.28</td><td>1.37</td><td>813</td><td>0.45</td><td>3684</td><td>1</td><td>transit</td></tr><tr><td>200</td><td>HAT-P-26 b</td><td>6.20</td><td>18.76</td><td>4.23</td><td>967</td><td>0.82</td><td>5079</td><td>1</td><td>transit</td></tr><tr><td>201</td><td>HAT-P-18 b</td><td>10.39</td><td>62.31</td><td>5.51</td><td>818</td><td>0.77</td><td>4870</td><td>1</td><td>transit</td></tr><tr><td>202</td><td>HD 97658 b</td><td>2.34</td><td>7.55</td><td>9.49</td><td>729</td><td>0.77</td><td>5119</td><td>1</td><td>transit</td></tr><tr><td>203</td><td>HAT-P-17 b</td><td>11.08</td><td>169.76</td><td>10.34</td><td>758</td><td>0.86</td><td>5246</td><td>1</td><td>transit</td></tr><tr><td>204</td><td>WASP-84 b</td><td>10.70</td><td>222.53</td><td>8.52</td><td>780</td><td>0.85</td><td>5280</td><td>1</td><td>transit</td></tr><tr><td>205</td><td>HATS-6 b</td><td>10.95</td><td>101.41</td><td>3.33</td><td>693</td><td>0.57</td><td>3724</td><td>1</td><td>transit</td></tr><tr><td>206</td><td>EPIC 203771098 c</td><td>7.93</td><td>27.02</td><td>42.36</td><td>596</td><td>1.12</td><td>5743</td><td>1</td><td>transit</td></tr><tr><td>207</td><td>KOI-142 b</td><td>4.13</td><td>1.76</td><td>10.95</td><td>764</td><td>1.02</td><td>5513</td><td>1</td><td>transit</td></tr><tr><td>208</td><td>HATS-5 b</td><td>10.01</td><td>75.34</td><td>4.76</td><td>998</td><td>0.94</td><td>5304</td><td>1</td><td>transit</td></tr><tr><td>209</td><td>Kepler-51 b</td><td>6.95</td><td>2.10</td><td>45.15</td><td>496</td><td>1.04</td><td>6018</td><td>1</td><td>transit</td></tr><tr><td>210</td><td>HAT-P-2 b</td><td>10.44</td><td>2778.51</td><td>5.63</td><td>1443</td><td>1.36</td><td>6290</td><td>1</td><td>occultation</td></tr></tbody></table>

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