Report - School of Physics
Report - School of Physics
Report - School of Physics
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
2.3 Summary <strong>of</strong> Prospects 2005–2015<br />
The prospects for the main search experiments described in this section are summarised<br />
in Table 5. This table presents only a simplified picture <strong>of</strong> planet detection<br />
capabilities, ignoring the comparative importance <strong>of</strong> finding large numbers <strong>of</strong> exoplanets<br />
with only an estimation <strong>of</strong> M sin i or r/R, or more comprehensively characterising<br />
a smaller number <strong>of</strong> planets (with mass, radius, albedo, and age). It also<br />
ignores the fact that different objects will be detected by different methods, and<br />
that different methods supply complementary astrophysical information.<br />
Table 5: Predictions for the numbers <strong>of</strong> planet detections out to 2015 according to the major experiments<br />
currently planned, and the planet mass range given in the first column (M ⊕ ∼ 0.003M J ).<br />
The predictions depend sensitively on the (unknown) frequency <strong>of</strong> occurrence <strong>of</strong> (especially the<br />
lower-mass) planets, uncertain sample sizes, stellar jitter, etc. These are generally assessed somewhat<br />
differently for each project, and details are given in the accompanying text. The numbers<br />
must be understood as indications <strong>of</strong> possible developments only.<br />
M Planet 2004 2008–10 2008–10 2008 2010 2010–12 2015 2016 2016<br />
(M J ) Radial Velocity Transits COROT Kepler Eddington SIM Gaia<br />
(ground) (ground) astrom photom<br />
(a) (b) (c) (d) (e) (f) (g) (h) (i)<br />
1–10 90 200–250 100–1000 5–15 see below 200 15 000 3000<br />
0.1–1 30 150–200 0 50–150 see below 50 5 000 0<br />
0.01–0.1 0 10–20 0 10–30 see below 20 0 0<br />
0.003–0.01 0 0 0 0–3 0–640 0–660 0–5 0 0<br />
The columns <strong>of</strong> the table give results expected for: (a) the present situation, dominated by radial<br />
velocity detections; (b) the situation projected in the year 2010 from ground-based radial<br />
velocity observations (estimates by Udry, see Section 2.1.1); (c) ground-based transit detections:<br />
hot Jupiters extrapolated from Horne (2003); (d) COROT (estimates by Bouchy & Rauer, see<br />
Section 2.2.1); (e) Kepler (taken from the Kepler www site, see Section 2.2.1); (f) Eddington (estimates<br />
by Favata, see Section 2.2.1); (g) SIM (estimates by Perryman from the surveys noted in<br />
Section 2.2.2); (h–i) Gaia astrometric and photometric detections (see Section 2.2.2).<br />
The estimated detections for Eddington are not available as a simple function <strong>of</strong> mass, but have<br />
been classified (as detailed under the relevant section) as follows, with the same assessment then<br />
made for the Kepler mission using the same assumptions:<br />
– Eddington: 14 000 planets in total (in 12 500 systems)<br />
– Kepler: 51 000 planets in total<br />
– Eddington: 8000 hot planets, 5600 with R > 5R ⊕<br />
– Kepler: 30 000 hot planets, 22 000 with R > 5R ⊕<br />
– Eddington: 660 Earths (0.5 < R < 2.0R ⊕ )<br />
– Kepler: 19 000 Earths (0.5 < R < 2.0R ⊕ )<br />
– Eddington: 160 habitable zone planets, <strong>of</strong> which 20 ‘Earths’<br />
– Kepler: 530 habitable zone planets, <strong>of</strong> which 35 ‘Earths’<br />
38