Report - School of Physics
Report - School of Physics
Report - School of Physics
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3.3 ESA Themes: 2015–2025<br />
In mid-2004, ESA solicited a call for ideas for its scientific programme beyond 2015,<br />
resulting in several outline proposals in the area <strong>of</strong> exo-planets:<br />
A Large UV Telescope (Lecavelier): the proposal considers a large UV telescope<br />
as a promising way to conduct a deep search for bio-markers in Earth-mass<br />
exo-planets, through the detection <strong>of</strong> relevant atmospheric signatures (such as ozone,<br />
water, CO, and CO 2 ) in a very large number <strong>of</strong> exo-planets, and planetary satellites,<br />
up to several hundred parsec distant. It notes that the detection <strong>of</strong> atmospheric signatures<br />
in HD 209458b has been made through space UV observations, and stresses<br />
that large numbers <strong>of</strong> prime targets for these observations will be detected by Gaia.<br />
It underlines the possibility <strong>of</strong> time-resolved spectroscopy (over the 10-min typical<br />
transit time <strong>of</strong> an Earth-mass planet) providing spatial information <strong>of</strong> atmospheric<br />
constituents along the planet surface (poles versus equator, presence <strong>of</strong> continents).<br />
A JWST-size telescope is proposed, and some quantitative expectations are given.<br />
Search for Planets and Life in the Universe (Léger): the proposal makes the<br />
general case for the continued development <strong>of</strong> an ESA strategy for the improved<br />
detection and characterisation <strong>of</strong> exo-planets, primarily through the techniques <strong>of</strong><br />
transits and direct detection. This proposal was submitted on behalf <strong>of</strong> more than<br />
200 individuals and institutions.<br />
Astrometric detection <strong>of</strong> Earth-Mass Planets (Perryman): the proposal<br />
points out that, beyond the micro-arcsec astrometric accuracies <strong>of</strong> ESA’s Gaia mission,<br />
10 nano-arcsec accuracies would permit the detection <strong>of</strong> astrometric perturbations<br />
due to Earth-mass planets around Sun-like stars at 100 pc. If a survey-type<br />
mission were feasible, the concept could lead to the systematic survey <strong>of</strong> many hundreds<br />
<strong>of</strong> thousands <strong>of</strong> stars for Earth-mass planets – important for the generation<br />
<strong>of</strong> target objects if the fraction <strong>of</strong> Earth-mass planets turns out to be very small.<br />
Earth-mass perturbations around a solar-mass star are 300 nano-arcsec at 10 pc,<br />
or 30 nano-arcsec at 100 pc, the latter requiring an instantaneous measurement accuracy<br />
a factor 3 better, i.e. 10 nano-arcsec at, say, 12 mag. This is a factor <strong>of</strong><br />
some 1000 improvement with respect to Gaia. Keeping all other mission parameters<br />
(efficiency, transverse field <strong>of</strong> view, mission duration, total observing time per star,<br />
and image pixel sampling, etc.) unchanged, we can consider reaching this accuracy<br />
simply through a scaling up <strong>of</strong> the primary mirror size. The Gaia primary mirror<br />
has an along-scan dimension D = 1.4 m and a transverse dimension H = 0.5 m; the<br />
final accuracy scales as σ ∝ D −3/2 H −1/2 . These desired accuracies would therefore<br />
require a primary mirror size <strong>of</strong> order 50×12 m 2 , and a focal length (scaling with D)<br />
<strong>of</strong> about 1600 m, similar to the scale <strong>of</strong> the optics derived for the mini-version <strong>of</strong><br />
Life Finder. Accuracy levels <strong>of</strong> ∼ 10 nano-arcsec are still above the noise floors<br />
due to interplanetary and interstellar scintillation in the optical, or stochastic gravitational<br />
wave noise. Astrometric accuracy limits due to surface granular structure<br />
and star spots were discussed in Section 1.3. To reach the astrometric precision <strong>of</strong><br />
300 nano-arcsec at 10 pc means that the photocentre <strong>of</strong> a star must be determined to<br />
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