Report - School of Physics
Report - School of Physics
Report - School of Physics
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The planetary lensing events have a typical duration <strong>of</strong> 2–20 hr (compared to the<br />
typical 2–20 weeks duration for lensing events due to stars), and must be sampled by<br />
photometry <strong>of</strong> ∼ 1% accuracy several times per hour over a period <strong>of</strong> several days,<br />
and with high angular resolution because <strong>of</strong> the high density <strong>of</strong> bright main-sequence<br />
stars in the central bulge. The proposed polar orbit is oriented to keep the Galactic<br />
bulge in the continuous viewing zone. Most <strong>of</strong> the multiple-planet detections in<br />
the simulations <strong>of</strong> Bennett & Rhie (2002) are systems in which both ‘Jupiter’ and<br />
‘Saturn’ planets are detected. Since multiple orbits are generally stable only if they<br />
are close to circular, a microlensing survey will be able to provide information on the<br />
abundance <strong>of</strong> giant planets with nearly circular orbits by measuring the frequency<br />
<strong>of</strong> double-planet detections and the ratios <strong>of</strong> their separations.<br />
Just over 100 Earths would be detected if each lens star has one in a 1 AU orbit. The<br />
peak sensitivity is at an orbital distance <strong>of</strong> 2.5 AU, with 230 expected detections if<br />
each lens star had a planet in such an orbit. Although the prime quantity obtained<br />
from a microlensing detection is the mass ratio between planet and star, additional<br />
information or hypotheses can be combined to estimate the mass <strong>of</strong> the host star,<br />
the planetary mass, the distance to the host star, and the planet-star separation in<br />
the plane <strong>of</strong> the sky.<br />
One <strong>of</strong> the disadvantages <strong>of</strong> lensing experiments is that a planet event, once observed,<br />
can never (in practice) be seen again – follow-up observations for further<br />
characterisations are not feasible (unlike the case for any <strong>of</strong> the other principal<br />
detection methods). Nevertheless, a mission like MPF/GEST will provide important<br />
observational and statistical data on the occurrence <strong>of</strong> low-mass planets (Earth<br />
to Jupiter masses), low-mass planets at larger orbital radii, multiple systems and,<br />
significantly, free-floating planets formed as a by-product <strong>of</strong> the system formation.<br />
Detection by microlensing could in principle also be included in the Eddington mission,<br />
but the Eddington team has made no detailed evaluation <strong>of</strong> feasibility, and its<br />
inclusion would be likely to drive instrumental requirements in a non-trivial manner.<br />
2.2.4 Other Space Missions: JWST, Spitzer, SOFIA<br />
JWST: JWST (http://www.jwst.nasa.gov/) is a collaboration between NASA,<br />
ESA and the CSA. It will be a passively-cooled (40–50 K) observatory spacecraft<br />
with an 18-segment primary mirror having an effective aperture <strong>of</strong> about 6.5 m<br />
and diffraction-limited performance at 2 µm, equipped with four principal science<br />
instruments and a fine guidance sensor. It is scheduled for launch in 2011 into an<br />
L2 Lissajous orbit. The observatory is optimised for the 1–5 µm band, but will<br />
be equipped to cover 0.6–28 µm with a combination <strong>of</strong> imaging (through fixed and<br />
tunable filters) and low- to moderate-resolution (100 < R < 3000) spectroscopy.<br />
The ‘Origin and Evolution <strong>of</strong> Planetary Systems’ is one <strong>of</strong> JWST’s five science<br />
themes, and the science requirements are drafted accordingly.<br />
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