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PHYS 400

 

SPECIAL PROBLEMS IN PHYSICS

 

 

 

 

 

 

CURRENT AND FUTURE SEARCHES FOR EXTRASOLAR PLANETS

 

 

 

 

 

 

ATAKAN ERDEN

71689-4

PHYSICS-4

 

 

 

 

 

 

SUPERVISOR: Asist. Prof. Dr. SέNAN KAAN YERLέ

                                       

APRIL 14, 2004

 

 

 

 

 

 

 

Table of Contents

 

 

 

 

 

1 INTRODUCTION…………………………………………………………………………..1

 

2. PLANET DETECTION METHODS.............................................................…………….1

            2.1 Pulsar Timing..........................................................................................................2

2.2 Doppler Spectroscopy (Radial Velocity)  .............................................................3

2.3 Astrometry………………………………………………………………………...3

2.4 Microlensing ...........................................................................................................4

2.5 Transits Photometry..............................................................................................5

 

 3.COMPARE THE METHODS...........................................................................................6

 

 

4.CONCLUSION…………………………………………………………………………….7.

 

References…………………………………………………………………………………….7

 

 

 

 

 

 

 

 

 

 

1.INTRODUCTION

The planets around main squence stars generated much more interest,and one astronomer even called it hysteria. Perhaps this because the detection of planets around main squence stars made the possibility of finding other Earths seem a lot closer. Should technology advance sufficiently to find other Earths – which it surely will – the interest will rise even further, and questions such as whether these extrasolar planets can support life will be everyone’s tongue. Indeed , many will ask if these new worlds are already inhabited.

In this project I prepared planet detection methods and summarized  results of them.

 

2.PLANET DETECTION METHODS

 

2.1 Pulsar Timing

The first widely accepted detection of extrasolar planets was made by Wolszczan (1994). Earth-mass and even smaller planets orbiting a pulsar were detected by measuring the periodic variation in the pulse arrival time. The planets detected are orbiting a pulsar, a "dead" star, rather than a dwarf (main-sequence) star. What is heartening about the detection is that the planets were probably formed after the supernova that resulted in the pulsar. Thereby demonstrating that planet formation is probably a common rather than a rare phenomenon.

 

2.2 Doppler Spectroscopy (Radial Velocity)

Doppler spectroscopy is used to detect the periodic velocity shift of the stellar spectrum caused by an orbiting giant planet. (This method is also referred to as the radial velocity method.) From ground-based observatories, spectroscopists can measure Doppler shifts greater than 3 m/sec due to the reflex motion of the star This corresponds to a minimum detectable mass of 33Me / sini for a planet at 1 AU from a one solar-mass (1 Mo) star, where i is the inclination of the orbital pole to the line-of-sight (LOS). This method can be used for main-sequence stars of spectral types mid-F through M. Stars hotter and more massive than mid F rotate faster, pulsate, are generally more active and have less spectral structure, thus making to more difficult to measure their Doppler shift. The minimum detectable planet mass increases as the square root of the planet's orbital size.

 

 

2.3 Astrometry

Astrometry is used to look for the periodic wobble that a planet induces in the position of its parent star. The minimum detectable planet mass gets smaller in inverse proportion to the planet's distance from the star. For a space-based astrometric instrument, such as the planned Space Interferometry Mission (SIM), that could measure an angle as small as 2 micro-arcsec, a minimum planet of mass of 6.6Me could be detected in a 1 year orbit around a 1 Mo star that is 10 pc from the Earth (gray descending line for stars out to 10 pc) and a 0.4 MJ planet in a 4 year orbit (dark-blue descending line for stars out to 500 pc).

From the ground, the Keck telescope is being equipped to measure angles as small as 20 micro-arc seconds, leading to a minimum detectable mass in a 1 AU orbit of 66Me for a solar-mass star at 10 pc.

The limitations to this method are the distance to the star and variations in the position of the photometric center due to star spots. There are only 33 non-binary solar-like (F, G and K) main-sequence stars within 10 pc of the Earth. The furthest planet from its star that can be detected is limited by the time needed to observe at least one orbital period. There are no planet detections that have been confirmed using this method.

 

2.4 Microlensing

This method uses stars in our Galactic bulge as sources of light rays which are bent by the gravitational fields of the “lens” stars in the foreground, between us and the Galactic bulge.  This gives a “microlensing light curve” that rises and falls. Planets that orbit these “lens” stars can be detected when the light rays from one of the lensed images pass close to a planet orbiting the lens star.  The gravitational field of the planet distorts the light curve: the deviation is typically about 10%, and duration is a few hours to a day (compared to 1-2 months for the lensing due to the star). 

Unique advantage: Strength of signal is nearly independent of planetary mass!  Microlensing signals of low-mass planets have shorter duration and lower detection probability compared to high-mass planets, but not a weaker signal.  So microlensing surveys with frequent observations of large number of stars should be able to detect terrestrial planets with good confidence.

The big challenge is that microlensing events are rare, so have to monitor millions of stars, and even of those that lens, only about 2% of earth-mass planets orbiting these stars will be in right position to be detected (if all the stars have earth-mass planets).  Also need very good angular resolution and fairly accurate (~1%) photometry.  Several other problems, but these are being addressed.

GEST (Galactic Exoplanet Survey Telescope)—1.5m space telescope with large field of view.  Will survey about 100 million stars.  Could detect planets down to Mars mass, should find ~100 Earth-mass planets at 1AU (if all stars have such planets).  “Free-floating” planets will also be detected! (Only method that can do that.) Will also be able to detect ~50,000 giant planets by transits.  Sensitive to planets at nearly all distances from star, unlike other methods.

 

2.5 Transits Photometry

Photometry measures the periodic dimming of the star caused by a planet passing in front of the star along the line of sight from the observer. Stellar variability on the time scale of a transit limits the detectable size to about half that of Earth for a 1 AU orbit about a 1 Mo star or Mars size planets in Mercury-like orbits with four years of observing. Mercury-size planets can even be detected in the habitable-zone of K and M stars. Planets with orbital periods greater than two years are not readily detectable, since their chance of being properly aligned along the line of sight to the star becomes very small.

Giant outer planets that produce a transit signal of 1% ( 120 times that of an Earth, i.e., a SNR >1000) but have orbital periods greater than 2 years can be followed up with Doppler spectroscopy or ground-based photometry.

Giant planets in inner orbits can also be detectable independent of the orbit alignment, based on the periodic modulation of their reflected light. For the 10% of these that have transits, the transit depth can be combined with the mass found from Doppler data to determine the density of the planet as has been done for the case of HD209458b and see if these inner giants are "inflated".

Doppler spectroscopy and astrometry (SIM) measurements can be used to search for any giant planets that might also be in the systems discovered using photometry. Since the orbital inclination must be close to 90° (sin i=1.) to cause transits, there is very little uncertainty in the mass of any giant planet detected.

 

3.COMPARE THE METHODS

 

Figure1:Detection Limits for Planets Around Solar-Like Stars

The limiting sensitivities for a solar-like star are shown for:

·                     Photometry with Kepler (the white region above and to the left of the light-blue lines), COROT (above and to the left of the lavender line); and ground-based photometry (above the solid green line)

·                     Doppler spectroscopy at 3 m/s (above and to the left of the red line); Planets detected using this method: the first 49 are shown as filled diamonds. (The latest data can be found at Extrasolar Planets Encyclopedia) To date (Nov 2001) about 70 have been detected.

·                     Astrometry with SIM at 2΅as (above and to the right of the gray and dark-blue lines)

Solar system objects: Mercury, Venus , Earth, Mars, Jupiter, Saturn, Uranus and Neptune are shown as solid blue dots .

The limits to the maximum orbits are related to the length of time needed to observe one or more complete orbits to see the periodic phenomena repeat its signature or by the lifetime of a space mission. Photometry is the only practical method for finding Earth-size planets in the continuously habitable zone. This unique search space is shaded green in the figure.

4.CONCLUSION

In final project I will concentrate on the technology currently being used or developed that will eventuallly lead to the detection of Earths. Estimates of the timescale of this endeavour suggest that by the 2010s we may possess the capability to find other Earth-sized planets and begin to ansver the question of whether or not they are suitable abodes of life.

 

 

5.REFERENCES

[1] Jean  Schneider, Extrasolar Planets Searches, http://www.obspm.fr/encycl/searches.html

update: 30 March 2004

 

[2] Stuart Clarck, Extrasolar Planets, 1998