Caption: The statistics for confirmed exoplanets (which we usually just call planets since that is what they are) given in the graphs are from the EPE Diagrams page of The Extrasolar Planets Encyclopaedia (EPE). The statistics were current circa 2021 Jul10 and are mostly from discoveries by Kepler spacecraft (main mission 2009--2013, K2 mission 2013--2018).
However, TESS (Transiting Exoplanet Survey Satellite, 2018--) is actively discovering exoplanets, and so there will be thousands more confirmed exoplanets in a few years if NOT sooner.
As of circa 2021 Jul10 there 3540 confirmed planetary systems and 4785 confirmed exoplanets (see The Extrasolar Planets Encyclopaedia: Catalog).
Note EPE used to allow inline linking to their graphs, but they have eliminated that useful feature, and so yearly downloadeds of updated graphs are now needed.
Graphs (i.e., Plots):
This semi-log plot was obtained from EPE: Diagrams: y-axis: year of discovery versus x-axis: log semi-major axis (i.e., mean planet orbital radius).
Features:
Recall astronomical unit (AU) = 1.49597870700*10**11 m.
Emphasis: These are NOT ordinary planets orbiting ordinary stars. They pulsar planets orbiting a pulsar: i.e., a radio pulsating neutron star.
This is a log-log plot.
Note that the stellar masses
are clustered around
1
solar mass (M_☉).
Remember that we are looking for
life as we know it,
and so there is a preference for observing
stars
that are like the Sun,
and so have about
1
M_☉.
The preference may be wearing off at least in the direction of lower mass
stars since it is now
known that they usually do have lots of
planetary systems
(e.g.,
Dressing & Charboneau 2013) some
which might be habitable.
In the direction of higher mass stars
the observational preference is probably still there.
Recall the trends for
main sequence stars
from the
Main-sequence rule:
So the more massive the star, the
shorter its lifetime on the main sequence
and the less time life as we know it has to evolve.
So our hypothesis is that larger the mass, the less likely there is to be
life as we know it.
Also going to larger stars increases
the same biases against discovery as going to smaller
planets for the same
reasons mutatis mutandis.
The upshot is that
we don't look at more massive stars too much in
the search for
planetary systems.
Note that stars
more massive than about 8 solar masses
(i.e., 8 M_☉) live only
a few million years on the
main sequence and explode
as
core-collapse supernovae---which is highly
inimical
for life as we know it.
There is a bimodal distribution
(i.e., one with Twin Peaks).
This observed distribution is probably very unrepresentative the real distribution.
Remember the two main
methods of detecting exoplanets
have a bias toward finding larger exoplanets.
Doppler spectroscopy is biased toward more massive
exoplanets and the
transit method
toward larger-radius exoplanets.
The two biases are NOT the same, but they are strongly correlated:
mass and radius tend to increase together.
But there are other factors.
For example, a more massive planet can
have smaller radius than less massive planet if it is sufficiently colder or made of sufficiently
denser materials.
The bias to larger larger exoplanets
partially explains the peak centered at about
1.2 Jupiter radii.
Why there is another peak centered at about
0.2 Jupiter radii,
yours truly doesn't know.
Probably some observational bias.
In the near future, the distribution will probably look quite different as
thousands of candidate
planets are added to the plot.
Yours truly suspects
the emerging new observed distribution that is better representative of the real
distribution will have only one peak.
One distribution corrected for bias is roughly flat from
about 0.1 Jupiter radii to
0.25 Jupiter radii, then
declines sharply to about 0.35 Jupiter radii
and then declines more slowly
(see Howard 2013, p. 5).
But this corrected distribution is far from being the last word.
See below for this is a log-log plot.
The fact that most points lie nearly on a straight line agrees with
Kepler's 3rd law which
has the formula
The shown plot is a band, NOT a line, because the
host star mass varies and
because of gravitational perturbations
in non-two-body systems.
This is a log-log plot.
The bias toward finding larger mass
planets close to
host stars
(i.e., with about 1 AU) is evident.
Other explication will have to wait until yours truly knows more.
This is a log-log plot.
The bias toward finding larger radii
planets close to
host stars
(i.e., with about 1 AU) is evident.
Other explication will have to wait until yours truly knows more.
M ↑, R ↑, L ↑, T_photosphere ↑ t_lifetime ↓ f ↓
which means that as stellar mass M increases,
stellar radius R increases,
luminosity L increases,
photospheric temperature increases,
main-sequence lifetime decreases,
and frequency f (see Wikipedia: Initial mass function) decreases.
P=[2π/(GM)**(1/2)]*R**(3/2) ,
where P is orbital period,
M is the host star (assumed much larger than the
planet mass),
G is the gravitational constant,
and
R is the mean orbital radius
(AKA the semi-major axis).
On a log-log plot, one gets
the linear relationship between logarithmic period and logarithmic radius
log(P)=(3/2)*log(R) + constant.