1
00:00:00,000 --> 00:00:08,566
[MUSIC]
音乐。
2
00:00:08,566 --> 00:00:13,022
Good morning, good afternoon, good
evening, whatever time,
早上好，中午好，晚上好，啥时候都好吧，

3
00:00:13,022 --> 00:00:17,489
your enthusiasm for exoplanets is bringing
you back, welcome.
你对外星的热爱又把你带到这里，欢迎。

4
00:00:17,489 --> 00:00:21,609
In this week, during this week, we will
continue the description
在本周的时间里，我们会继续说明

5
00:00:21,609 --> 00:00:26,730
of the properties of the exoplanetary
system that have been detected.
已经探测到的外星系统的性质。

6
00:00:26,730 --> 00:00:33,470
Of course the idea is, always to bring
constraints for planet formations, making
意思是，要一直考虑外星形态存在的限制，

7
00:00:33,470 --> 00:00:36,700
the link between initial conditions and
the
在初始条件和观察到的

8
00:00:36,700 --> 00:00:40,350
observed end state of the formation
process.
经过演化进程的状态间寻找联系。

9
00:00:40,350 --> 00:00:47,220
Now we start with the properties of the
central mass in the system.
我们先从系统中的中心质量开始。

10
00:00:47,220 --> 00:00:48,060
What do we expect?
我们希望什么？

11
00:00:49,270 --> 00:00:53,470
We assume that protoplanetary discs have
masses that
我们假设初始的时候圆盘形状态是有质量的，

12
00:00:53,470 --> 00:00:56,800
are scaling with the mass of the central
star.
并且用中央的恒星作度量。

13
00:00:56,800 --> 00:00:59,770
So you form bigger stars in bigger discs.
所以可以认为越大的恒星，周围的圆盘物质越大。

14
00:00:59,770 --> 00:01:05,368
Makes sense and as at least from the core
operation scenario you need more
这可以说的过去，并且至少需要更多物质去构建核心，

15
00:01:05,368 --> 00:01:11,750
solid material to build up the core and
then gather an equation of the core.
以聚合成相等的核心？

16
00:01:11,750 --> 00:01:16,150
it seems that you should be able to do it
more efficiently in a big disk.
看起来似乎圆盘越大，构建核心效率越高。

17
00:01:16,150 --> 00:01:20,441
So for more massive planets in more
massive discs,
同样盘子越大，行星也越大，

18
00:01:20,441 --> 00:01:25,430
so have more massive planets around more
massive stars.
同样盘子越大，行星也越大，

19
00:01:25,430 --> 00:01:29,850
And actually, that's the same for the
gravitational instability approach.
事实上，这和重力不稳定性接近是一样的。

20
00:01:29,850 --> 00:01:33,750
Because to get instability, you need a
massive disc.
因为要变得不稳定，就需要一个巨大的盘子。
21
00:01:33,750 --> 00:01:37,990
So you will, with this process, form
massive planets.
所以，照着这个进程，形成巨大的行星。

22
00:01:37,990 --> 00:01:41,040
It's even probably impossible to form
重力不稳定的圆型尘埃中形成小质量行星几乎

23
00:01:41,040 --> 00:01:44,840
small mass planets with gravitational
instability.
是不可能的。

24
00:01:44,840 --> 00:01:48,230
So, the prediction we can make is that
more
因此，我们可以预言，越大质量的恒星附近更有可能找到大质量行星

25
00:01:48,230 --> 00:01:52,110
massive planets are probably found around
more massive stars.
越大质量的恒星附近更有可能找到大质量行星

26
00:01:53,120 --> 00:01:56,810
So, what do we know from the observational
point of view.
如此，我们根据观察都发现了哪些观点。

27
00:01:56,810 --> 00:02:02,830
There have been several projects targeting
low mass
目前已经有一些项目把小质量恒星

28
00:02:02,830 --> 00:02:08,750
stars and high mass stars to search for
planet and try to answer this question.
和大质量恒星作为研究目标，以尝试回答这些问题。

29
00:02:08,750 --> 00:02:16,030
And maybe the first one to mention is the
one around low mass stars and dwarfs.
首先被提及的会是在低质量恒星和矮星附近的目标。

30
00:02:16,030 --> 00:02:21,259
And I will start with [INAUDIBLE]
velocities that's programmed here,
我将会从径向速度法开始，

31
00:02:21,259 --> 00:02:25,409
that is described that has been conducted
by Xavier [UNKNOWN]
描述的是由Xavier指导的

32
00:02:25,409 --> 00:02:29,975
from The [INAUDIBLE] Observatory in
collaboration with our team in
来自于位于Geneva的合作的天文台，

33
00:02:29,975 --> 00:02:34,060
Geneva and we have fellow [INAUDIBLE] M
dwarfs from the sun.
我们跟踪M矮星

34
00:02:36,610 --> 00:02:43,590
And from these observations, we could
infer frequencies
并且由这些观察，我们可以推断在那些恒星附近

35
00:02:43,590 --> 00:02:46,080
of planets of different types around those
stars.
不同类型行星出现的频数。

36
00:02:46,080 --> 00:02:52,360
For example, we have seen that giant
planets are very rare at the level
例如，我们发现巨大行星在1%~2%等级里是非常罕见的，

37
00:02:52,360 --> 00:02:59,560
of a percent or 2 if we go out to hundred
day period.
如果周期大于100Days。

38
00:02:59,560 --> 00:03:04,150
So big planets are rare around M dwarfs
from the radial velocity survey.
从径向速度法获取结果说明大行星在M矮星附近是很稀有的。

39
00:03:04,150 --> 00:03:06,950
On the contrary, super Earths and Neptune
are very
相反，超级地球和海王星却很多，

40
00:03:06,950 --> 00:03:10,330
numerous, at the level of 50%, plus minus
20.
在50%±20%的水平，

41
00:03:10,330 --> 00:03:12,590
So that's the same type of numbers
这和我们寻找类太阳的恒星，

42
00:03:14,710 --> 00:03:18,190
than what we find for solar type stars.
相比也是有同样的数量级。

43
00:03:18,190 --> 00:03:23,410
So it's easy to form small mass planets
around small star.
所以，更容易在小质量恒星附近形成行星。

44
00:03:23,410 --> 00:03:25,600
These findings can be compared with
这些发现可以和开普勒卫星

45
00:03:25,600 --> 00:03:29,218
the results obtained with the Kepler
satellite.
为所公认的结果相比较。

46
00:03:29,218 --> 00:03:33,135
In the Kepler field, we have something
like
在开普勒的领域，

47
00:03:33,135 --> 00:03:37,320
4,000 stars with a temperature smaller
than 4000 degrees.
像小于4000°的恒星有4000个。

48
00:03:37,320 --> 00:03:41,550
And those are defining our low mass stars.
并且那些都被定义为小质量恒星。

49
00:03:41,550 --> 00:03:46,270
Courtney Dressing and David Charbonneau
from The Center for Astrophysics in Boston
天文物理学的两个波士顿的科学家，

50
00:03:46,270 --> 00:03:54,730
had a look at the sample of M stars in
Kepler and derived the fraction of
在M恒星发现了一个例子，由此推断平均每个恒星有小部分行星

51
00:03:54,730 --> 00:04:00,560
planet per star on average around M dwarfs
in the Kepler sample.
附近有M矮星。

52
00:04:02,690 --> 00:04:08,220
The results, well one of the interesting
results is that there is
关于结果，其中一个有趣的结果是，

53
00:04:08,220 --> 00:04:14,370
almost no giant planet transit in front of
M dwarfs.
几乎没有巨大行星在M矮星前发生凌日现象。

54
00:04:14,370 --> 00:04:16,335
There is only one case known and
已知只有一个案例并且

55
00:04:16,335 --> 00:04:20,060
that has confirmed by ground-based radial
velocities.
通过了基于地面的径向速度法确认。

56
00:04:20,060 --> 00:04:25,070
But most of the planets are of small size
because from the
但是，大部分行星都很小，

57
00:04:25,070 --> 00:04:28,870
transit, from the Kepler data, we measure
the size of the planet.
因为，通过凌日，通过开普勒的数据，我们可以测量行星的大小。

58
00:04:28,870 --> 00:04:36,280
And so the findings of Dressing and
Charbonneau is that if we restrict the
所以D和C的发现

59
00:04:36,280 --> 00:04:42,250
sample of planets to be smaller than 4
earth's radii, so
如果我们限制为小于4倍地球半径，

60
00:04:42,250 --> 00:04:48,152
smaller than Neptune basically, then there
is an average of .9 planet
那么经本上小于海王星，那么平均每个M矮星会有一个0.9个行星。

61
00:04:48,152 --> 00:04:54,270
per M dwarf in the sample and if we only
consider even smaller planets,
如果我们只考虑更小的行星，

62
00:04:54,270 --> 00:05:00,850
earth size planet still within the 50 day
period, then
像地球大小的行星周期仍然小于50Days，

63
00:05:00,850 --> 00:05:06,770
we have an average of .5 planet per star
[INAUDIBLE] M dwarf.
那么平均一个M矮星会有0.5个行星。

64
00:05:06,770 --> 00:05:13,290
So very clearly the the formation
因此，很明显，

65
00:05:13,290 --> 00:05:18,400
of planet around M dwarfs is favoring the
M矮星附近，

66
00:05:18,400 --> 00:05:23,380
low size planets.
更容易形成小行星。

67
00:05:23,380 --> 00:05:30,060
Now if we have a look at the other side of
the spectrum of the sun trial star mass,
现在，如果我们看一下太阳频谱的另外一边，

68
00:05:30,060 --> 00:05:34,088
we need to go to stars with 2-3 solar
我们需要到2到3倍质量的恒星，

69
00:05:34,088 --> 00:05:38,250
masses to see the difference with the
solar type stars.
才能看到与类太阳恒星的区别。

70
00:05:39,410 --> 00:05:44,760
And so on the main sequence, we go up to
the AB dwarfs,
所以按照主星序，我们看看AB矮星，

71
00:05:44,760 --> 00:05:50,290
but those are hot, high-rotation stars for
which the spectral
但是那些外星很热，转速很高，对于那些光谱很

72
00:05:50,290 --> 00:05:55,600
lines are very broadened and so it's very
difficult to detect planet around those.
宽，并且很难在他们周围探测到行星。

73
00:05:55,600 --> 00:06:00,450
So a better approach is to look at G,
所以，更好的方法是观察巨大的，

74
00:06:00,450 --> 00:06:05,140
giants, that are evolved version of these
A-type star.
那些是进化了的A型恒星。

75
00:06:05,140 --> 00:06:09,830
And here in the diagram obtained from the
Exoplanet Encyclopedia in Paris,
在这里图表中，可以从外星百科全书中得到，

76
00:06:11,730 --> 00:06:16,360
it's just a number of planet in function
of


77
00:06:16,360 --> 00:06:20,965
the mass of the central star, and we see
that for high masses,

78
00:06:20,965 --> 00:06:26,660
2-3 solar masses, there are detection,
there are several tens of them.

79
00:06:26,660 --> 00:06:31,200
So, we do find planets around giant stars.

80
00:06:32,500 --> 00:06:38,430
If we look at the same sample, but now in
a diagram showing the planet

81
00:06:38,430 --> 00:06:44,120
mass versus the star mass, we see that
most of them are massive planets.

82
00:06:44,120 --> 00:06:45,940
Of course, there is a detection bias

83
00:06:45,940 --> 00:06:50,620
here because for giant stars, because of
intrinsic

84
00:06:50,620 --> 00:06:54,780
variation of the star, it's very difficult

85
00:06:54,780 --> 00:06:58,290
with radial velocities to detect small
mass planets.

86
00:06:58,290 --> 00:07:00,920
So there is a bias, but we clearly see

87
00:07:00,920 --> 00:07:05,910
that there are a lot fo massive planets
around giants.

88
00:07:05,910 --> 00:07:09,350
So how now, can we compare?

89
00:07:09,350 --> 00:07:11,570
Because we are completely biased for these

90
00:07:11,570 --> 00:07:14,185
giant stars, we have no small planet
detections.

91
00:07:14,185 --> 00:07:20,910
So we cannot compare directly the
frequencies with other type of stars.

92
00:07:20,910 --> 00:07:29,440
So what we can do is to consider the total
mass on the, the form of planets,

93
00:07:29,440 --> 00:07:35,349
the normal planetary mass in the system
normalized by the number of stars

94
00:07:37,730 --> 00:07:41,410
that is in the given bin of star mass.

95
00:07:41,410 --> 00:07:44,190
So, we can roughly make 3 big bins.

96
00:07:44,190 --> 00:07:46,560
We have the small mass stars, the M
dwarfs.

97
00:07:46,560 --> 00:07:49,680
We have the solar type stars, and we have

98
00:07:49,680 --> 00:07:53,840
the more massive stars, the evolved stars,
the giants.

99
00:07:53,840 --> 00:07:57,000
And in each bin, we put the total mass of
the

100
00:07:57,000 --> 00:08:01,410
planets and we normalize by the number of
stars in each bin.

101
00:08:01,410 --> 00:08:03,550
And you obtain this figure that was made

102
00:08:03,550 --> 00:08:07,840
by my colleague [UNKNOWN], a few years
back.

103
00:08:07,840 --> 00:08:15,640
And that very clearly shows how the
content under the form of planet, the, the

104
00:08:15,640 --> 00:08:18,830
material under the form of planet is

105
00:08:18,830 --> 00:08:21,400
increasing with the mass of the primary
star.

106
00:08:23,010 --> 00:08:27,630
So the mass of planetary material scales
with the mass of the star.

107
00:08:29,930 --> 00:08:35,420
And again, if we come back as you already
have seen this slide

108
00:08:35,420 --> 00:08:40,450
before in the course, that's the detection
of very massive

109
00:08:40,450 --> 00:08:45,440
planet in the outer regions of systems of
massive stars.

110
00:08:45,440 --> 00:08:51,310
They are A Stars and the detection have
been made by direct imaging.

111
00:08:51,310 --> 00:08:53,360
Of course if they are massive and far from

112
00:08:53,360 --> 00:08:58,940
the star, it's easier to detect the planet
through imaging.

113
00:08:58,940 --> 00:09:03,570
But if those planets would exist around
smaller mass stars, it

114
00:09:03,570 --> 00:09:08,810
would even be easier to detect them and we
do not.

115
00:09:08,810 --> 00:09:13,770
So it seems that these massive stars have,
are

116
00:09:13,770 --> 00:09:17,890
favorable place for the formation of these
big planets outside.

117
00:09:17,890 --> 00:09:24,140
And there is even another case where the
central star is a B9,

118
00:09:24,140 --> 00:09:29,645
it's compound [INAUDIBLE], and that there
is a companion of the level of

119
00:09:29,645 --> 00:09:35,230
12-13 Jupiter masses at 55 AU from the
central star.

120
00:09:35,230 --> 00:09:39,460
So, are those system very common or not?

121
00:09:39,460 --> 00:09:42,889
That's a very important question because
planet formation scenario

122
00:09:42,889 --> 00:09:45,960
based on the core [UNKNOWN] have
difficulties to form them.

123
00:09:45,960 --> 00:09:49,910
So, you can form maybe the planet in the
inner region of the

124
00:09:49,910 --> 00:09:51,590
system and have the planet move

125
00:09:51,590 --> 00:09:55,490
outside by migration, by planet-planet
interaction, all,

126
00:09:55,490 --> 00:10:02,150
all type of processes that can happened,
but if most of those stars

127
00:10:02,150 --> 00:10:06,056
have these planets, then it's starting to
be difficult to explain it this way.

128
00:10:06,056 --> 00:10:11,820
So, the statistics about the massive
planet in the outer region

129
00:10:11,820 --> 00:10:16,570
of massive stars will be an interesting
question to be addressed by the

130
00:10:16,570 --> 00:10:23,250
new generation of planet imager that are
being installed these days on the

131
00:10:23,250 --> 00:10:30,150
large telescope G pie on Gemini, and a
sphere on the VAT.

132
00:10:30,150 --> 00:10:36,831
And maybe in the next version of the book,
we will have results on these aspects.

133
00:10:36,831 --> 00:10:37,418
Thank you.

134
00:10:37,418 --> 00:10:44,379
[MUSIC]


