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00:00:01
[music]
00:01:08
Well, let's start 21 minutes, it seems,
00:01:12
Good evening, that means Today we are
00:01:16
finishing this extragalactic part, we are
00:01:18
slowly moving on to cosmology in the
00:01:20
second half of the pair And next time
00:01:22
we have two pairs We are agreeing on
00:01:25
cosmology and accordingly 24
00:01:28
are arranging a class
00:01:31
I will ask you
00:01:33
Please tell your colleagues this can
00:01:39
be useful Well, it’s useful for me And it’s
00:01:41
useful for you next time people
00:01:43
came to the maximum
00:01:45
Well, firstly, I’m interested to see
00:01:47
when there are a lot of you, and
00:01:50
secondly,
00:01:52
look at what the reason is, it’s more
00:01:54
practical,
00:01:55
it means Thanks to Vsevolod, the lecture
00:01:58
is being laid out, but the
00:02:00
last lecture should be posted right away, he’s
00:02:03
obviously won’t be able to
00:02:05
and therefore And she will have a lot of everything on the
00:02:08
test. Well, that is, no, there will be a decent
00:02:10
number of tasks from the last two pairs.
00:02:12
Therefore, so that people do not find themselves in a situation,
00:02:14
someone can quite rightly
00:02:16
assume that they will all look at the video
00:02:18
Well, there, except for the first two lectures and this is
00:02:21
kind of normal and good. I don’t argue with
00:02:23
this, but they won’t watch the last lecture before the test
00:02:25
on video; they just won’t have time to do it.
00:02:28
And that’s why they can run
00:02:31
into some pretty difficult assignments. Well,
00:02:34
for me, at least,
00:02:35
so I would suggest you tell
00:02:39
your colleagues why I mean, they
00:02:41
’ll see this video in a week. It’s good if as
00:02:45
many people as possible come
00:02:48
and, accordingly, if there are any
00:02:51
questions about the test, as usual, you can
00:02:54
ask me now and at the next
00:02:56
lecture, when a lot of people come there, I’ll do
00:02:58
something too I answer well, all this
00:03:01
is clear then let’s move on to the
00:03:04
electronic part, which means last time we
00:03:07
started talking about extraclactic
00:03:09
astronomy, today we are finishing we
00:03:11
said that
00:03:13
from the point of view of matter,
00:03:17
dark matter dominates, the
00:03:19
fundamental difference is that
00:03:21
although dark energy generally dominates,
00:03:24
dark energy cannot be collected in
00:03:26
a heap, that is, it acts in the Universe But
00:03:29
even two and a half forces, let
00:03:32
’s say, there would be no dark energy
00:03:35
at all, so we thought 25 years ago, but
00:03:39
not all But most people don’t
00:03:41
have any dark energy.
00:03:43
So, our Universe at the beginning began
00:03:46
to expand, we and a little bit with you
00:03:48
next time, and this time we’ll talk about
00:03:50
why
00:03:51
we also have counteracting forces
00:03:54
of gravity, that is, matter tries to
00:03:56
gather together under the influence of its
00:03:57
own gravity and resists
00:03:59
this expansion. That is, all structures
00:04:01
in the Universe grow in spite of the expansion of
00:04:04
the Universe; these are two main
00:04:06
opposing forces, especially in the
00:04:08
first half of the life of the Universe, now
00:04:10
there is still dark energy, which
00:04:12
additionally leads to the effect of such,
00:04:14
if you want, repulsion, in fact,
00:04:16
it’s not exactly repulsion of
00:04:20
objects from each other, of course, but the
00:04:23
Metric of the Universe is changing in such a way
00:04:26
that the expansion proceeds at an increasingly faster pace and,
00:04:29
accordingly, against the background of this
00:04:31
accelerating expansion continue to
00:04:34
grow the structure at the beginning I repeat there
00:04:36
was no accelerated expansion of the structure
00:04:38
growing now they also continue to grow
00:04:40
this makes it difficult accordingly
00:04:44
this structure is something that consists of a
00:04:47
substance of ordinary and dark
00:04:49
ordinary substance It has such good
00:04:52
deseptic characteristics, that is, it knows
00:04:54
how to cool down it can
00:04:55
get rid of effectively moment of
00:04:58
rotation and therefore can form
00:05:00
compact structures like you and me,
00:05:03
dark matter, due to the weak
00:05:06
interaction between particles,
00:05:08
cannot do this, therefore dark matter
00:05:11
does not dominate within the physics
00:05:14
department of the city of Moscow, planet Earth of
00:05:18
the Solar System and even the disk of the Galaxy is
00:05:23
more complex. Of course there is a rotation curve there the
00:05:26
contribution of dark matter is large in
00:05:28
the central parts, well,
00:05:31
dark matter itself does not dominate, but on
00:05:33
large scales, starting from the scale of the
00:05:35
full size of the Galaxy, dark
00:05:37
matter dominates, so this skeleton of
00:05:40
the Universe is the result of numerical
00:05:41
modeling with a very large scale,
00:05:44
this segment is 125 megaparsecs Well,
00:05:48
that is, there approximately half a billion
00:05:49
light years in a ruble, on this
00:05:52
scale, structures are mainly composed of
00:05:54
dark matter, and when the
00:05:57
first
00:05:59
computer simulations were carried out to model the
00:06:01
formation of a large-scale structure,
00:06:04
in essence, we can say that they considered
00:06:06
dark matter as one, not that they forgot about the
00:06:09
ordinary ones, just ordinary dark ones were put
00:06:11
in one pile and did not reach the
00:06:13
scale where the role of
00:06:15
ordinary matter becomes important when, firstly,
00:06:18
very compact structures can arise And
00:06:20
secondly, when these contact structures
00:06:22
give feedback, ordinary matter
00:06:24
can form stars, it can
00:06:25
trigger the work of quasars and all this
00:06:27
injects energy back stars
00:06:29
explode alone
00:06:31
Stellar winds, quasars emit a lot and
00:06:35
can also launch such a wind, there are
00:06:36
powerful jets there and this affects the
00:06:40
scale of the
00:06:41
inner part of the Galaxy, let’s say, but
00:06:44
on such large scales
00:06:46
dark matter dominates and let me remind you that it is very
00:06:48
important that dark matter could begin to
00:06:51
create this structure early because it
00:06:53
does not participates in electromagnetic
00:06:55
interaction, and in the era of radiation dominance,
00:07:01
dark matter could already create
00:07:03
compact structures, and therefore, when
00:07:05
ordinary matter also received this
00:07:07
opportunity after the era of combination,
00:07:10
ordinary matter turned out to be
00:07:12
unable to when there are only small
00:07:13
fluctuations, the fluctuations were already quite
00:07:15
large because they this time
00:07:17
they have grown in dark matter and for the
00:07:20
last time I will repeat this skeleton of
00:07:22
the Universe mainly consists of dark
00:07:25
matter, such large areas are a cluster of
00:07:28
galaxies, the matter continues to flow along the fibers in a
00:07:30
cluster of galaxies,
00:07:33
that is, today a cluster of
00:07:35
galaxies are those objects that
00:07:36
continue to form. Is it possible to
00:07:39
see this skeleton People are trying very hard in the Universe,
00:07:43
for this they need to learn to see dark
00:07:45
matter at least by indirect methods But
00:07:47
this is the first result This is quite a
00:07:49
long time ago 10 years ago This is the first
00:07:51
rib from the first bone from this
00:07:54
skeleton of the Universe that they managed to
00:07:56
see a
00:07:57
cluster of galaxies and the contours can be
00:08:01
seen here the contours show
00:08:03
the distribution mass, no matter what it is
00:08:07
created by. Because these contours
00:08:08
are built according to the effect of weak
00:08:10
gravitational lensing, that is, they
00:08:12
generally describe the curvature of
00:08:13
space in this area. Well, since
00:08:16
we are within the framework of the assumption that
00:08:18
this curvature is entirely due to
00:08:20
some kind of mass, this means that this is the distribution
00:08:24
of mass and we see that of course the cluster
00:08:28
itself contains more matter than between them, but
00:08:31
between them there is also a lot of matter
00:08:33
and it does not manifest itself, that is,
00:08:37
it does not emit, and this means that
00:08:40
thanks to weak lensing it
00:08:42
was possible for the first time to reveal what was
00:08:44
naturally predicted by the theory
00:08:47
that clusters of galaxies are connected
00:08:51
such fibers, filaments, channels like
00:08:55
me Name in which dark
00:08:57
matter dominates, ordinary matter is also there
00:08:59
in the form of such a warm gas that gives
00:09:02
very little radiation does not form stars,
00:09:04
so you see it is quite difficult, in
00:09:07
principle, you can detect its
00:09:08
presence not now so in the future
00:09:11
But in general the distribution the masses by
00:09:14
the lead are determined quite well; the
00:09:16
same structures can exist between
00:09:18
galaxies, but they are less pronounced. Therefore,
00:09:21
in this work five years
00:09:24
ago, people went a slightly different
00:09:26
way, they took several
00:09:31
pairs of galaxies under a hundred, in my opinion it was not
00:09:34
written
00:09:35
there, there was a park of galaxies for about a hundred for
00:09:38
each individual pair
00:09:43
I apologize for each individual pair to
00:09:46
draw out by weak lensing This
00:09:48
fiber does not work, but by summing up
00:09:50
the results
00:09:51
it is possible to achieve the desired result, that
00:09:55
is, again the distribution of
00:09:56
mass is shown and it is clear that the Galaxies are connected by
00:10:00
such filaments that are not visible from
00:10:04
direct observations of electromagnetic
00:10:06
waves nothing there is not detected, but
00:10:08
when you process
00:10:11
data on a large number of
00:10:13
galaxies, then such a thing shows up
00:10:16
well. So there are a
00:10:19
huge number of hypotheses about what dark matter could be. That
00:10:21
is, you can read a whole course about it and
00:10:24
maybe in cosmology departments people
00:10:25
do this, we have it in our cosmology departments
00:10:28
Directly super specialists on these
00:10:32
issues at the beginning It’s easier to say than it can’t be the
00:10:35
very first thing that people understood, but
00:10:37
somewhere in the 90s it can’t be
00:10:40
baryons of any kind. That is, it can’t
00:10:43
be there; there’s dust, compact remnants of stars
00:10:47
that it can’t be can't be there
00:10:50
hot warm cold any gas
00:10:53
ordinary matter we throw out the
00:10:55
next step throws out everything that is in the
00:10:58
standard model of particle physics
00:11:00
so the most popular
00:11:03
models for describing dark matter are
00:11:07
particles not included in the standard model
00:11:11
particles that can be
00:11:13
naturally produced in the early universe
00:11:17
and particles such that they do not participate
00:11:20
at least so clearly and well in
00:11:23
electromagnetic interaction, by the way, it is
00:11:25
not necessary that they do not
00:11:27
participate at all. For example, Xiaomi are
00:11:29
candidates for particles of removable matter,
00:11:32
axions can interact with a
00:11:34
magnetic field, there is a wonderful
00:11:35
Primakov effect,
00:11:36
but it’s just a very weak
00:11:38
interaction here weak means not
00:11:40
intense, not like weak nuclear, but
00:11:43
there are other Models there have been the
00:11:46
most popular for a long time And maybe now there
00:11:48
was a neutralin model, that is, we are talking
00:11:51
about neutral super partners of ordinary
00:11:54
particles And neutralin is not a separate
00:11:57
superposition particle, be that as it
00:11:59
may, if it some
00:12:01
particles You can take a specific
00:12:04
hypothesis and see what is predicted
00:12:06
for this particle See Can you
00:12:09
somehow detect the presence of
00:12:11
these particles of the main ideas two or
00:12:13
particles interact with themselves in
00:12:16
space or with ordinary matter in
00:12:18
space and you observe what -these effects
00:12:21
That is, these are astronomical
00:12:22
detection methods or you catch particles
00:12:25
right in the laboratory, that is, you observe
00:12:28
some laboratory processes associated
00:12:30
with the interaction of particles of dark
00:12:32
matter with ordinary matter; the detector,
00:12:36
respectively, if we are talking about
00:12:39
astronomical methods, the most
00:12:41
popular is the search for annihilation
00:12:44
in many models
00:12:46
particles of dark matter, particles can
00:12:49
annihilate each other, but for
00:12:52
this it is not necessary that they have a
00:12:53
positive and negative charge there. As
00:12:55
you understand, there are no zones that perfectly
00:12:56
annihilate each other, they are
00:12:58
particles themselves, and at the same time normal
00:13:02
quanta of electromagnetic radiation are born and in
00:13:06
most popular models
00:13:09
it turns out that the energy of these banks
00:13:12
falls into the gamma range, which is
00:13:14
good, even because there are
00:13:16
not so many sources in the gamma range. And therefore there is
00:13:19
hope of detecting extra
00:13:21
gamma radiation, which cannot be
00:13:22
explained by anything else. Where to look. So,
00:13:25
first of all, you need to look where there is more
00:13:27
darkness substances because the probability of
00:13:30
interaction of particles is proportional to the
00:13:31
square of their density,
00:13:34
respectively, you can look at the center of
00:13:36
our galaxy in the center of
00:13:38
some nearby galaxies or look for a common
00:13:41
intercom, this is a simulation of a
00:13:43
large-scale structure, a general background from the
00:13:45
entire Universe, you can look for an extra homophone in
00:13:48
this way people do it all the time
00:13:50
and with enviable
00:13:56
irregularly but with such repeating
00:13:59
frequency, results appear
00:14:01
when people
00:14:03
claim that they see a gamma signal
00:14:07
which, in their opinion, is not explained within the
00:14:10
framework of standard astrophysical
00:14:12
models, as a rule, it all
00:14:13
resolves after more or less
00:14:16
time, resolves in rare cases
00:14:18
due to the fact that people check the
00:14:22
analysis itself and find there are errors. That is, there is
00:14:24
simply no extra signal, but more often it
00:14:27
resolves because it is possible to find
00:14:29
astrophysical candidates for the creation of
00:14:32
this extra gamma radiation,
00:14:35
respectively, if we leave aside
00:14:39
such indirect astronomical
00:14:42
searches, that is, direct laboratory
00:14:45
searches about LX, I won’t talk about there was
00:14:48
Hope, but nothing there have not been found and are unlikely to be
00:14:52
found associated with dark matter,
00:14:53
but there are a large number of underground
00:14:55
laboratories, this is an abstract picture at
00:14:58
first glance, this is a diagram of an underground
00:15:01
laboratory Grand sasa This is the mountains
00:15:03
from above And this is a plan of a
00:15:05
complex of halls and tunnels under the mountain in
00:15:09
order to be shielded from the background of
00:15:11
external particles accordingly, there are
00:15:14
several large halls where there is a wide
00:15:16
variety of equipment, the
00:15:18
operation of which requires such
00:15:20
powerful protection from cosmic rays, and in
00:15:24
such laboratories Granzasa is not
00:15:26
the only one
00:15:27
in such laboratories there is quite a
00:15:29
lot there, there are about a dozen detectors in the world
00:15:31
that search for particles of
00:15:34
removable matter using different methods, a
00:15:36
noticeable part of these experiments
00:15:40
is that people want to
00:15:43
observe the scattering of particles of dark
00:15:45
matter; they must be quite
00:15:46
massive; scattered particles of dark
00:15:49
matter on the
00:15:50
substance of the detector;
00:15:52
and accordingly, the
00:15:55
techniques of these experiments are being improved; at the beginning it
00:15:58
was very popular because
00:15:59
they were very expensive experiments;
00:16:01
the rate was very high Well, in general, this is a
00:16:04
job. It’s clear that there is a complex of
00:16:05
underground laboratories, it must be
00:16:07
used, there are some clear
00:16:08
methods, you choose from several
00:16:11
projects, there were always many that are
00:16:14
better, you implement it, it’s not super
00:16:16
big money, but gradually it
00:16:18
comes to larger and more
00:16:20
expensive installations, so probably
00:16:23
the number of detectors decreases over
00:16:25
time, but the quality increases,
00:16:29
one of the
00:16:32
last such large bursts was the
00:16:35
year 17, when an
00:16:40
inexplicable gamma signal from
00:16:44
Andromeda was announced. Here it is, the Andromeda Nebula,
00:16:47
but in the end it was possible to explain it and the
00:16:51
excess of gamma
00:16:53
radiation from the central part of our
00:16:55
galaxy is constantly discussed here, the main candidates for
00:16:58
explaining the excess are almost always
00:17:00
millisecond pulsars; they are also
00:17:03
sources of gamma radiation and,
00:17:05
accordingly, a fairly large
00:17:07
population of pulsars. This can
00:17:08
explain everything, but inevitably, I would say that
00:17:12
every new large
00:17:14
cosmic gamma observatory is
00:17:16
necessarily included in the program as an important point in the search for a
00:17:19
migration signal, that is new
00:17:22
large observatories should be there,
00:17:23
say, an order of magnitude more sensitive than the
00:17:25
previous ones, so what is interesting
00:17:28
is important. It is very possible to open in gamma. And in
00:17:30
gamma, two super things can be discovered: the
00:17:32
annihilation of dark matter and the evaporation of
00:17:34
primary blacks.
00:17:36
Accordingly, these tasks are
00:17:38
necessarily included. Although of course they are
00:17:41
impossible to some extent make them
00:17:43
the main ones because most likely they wo
00:17:45
n’t find anything But fortunately there are a lot of gamma sources
00:17:48
And therefore there are always a lot of main tasks
00:17:50
You have a huge number of
00:17:53
different objects of interesting physicists that
00:17:55
are interesting to study, so the gamma-ray
00:17:58
observatory is not launched for this purpose,
00:17:59
please, first of all, to
00:18:01
discover the
00:18:03
annihilation signal or the signal from
00:18:06
final stages of evaporation of black holes But
00:18:08
this, of course, is always very attractive,
00:18:11
perhaps
00:18:13
good. So let’s summarize some results
00:18:16
about dark matter. So,
00:18:20
dark matter manifests itself on the
00:18:24
scale of the Galaxy cluster; individual
00:18:26
galaxies; based
00:18:27
on the results of lensing, we see the
00:18:31
distribution of mass up to the
00:18:34
mass between galaxy clusters;
00:18:38
dark matter is an extremely important
00:18:41
ingredient modeling the growth of the
00:18:42
large-scale structure of the Universe and
00:18:45
finally, we have
00:18:48
different methods for estimating the total density of
00:18:51
the Universe, but for example,
00:18:53
we estimate the total density thanks to data on the cosmic
00:19:01
microwave background radiation, we can limit the share of baryonic matter by nucleosynthesis and we are left with an
00:19:03
inexplicable piece, and then this is dark
00:19:07
matter and the beauty is that that all this
00:19:09
together is perfectly explained by one
00:19:11
hypothesis, I repeat, that we have one
00:19:14
type of dark matter, this could be 1
00:19:17
type of
00:19:20
very stable or
00:19:23
very stable or very
00:19:25
stable elementary particles, the theory
00:19:28
predicts the existence of a whole
00:19:30
set of such particles, there is plenty to
00:19:32
choose from, therefore I would say that
00:19:36
[music] a
00:19:37
huge complex of various
00:19:39
observational data over time. Only
00:19:42
more and more strongly testifies in
00:19:45
favor of the fact that the dark
00:19:46
matter hypothesis is the best, but at the same time It
00:19:49
remains a hypothesis, the hypothesis is not
00:19:50
the only one, there is a competitor,
00:19:52
accordingly, what we hope for.
00:19:55
First of all, I would said that first of
00:19:58
all, on the detection of the results of
00:20:01
annihilation, it could be excess
00:20:03
gamma radiation, it could be personal
00:20:04
antiparticles as a result of annihilation, they are not
00:20:07
necessarily just born, you can
00:20:09
have a couple of particles of antiparticles and an
00:20:12
excess of antiparticles can also be
00:20:14
explained by this, it was a
00:20:16
wonderful job, I don’t remember 10 years
00:20:19
ago probably at the first lectures I
00:20:21
talked about this experiment, this is
00:20:23
Pamela’s experiment,
00:20:26
we observed them, in particular, positrons in
00:20:30
cosmic rays,
00:20:32
it was on a small satellite, resource
00:20:35
D as an additional load,
00:20:36
the satellite is needed for something completely different, and they
00:20:39
discovered an excess of positrons, this
00:20:41
simply caused a flurry of publications, I don’t know
00:20:44
there are a hundred in a week something like that
00:20:47
because it could be
00:20:49
explained in particular by dark matter and
00:20:53
it was extremely interesting and the search for an
00:20:55
antiparticle is one of the clear
00:20:57
opportunities to also detect an extra
00:21:00
animation signal and in this sense
00:21:02
it relates to the evaporation of black matter but
00:21:06
positrons were successfully explained Although not
00:21:09
completely, that is, there is no final
00:21:10
confirmation. But it turns out that this is
00:21:12
very successfully explained by the work of
00:21:14
pulsars.
00:21:15
As you remember, when
00:21:17
a radio pulsar operates, first of all it does
00:21:19
not emit radiation, but the parent
00:21:21
wind of particles and basically these are
00:21:24
electron positrons, respectively,
00:21:27
extra electronics, it is difficult to find them and there are so
00:21:29
many of them it’s easy to find extra positrons
00:21:31
because there are few of them, so I
00:21:35
think this will happen earlier, but reliable
00:21:37
registration of dark matter particles is,
00:21:39
of course, laboratory registration, so
00:21:41
even if there are very reliable data on
00:21:45
registration of the migration signal,
00:21:48
nevertheless, laboratory experiments will not only
00:21:50
not stop, but on the contrary, they may
00:21:52
begin carry out more intensively
00:21:54
because the range of parameters will narrow,
00:21:56
the disk will become clear,
00:21:57
well,
00:22:00
let's move on, let's
00:22:02
look again, let's see,
00:22:06
let's see
00:22:08
This is a rather old video
00:22:10
showing the growth of a cluster of galaxies, a
00:22:15
group of galaxies is better to say These are not
00:22:18
clusters, in fact, the formation of large
00:22:20
Galaxy and its satellites
00:22:22
on the left, the results were of modern
00:22:24
modeling
00:22:26
The Galaxy is being formed as a result of the
00:22:27
merger of a large number of dark heads, that
00:22:31
is, all that you see in this
00:22:33
picture, by and large, this dark
00:22:34
matter, in fact, I repeat, there are
00:22:38
5/6 of dark matter, 1/6 of ordinary
00:22:41
matter, but ordinary matter here
00:22:43
behaves the same way as dark matter
00:22:45
doesn’t manifest itself in any way, but it was necessary to move on and in the
00:22:49
last 10 or so years people have
00:22:52
made very big steps in this
00:22:54
direction, the
00:22:55
first large such program, there were
00:22:57
several of them in the world, now
00:22:59
there was a program and the idea was
00:23:03
that you carry out modeling for a very
00:23:06
large volume, that is one that is
00:23:09
already quite homogeneous The Universe is
00:23:12
heterogeneous on a small scale Yes, somewhere
00:23:14
there is Moscow where you have practically nothing
00:23:19
on a large scale on the scale of hundreds of
00:23:22
millions of light years let's say the Universe
00:23:24
becomes homogeneous we model
00:23:26
such a large scale and model it
00:23:28
from primary fluctuations somewhere
00:23:31
red displacement 30 from the first from the
00:23:34
first ten million years of the life of
00:23:36
the Universe to the present day, people did this
00:23:39
50 years ago, it is important to what level you
00:23:41
reach what resolution do you find the
00:23:44
level you have
00:23:47
n’t reached yet, but have reached the level of details
00:23:50
of the Galaxy This was an important step
00:23:52
modeling the chandelier They could
00:23:55
simulate in their program the
00:23:58
evolution of a huge number of galaxies, groups of
00:24:00
galaxies, clusters of galaxies,
00:24:02
superclusters of galaxies, and
00:24:05
in these pictures this is shown
00:24:08
accordingly, the history of
00:24:12
three galaxies is shown here, time goes from left to right,
00:24:15
time is scaled through
00:24:18
redshift Z5 Z4 Z3 Z2 Z1 z0 this is
00:24:23
our time
00:24:24
Z1 says that between this
00:24:28
cell the Universe stretched twice
00:24:33
and, accordingly, Z5 says that
00:24:35
between this and this cell the
00:24:37
Universe stretched 6 times, that is, the
00:24:39
coefficient Z plus 1,
00:24:42
and here it is shown what
00:24:45
the Galaxy really looks like in ordinary matter. That
00:24:48
is, this is no longer dark matter and the
00:24:51
modeling takes into account that Well, of course,
00:24:53
not at the level of an individual star, but
00:24:55
it is taken into account that stars are born, they
00:24:58
can explode as supernovae,
00:25:00
eject matter, emit energy,
00:25:01
impulses into the external environment,
00:25:04
quasars can be launched, that is, the
00:25:06
reverse influence of matter on the
00:25:09
dynamics of the formation of the Galaxy is taken into account, so
00:25:11
we see How
00:25:13
the appearance of the Galaxy is changing, here there is
00:25:16
clearly rapid star formation, see
00:25:19
no obvious bulge yet,
00:25:21
many star formation regions have not stood out. Everything
00:25:23
has a rather complex shape, so the
00:25:25
Galaxies are slowly standing out. The
00:25:27
central part, and finally it
00:25:28
becomes a galaxy like this. The
00:25:32
colors we see around here are not chosen randomly. this
00:25:36
really corresponds to the
00:25:37
visual image of galaxies, that is,
00:25:40
yellow stars give such a
00:25:42
blue color, if there is dust,
00:25:46
it gives us redness, such, that
00:25:49
is, the resolution has been brought up, this is very important
00:25:51
to the resolution that the
00:25:53
Hubble telescope gives for distant
00:25:55
galaxies. You can compare the results of
00:25:58
calculations with real galaxies
00:26:01
and this, of course, was a big step forward and
00:26:03
I repeat. It’s good that there are several
00:26:05
such programs, they just check each
00:26:07
other, here again the growth of
00:26:11
several large galaxies is shown, here is a
00:26:18
Galaxy that will become a disk spiral like ours. Here is a Galaxy that will become a disk one. But
00:26:20
cool, and here is a Galaxy that
00:26:22
will become electric Pay attention in the
00:26:24
past They were all so very
00:26:26
curly. Well, that
00:26:29
is, you can understand how you go on the subway. And there are
00:26:31
three guys sitting there,
00:26:35
about 50 years old, like me, and now they are so
00:26:39
neat, some may be
00:26:41
partially bald, but you are not you know
00:26:43
what they were like there 20 years ago,
00:26:45
maybe they wore dreadlocks, Iroquois,
00:26:48
something else, it was some kind of stormy
00:26:50
youth, maybe it wasn’t and it was
00:26:52
unlucky, but there were always galaxies
00:26:54
And
00:26:56
now we can better understand how this
00:26:59
happens, compare it with using observations
00:27:01
to correct theoretical models. That
00:27:03
is, this is such a normal way
00:27:05
of cognition when the result, in principle,
00:27:06
is a model.
00:27:08
We want to understand, we need to get this into our
00:27:11
head. Or at least draw
00:27:12
pictures to understand how they draw with a
00:27:14
computer. But since we can’t do this right away,
00:27:17
we could be wrong. then
00:27:20
we need to compare with observations
00:27:21
When you achieve
00:27:23
ideal matching, you seem to be saying
00:27:26
that at home we understand everything well, here
00:27:36
you can see the beautiful results of mergers. That is, all these strange arcs and sleeves, first here, but here, too, you can see these are the results of the merger of the Galaxy with
00:27:39
quite massive satellites
00:27:41
incomparable in mass of the Galaxy itself but
00:27:44
quite massive which give such
00:27:46
beautiful large details,
00:27:49
respectively, I repeat that everything can be
00:27:51
calculated from primary fluctuations, that
00:27:54
is, from very large scales to the
00:27:55
formation of
00:27:56
individual galaxies with their satellite, you
00:28:00
can calculate the formation of galaxies of
00:28:03
different types, that is, compare with
00:28:05
observations to determine share of galaxies
00:28:06
of different types,
00:28:08
all the Galaxies at our moment are shown here
00:28:10
as they are reproduced and chandeliers
00:28:13
are disk Galaxies here all the
00:28:17
spirals are shown enviable No there are
00:28:20
elliptical Galaxies it is clear that there is
00:28:23
no blue color here because there
00:28:25
is no fresh star formation all the gas
00:28:27
is in such a shape in such a
00:28:29
state that the
00:28:31
Jeans mass is very large and
00:28:34
therefore the formation process does not proceed
00:28:36
and various irregular galaxies are
00:28:39
obvious results of recent mergers
00:28:41
to galaxies there with some very vigorous
00:28:45
star formation that ultimately show
00:28:48
such an irregular structure,
00:28:52
such a problem existed for a long time The
00:28:55
problem of the properties of our local group of
00:28:59
galaxies could not be solved combine
00:29:02
the result of calculations with observational data,
00:29:05
in fact, what is the problem, how does this
00:29:08
bright beautiful picture differ from
00:29:10
this one, here the dark matter
00:29:12
in the local group of galaxies is shown, remember the
00:29:14
local group, this is us, fog from Andromeda,
00:29:16
big things clouds Galaxy in a
00:29:17
triangle, but there are still many all sorts of
00:29:19
satellites, sometimes with beautiful ones with
00:29:21
rather boring names M32
00:29:24
here shows dark matter if we
00:29:27
saw it. But this is what it really is
00:29:30
and, accordingly, two large
00:29:33
Galaxies are visible, but also every little thing,
00:29:35
it was really possible to show that
00:29:38
in many of these dark heads the
00:29:43
star formation process does not start,
00:29:45
just that is, this picture it seems to be
00:29:48
correct, that is, indeed, in the
00:29:49
local group of galaxies there are many small
00:29:51
hungers. There is ordinary matter mixed with
00:29:53
dark matter, but ordinary matter does not go
00:29:56
into the stage when star formation begins,
00:30:01
if we do, it means that at the level of
00:30:03
individual galaxies it is important that Galaxies
00:30:05
interact with each other This is a
00:30:07
normal process of Galaxies growing,
00:30:08
merging with each other, this is a well-known
00:30:11
beautiful pair of galaxies, the photo is very
00:30:14
old, these are still plates from I think
00:30:16
black and white, sometime in the 60s and
00:30:19
seventies. And this modeling is
00:30:21
also, generally speaking, quite old,
00:30:22
designed specifically to show us this pair of galaxies.
00:30:27
Well, this is happening approximately the following as a
00:30:30
result of the interaction of galaxies,
00:30:32
naturally, some part of the matter
00:30:34
may be lost as a result of this,
00:30:39
but in general there is an enlargement
00:30:42
of the Galaxy, remember the transformation of planets
00:30:44
there is such a problem If you
00:30:46
collide two ten-meter stones,
00:30:48
they scatter into dust And if you
00:30:50
collide two ten-kilometer bodies
00:30:53
two such planets have already wintered, then they
00:30:56
want to lose some of the matter, but they
00:30:58
will collect a lot of their gravity And therefore,
00:31:00
growth will continue if
00:31:03
bodies with dimensions of 10,100
00:31:05
thousand kilometers collide with you The planet is growing Well,
00:31:07
Galaxies are also mostly growing And let us also
00:31:10
remember the collision of galaxies
00:31:12
can lead to the fact that
00:31:16
if you will simply have an area
00:31:20
filled with gas without dark matter and
00:31:24
this gas can form a small
00:31:25
Galaxy As a result, you will get a
00:31:28
Galaxy without dark matter
00:31:29
collision Galaxy one of the ways is
00:31:31
the separation of ordinary matter and dark matter
00:31:34
if we collide Galaxies as in the
00:31:36
previous one Let's go back here for a
00:31:38
second this Two normal, rather
00:31:40
large Galaxies and we can expect that
00:31:43
each had a supermassive Black Hole in the center
00:31:46
and, accordingly, if two Galaxies
00:31:48
merge, then the black holes being the most
00:31:51
massive objects in the galaxy, it doesn’t matter
00:31:54
that the Galaxy itself is a thousand times more
00:31:55
massive, the Black Hole is still
00:31:57
superior to everyone individually and they will
00:32:00
descend quite effectively to the minimum of the
00:32:03
total gravitational potential, that
00:32:05
is, to the center. So there is an
00:32:07
obvious prediction, if we see this, then we
00:32:10
should see double supermassive
00:32:12
black ones, and indeed we see such
00:32:14
objects, we see them very differently, the right
00:32:16
picture is more boring, this is the X-ray
00:32:18
data, the square we clearly we see two
00:32:22
central sources in this galaxy,
00:32:25
they are quite powerful
00:32:27
and Paddington luminosity,
00:32:30
we understand that we need
00:32:33
supermassive black holes to
00:32:34
explain each of these sources, that
00:32:36
is, the Galaxy obviously, like many
00:32:38
galaxies,
00:32:41
experienced a major merger with ours, as
00:32:44
you remember, by the way, it’s interesting the film
00:32:47
Heart of a Dog is a lot of I watched your
00:32:48
two-part series well, yes, because the
00:32:52
main event in my life is the main
00:32:54
event of your life in the future,
00:32:56
remember the fortune tellers, here we have
00:32:59
the main merger in the future, the merger with the
00:33:01
Andromeda nebula, but some have
00:33:03
already had it, it’s very beautiful, there are two
00:33:06
pairs of jets, that is, here is one center
00:33:08
from where 2G it comes out Here is another center
00:33:10
from where 2 Jets come out this is
00:33:12
lozar 375 respectively here
00:33:16
obviously we have two black holes if
00:33:19
we see them so well Individually there is a
00:33:22
very large distance between them and
00:33:25
These black holes will not merge in the next 10
00:33:29
billion years but in
00:33:32
some cases it turns out differently
00:33:34
and accordingly we can expect the
00:33:37
merger of supermassive black holes, this is an
00:33:39
important prediction because in the future it
00:33:41
will be possible to observe the merger of black
00:33:45
holes, the most important thing is that a powerful
00:33:47
gravitational wave signal is emitted,
00:33:49
the signal is emitted if you have
00:33:51
two point bodies rotating suddenly around each other,
00:33:54
the signal is released but doubled
00:33:56
orbital purity That is, if the orbital period is
00:34:01
a year, then the period of the wave will be six months
00:34:07
Estimate the orbital period quite
00:34:09
simply, we can
00:34:11
make a very simple assessment like this, very
00:34:14
childish We have
00:34:24
Kepler’s law, yes you can see Turn on the light, it’s
00:34:28
visible more or less but everything is simple here, you
00:34:30
should know Kepler's law without me,
00:34:32
respectively, at the final stages of
00:34:35
the merger. You can say that the semi-major
00:34:37
axis of the orbit is approximately several
00:34:42
Schwarzened radii of the black hole, the
00:34:44
Schlakshierd Radius is 2G per C
00:34:47
square, well, and accordingly, all this
00:34:50
can be put there and we will get the
00:34:52
characteristic times that is, characteristic
00:34:56
Let's still write
00:35:00
pravitational waves at a later stage the root will be
00:35:05
4 pi square Well, let me have a Black
00:35:09
hole Well, okay, I'll leave the same ones,
00:35:11
you can just put two of them,
00:35:14
and instead I'll substitute this thing, that
00:35:18
is, two m by C square in cube up to,
00:35:24
well, you can try. If you put a
00:35:27
mass like 10 million masses of the sun in there,
00:35:30
then you will get some times there of the
00:35:32
order of one month one month This is
00:35:35
what we have 10 5
00:35:38
10 6 3 by 10 6 seconds in this spirit should
00:35:42
get
00:35:43
This quite long times,
00:35:45
respectively, to get the
00:35:47
wavelength, you multiply the speed of light by this
00:35:49
time, you get a larger wavelength.
00:35:51
By the way, I forgot,
00:35:54
we have a doubled Orbital, which means the
00:35:57
frequency is higher, the period is smaller, that is, so
00:36:01
we need to add two,
00:36:03
it’s clear. Yes, why is the two because of the doubled
00:36:06
we move from orbital period to the
00:36:09
period of the wave,
00:36:12
to register such waves, large
00:36:15
detectors are needed and these are space detectors,
00:36:18
respectively, the
00:36:20
distance between the satellites is
00:36:24
several million kilometers.
00:36:26
This is what it turns out to be
00:36:29
somewhat 10-11 cm,
00:36:34
respectively, you can
00:36:36
estimate for which black holes it is
00:36:40
suitable, respectively, the
00:36:42
Schwartzuld radius is three kilometers
00:36:44
for the masses of the sun are 3 million
00:36:46
kilometers. Well, three million kilometers
00:36:48
means about a million masses of the sun. Well, the
00:36:53
cosmic interferometer is most
00:36:55
sensitive to mergers of blacks with masses of
00:36:59
about a million masses of the sun.
00:37:01
Well, they will see something like 10
00:37:03
million there, that is, not some kind of hard
00:37:05
limit, millions characteristic value of the sun,
00:37:09
but you can look for longer waves
00:37:13
because there are black holes with masses of a
00:37:16
billion from the sun and the main thing is not
00:37:19
only their bursts, but while you have these
00:37:22
black holes getting closer they still
00:37:25
emit, that is, the Universe is filled with
00:37:28
pairs of black holes that emit
00:37:30
gravitational waves to different frequencies
00:37:34
and, accordingly, you can look for this
00:37:36
signal and
00:37:39
the best approach to this was invented by Mikhail
00:37:42
Vasilyevich Sazhin in traffic police in
00:37:45
1978, the idea is this:
00:37:50
if a gravitational wave passes through here,
00:37:53
then here
00:37:55
space time changes periodically,
00:37:57
respectively, we look out through
00:38:00
this distorted space time and
00:38:02
external events will seem
00:38:04
distorted to us, we need some very
00:38:07
accurate stable external events.
00:38:09
Observing which we understand that a
00:38:11
gravitational wave is passing through us. In order not to be
00:38:13
confused, we need to observe many
00:38:15
such events throughout the sky so that it does not
00:38:19
turn out that there is a problem with a
00:38:21
specific source.
00:38:24
a person comes to the doctor, I have such a
00:38:26
problem, it’s just a nightmare, look, it
00:38:29
hurts like that, it hurts like that, it hurts like that, it
00:38:31
hurts, it hurts, it’s understandable That
00:38:37
is, if you see everywhere Well, it’s like
00:38:41
about the same effect, in reality,
00:38:43
you see correlations This means that
00:38:46
something is happening to you, especially if
00:38:49
the objects are not connected for a reason and the idea
00:38:51
is that you can
00:38:52
observe a certain number in real life,
00:38:56
these are dozens of
00:38:57
radio pulsars all over the sky,
00:38:59
radio pulsars with a very precise time of
00:39:02
arrival of the pulse. That is, as a rule,
00:39:03
it is necessary for such high stability
00:39:05
requires a high rotation frequency and these are
00:39:09
always millisecond pulsars. That is,
00:39:12
now there are several projects working, three
00:39:14
are working and two are still starting to work
00:39:17
European American Well, conditionally,
00:39:19
this Australian one
00:39:21
is starting to work Indian Chinese
00:39:24
projects, in each project there are
00:39:25
several dozen pulsars somehow
00:39:28
scattered around the sky
00:39:30
and, accordingly,
00:39:34
correlated failures are observed are not observed,
00:39:36
correlations are sought in the failures of the
00:39:40
arrival of pulses from these pulsars if a
00:39:43
gravitational wave passes, that is,
00:39:45
predictions of what the distribution will look like,
00:39:46
what the correlation will
00:39:49
look like, that is, people know what they are looking for,
00:39:52
here it is schematically shown that if we have
00:39:55
space-time curved here then
00:39:57
these are signals from different sources and
00:40:00
they will all be somehow distorted and there will be
00:40:04
some kind of correlation, this is a picture from work
00:40:07
seven years ago
00:40:09
and seven years ago. These three projects
00:40:12
have begun to approach the sensitivity
00:40:15
which already falls into an interesting
00:40:17
strategic range, which means I repeat.
00:40:19
They are not looking for separate bursts They are looking
00:40:22
rather for gravitational wave noise
00:40:24
that is emitted by a large set of
00:40:27
double black holes in the Universe of double
00:40:29
supermassive black holes in the Universe Well,
00:40:32
since then all the groups have continued
00:40:34
to work, but so far Unfortunately they have
00:40:37
n’t seen anything special two years ago the
00:40:40
American nanograph group announced
00:40:42
that they see some kind of Signal,
00:40:45
this is, respectively, data from different
00:40:47
pulsars based on the deviations of their pulses And
00:40:51
this is the distance between the pulses in the sky Well,
00:40:54
they see some kind of correlation,
00:40:56
amazingly, it is completely
00:40:57
different from what is predicted for
00:40:59
gravitational noise,
00:41:00
the signal is not to say that it is very it is strong,
00:41:03
but it is a significant signal; it is
00:41:05
unknown how it is explained. Therefore,
00:41:08
accordingly, people are waiting for other
00:41:10
groups to reach the same level of
00:41:12
sensitivity and this is apparently just
00:41:15
a matter of several years, that is, apparently
00:41:18
in the coming years there will be
00:41:21
some clarity on this signal, this
00:41:23
will be quite interesting ok So
00:41:27
I have a little time left, I wanted to
00:41:31
write a couple of simple examples for you on the board
00:41:34
just so that you have some useful estimates
00:41:36
in your heads,
00:41:42
so
00:41:44
let’s start with what it means, well, first of all, let
00:41:48
’s estimate the mass of the Galaxy, it’s all very
00:41:51
simple here we have a Galaxy
00:41:53
disk And all this is immersed in a large halo; the
00:41:57
characteristic size of the Gala is 100
00:41:59
kiloparsecs and we know that the
00:42:03
radial velocity curve somehow
00:42:06
stretches to large distances up
00:42:08
to these same
00:42:12
kiloparsecs and the speed is about 220 by 220; it’s
00:42:16
just a number easier to remember than 200
00:42:22
and, accordingly, that we get
00:42:24
mass in this volume, I will assume that the
00:42:27
enchantingly symmetrical distribution of
00:42:30
mass in this volume will be squared by R
00:42:33
divided by 2G is correct
00:42:37
if it is incorrect to say
00:42:41
2gm by R
00:42:45
so well that I end
00:42:49
up with
00:42:50
two and two squared by 10 is 10/7
00:42:56
squared 1014 correct for a radius of 100
00:43:00
kilo parsecs 100 kilos is 10 in 5
00:43:05
parsecs this is 31 by 1018 centimeters here
00:43:10
I have a deuce left here what is there 667
00:43:13
by 10 minus 8
00:43:16
equals equals equals
00:43:19
one deuce I will reduce it
00:43:23
will remain a deuce 2 by 3 6 has been reduced, that
00:43:28
is, these coefficients seem to be going away.
00:43:30
I hope I haven’t lost the two anywhere, so all that
00:43:33
remains is to collect the orders
00:43:37
somewhere, there should be
00:43:44
must be.
00:43:46
So we are collecting the order 10-19 10 18 37 and
00:43:53
another 845 1045 grams,
00:43:57
this is respectively 1/ 2 by 10-12 masses of
00:44:01
the sun Well, 1/2 you understand, this is such a
00:44:04
value of the order of units,
00:44:07
so you and I don’t really
00:44:11
remember anything except the rotation curve,
00:44:13
we got that the mass of the galaxy is 10-12
00:44:18
masses of the sun, what else can we say?
00:44:21
So here
00:44:24
we have, as it were
00:44:27
we have a hot gas
00:44:30
and point B We will have
00:44:33
about this gas gas in Gal
00:44:38
let's ask a simple question What is the
00:44:40
temperature of this gas
00:44:42
with the temperature of this Gas Everything is clear
00:44:47
because we have a system implemented
00:44:52
and accordingly the
00:44:55
gravitational energy is double
00:44:58
the kinetic in this case thermal and
00:45:01
therefore we can write that the three second
00:45:04
CT we believe that this is hydrogen, all the
00:45:06
particles are the same Well, it doesn’t matter to us at all
00:45:08
What kind of
00:45:16
GM it will be for mass, particles for size Well, if
00:45:21
you want, add 1/2 to taste, this, in
00:45:23
principle, is not very important and from here
00:45:26
you can express the temperature here if you
00:45:28
do the math, I got 2 by 10 6
00:45:32
cells of the
00:45:34
Patsays, a mass of 10-12, which is what it is, that
00:45:40
is, our galaxy is filled with
00:45:43
such coronal gas, remember we
00:45:45
said that the stellar medium has different
00:45:47
phases, different states, and in particular, there is a
00:45:50
state of coronal gas, and finally the
00:45:53
last example is
00:45:55
we we know that there is the Andromeda Nebula,
00:45:59
we know that there is our Milky Way Galaxy
00:46:02
and they are falling on each other, the
00:46:05
distance between them is 770 kiloparsecs,
00:46:08
which I substituted, it was interesting
00:46:10
to imagine 750 kiloparsecs, it’s probably
00:46:13
easier to calculate this way, let’s write 750 parsecs
00:46:16
between them and they are falling on each other,
00:46:20
falling on each other friend under the influence of their
00:46:23
own gravity, their mass is
00:46:25
approximately the same
00:46:31
10-12 mass We will assume that they are
00:46:34
the same and ask And when will they
00:46:35
fall How long to wait, maybe you have
00:46:39
some plans, then it all counts, it’s all
00:46:43
fantastically simple,
00:46:44
firstly, we again remember
00:46:50
Kepler’s law
00:46:55
and then we remember a very simple thing,
00:46:58
look,
00:47:00
here I have an ellipse. Yes,
00:47:03
accordingly, this
00:47:08
is the major axis, that is, two, and this is the
00:47:11
semi-major axis
00:47:14
and the ellipse is characterized by some kind of
00:47:17
eccentricity. But let me be.
00:47:20
Let me somewhere have a focus ellipse
00:47:24
if I increase the eccentricity of the ellipse
00:47:27
becomes even more elongated for me
00:47:30
and the focus shifts even closer here.
00:47:34
That is, I do not change
00:47:36
the semi-axis of the orbit, I only change
00:47:39
the eccentricity,
00:47:41
it stretches me out and in the
00:47:44
limit Naturally it stretches out into a
00:47:46
thread like this
00:47:48
Well, that is, this is a completely elongated one
00:47:50
and back
00:47:53
like this I have one body here, another body
00:47:56
here, the second one is actually in focus
00:47:58
at the moment
00:48:00
and it turns out very simply that the
00:48:03
time of fall
00:48:05
is equal to 1/2 of the
00:48:08
orbital period
00:48:11
because they fall on each other under the
00:48:14
influence of their own gravity, but
00:48:15
consider that this body is falling on this the
00:48:17
time of fall is one-half of the
00:48:18
orbital period And now we
00:48:20
can simply, according to Hitler’s law, calculate the
00:48:21
time of fall of
00:48:24
m31 on us, respectively, it will be
00:48:29
1/2 of the root 4 square and the cube is M1 plus
00:48:37
m2 Let’s substitute then we’ll do it
00:48:41
Well, what’s two pi, I’ll get two
00:48:46
that means there will be a root of
00:48:50
750 cubed
00:48:53
3.1 cubed
00:48:57
10 to 9 because there is a kilo parsec and
00:49:02
1018 cubed 254 here
00:49:06
respectively 6 and 7 let by 10 minus
00:49:09
8 two
00:49:12
10-12 sun 10 12 2 at 10:33
00:49:18
well let’s see what we have left and
00:49:29
7 and 5 in a cube
00:49:32
3 in a cube
00:49:34
divide by 4 by 6 and 7 we collect the orders one
00:49:40
two in a cube 6
00:49:43
plus 9 is 15 plus 54 This is 69
00:49:50
69 plus 8 more 77
00:49:55
77 And this is 45 Correct 77 -45
00:50:01
this is 32 correct
00:50:04
1032
00:50:07
Very good Very good that means it will be
00:50:12
three pi I'll take the three out of here now
00:50:16
I'll set it aside
00:50:17
by seven and a half by 10-16
00:50:22
And everything else is actually all
00:50:25
approximate disappears Yes because it will become
00:50:28
7.5 sixes will be approximately reduced from the
00:50:30
construction site four It will be approximately
00:50:32
reduced here Good
00:50:35
well, that
00:50:37
means I get about two
00:50:43
and one but two with a tail of some kind
00:50:48
for 10-17 and pi and you remember that in the year
00:50:53
pi for 10 seventh seconds is a second one
00:50:56
year is approximately equal to pi for 10 seventh
00:51:00
seconds So I did it approximately
00:51:05
20 billion years, about
00:51:08
three I lost it, so it
00:51:10
turns out when I calculated on a piece of paper
00:51:14
I got 7 billion years there, but
00:51:16
we got the characteristic time correctly,
00:51:17
I don’t know where I lost the three,
00:51:19
respectively, the time of fall. This is
00:51:23
several billion years, it is our
00:51:25
Galaxy on this optimistic note.
00:51:28
five-minute break
00:51:33
and I remind you But I hope that everyone
00:51:35
present knows that the lecture
00:51:38
is posted on my Xray page by
00:51:41
themselves suru slash Tilda polar further
00:51:44
section of the lecture Well, our course is at the top and the
00:51:47
slides of all lectures are there too Well, as
00:51:50
everything is uploaded video In
00:51:53
each lecture I attach a direct link to
00:51:55
YouTube and in my YouTube channel They are
00:51:58
collected in a single playlist Well,
00:52:00
accordingly, you can go through this way,
00:52:03
you can go through this way, you can go directly through the channel
00:52:06
As convenient for you,
00:52:08
okay, and we move on to the chat to our
00:52:12
final topic on cosmology of which
00:52:16
we will talk for the rest of the time
00:52:18
today and two pairs next time
00:52:20
we will start with the fact that I may even
00:52:23
repeat some things, I want to emphasize
00:52:26
that
00:52:27
there is, again, a huge complex of
00:52:30
observational data that shows
00:52:32
us the evolving universe, this is very
00:52:34
important because only 100 years
00:52:37
ago the
00:52:38
idea of ​​an evolving universe was
00:52:41
just fantastically psychologically
00:52:43
uncomfortable for many people and Einstein
00:52:46
came up with the lambda term as a
00:52:49
technological constant, as if dark
00:52:52
energy, in order to solve this
00:52:55
problem in order to make
00:52:57
the universe eternal and unchanging as a whole, but
00:53:00
we know that in general it is
00:53:01
evolving, we have a lot of
00:53:04
observational data, in particular, there are deep
00:53:06
deep fields of Hubble, soon
00:53:09
there will be deep fields of James Webb,
00:53:14
respectively, here we can get
00:53:17
to the very early history of galaxies, but with
00:53:20
James Webb we will get to the
00:53:22
formation of the very first
00:53:24
galaxies and we can look at this
00:53:28
whole picture in more detail in more detail finally
00:53:30
we can zoom in again we saw
00:53:32
such a picture
00:53:33
these are indeed generally distant
00:53:37
Galaxies and we see that their shape is far
00:53:40
from what we see our surroundings
00:53:43
and accordingly we can Well of course not
00:53:47
for one Galaxy but we can
00:53:48
build such a gallery as
00:53:51
Galaxies change characteristically from time to time there from the
00:53:55
first billion years of the life of the Universe to
00:53:57
the present day, we can by the way compare this with the
00:54:00
results of the calculation of the complex and the chandelier
00:54:03
with or something similar Needles there are new
00:54:06
reincarnations of the chandelier
00:54:08
and we will see that is, we are we are seeing
00:54:12
voucha We see that the world galaxies are changing,
00:54:14
we see the era when it begins
00:54:17
to form and part of the history of the Universe
00:54:21
is given to us, for example, through this data,
00:54:23
through the history of the formation of galaxies, we
00:54:27
see How structures are formed This is
00:54:29
an image of a cluster of galaxies, you see the
00:54:31
effect of lensing on the cluster, that is,
00:54:35
we see distant Galaxies through
00:54:37
the cluster and therefore they
00:54:40
appearance and I will say some very weakly But
00:54:43
it is clear that in general they form into
00:54:46
such a structure of
00:54:48
concentric pieces of some kind
00:54:52
and this, in addition to allowing us to
00:54:55
determine the mass of clusters, which is important,
00:54:57
allows us to study many other things and
00:55:00
Observing a large number of
00:55:02
galaxy clusters We nevertheless see an era
00:55:05
when a cluster of galaxies is simply
00:55:07
not yet formed, we see the evolution of the
00:55:10
large-scale structure of the Universe and
00:55:12
this picture, too, in my opinion, we saw the right
00:55:16
picture, this is a thoughtful inner
00:55:18
square and here there are Six galaxies
00:55:20
at Redshift 5.3,
00:55:23
which corresponds to approximately the first
00:55:25
billion years of the life of the Universe, these
00:55:28
Galaxies
00:55:29
are located close to each other in
00:55:32
three-dimensional space, we can
00:55:34
calculate that in the future they will form a
00:55:36
cluster, but at that moment the cluster is
00:55:38
not there
00:55:39
yet. Gravity needs to work to
00:55:42
form a cluster,
00:55:45
we saw this video. I don’t know whether it will work
00:55:47
here or not. It won’t
00:55:51
work for me. But it will work. Hurray for this
00:55:54
accordingly, computer
00:55:56
modeling of the formation of elements of the
00:55:58
scale structure and it all begins,
00:56:00
we saw z28 approximately, that is,
00:56:03
the Universe was 30 times smaller
00:56:04
compared to its
00:56:06
modern size, but
00:56:10
the size of the Cube is artificially maintained up to Otherwise, we did
00:56:13
not see anything, we can
00:56:16
study the formation of galaxies of clusters of
00:56:20
galaxies on different scales
00:56:22
to compare this with observations and
00:56:25
some time ago,
00:56:30
the word laniacs appeared in the vocabulary of educated people.
00:56:36
This is our supercluster of galaxies. Our
00:56:39
galaxy is part of the local group.
00:56:53
100 thousand large galaxies are
00:56:55
approximately half a billion light
00:56:58
years in diameter and today
00:57:01
superclusters are the largest
00:57:02
structures that exist in the Universe,
00:57:05
no more structures will arise, and
00:57:07
moreover, if dark energy does not
00:57:09
decay into anything, the surroundings of superclusters of
00:57:12
galaxies will begin to fly apart over time,
00:57:16
accordingly, this is an understanding of that how
00:57:19
Laniakia behaves It arises from a
00:57:21
complex of observational data on a
00:57:24
large number of galaxies We, of course, do not
00:57:26
see how they move,
00:57:28
we can measure
00:57:30
velocities along the line of sight, only
00:57:34
transverse movement; we do not
00:57:36
observe any
00:57:37
accuracy for this is not enough. But
00:57:41
nevertheless, having analyzed a large complex of
00:57:43
data on these velocities we can
00:57:44
reproduce how everything happens, it’s
00:57:46
quite funny,
00:57:49
there’s this, our cluster, and here’s the
00:57:52
neighboring cluster that’s forming, that
00:57:54
is, along all these trajectories there’s an
00:57:56
animation of it, you can find it at this
00:57:59
address, this is the work, respectively,
00:58:01
September 14,
00:58:05
our supercluster is being formed.
00:58:08
Galaxies move along these trajectories
00:58:11
everything flows here and here a
00:58:14
large massive object is formed. But here everything
00:58:16
flows in the other direction,
00:58:18
respectively, somewhere there is
00:58:19
a watershed, it looks like a system of two
00:58:22
giant rivers on the continent, here it is
00:58:25
somewhere here, the watershed passes
00:58:27
from here, it will flow here, and from here it will flow
00:58:30
here and in Laplata,
00:58:32
accordingly, there are also areas where
00:58:36
Galaxies seem to be close, but they will
00:58:38
move in different directions and we can
00:58:41
say that they already belong to different
00:58:43
superclusters, but most likely in the
00:58:45
future, due to the accelerated expansion of the
00:58:46
Universe, they will still be separated from these clusters.
00:58:49
Please note although in
00:58:51
principle it’s like a
00:58:54
quasi-three-dimensional picture, yes,
00:58:57
and it exists, and in three degrees it can even be
00:59:00
rotated, but the axes are not written in
00:59:04
parsecs of light years. But in general, at
00:59:06
speeds of kilometers per second,
00:59:08
this is due to the fact that we still receive data
00:59:10
through measurement speeds at
00:59:14
large distances for a large
00:59:16
number of galaxies that are
00:59:17
used here, individual determination
00:59:19
of distances does not work
00:59:22
through some objects there, I don’t know
00:59:25
the correlation of parameters, something else,
00:59:27
you determine everything through speed and
00:59:30
then recalculate within a
00:59:31
certain model, but everything works
00:59:33
quite well And in in particular, we
00:59:36
are beginning to understand quite well how
00:59:38
our supercluster of galaxies lives, how it grows, how it develops, we
00:59:41
can go to an
00:59:43
even larger scale. Let’s pay
00:59:45
attention. Here it is 12 thousand kilometers per
00:59:49
second, here it is already 20 thousand. That is, this is a slightly
00:59:52
larger scale, this whole
00:59:55
beautiful fibrous structure of the Universe is
00:59:57
Well there are people who believe that it is
00:59:59
fractal, in fact it’s nothing so
01:00:01
simple,
01:00:02
its properties differ from the classical
01:00:05
fractal. But
01:00:08
something formed on a small scale
01:00:11
can be part of something even larger,
01:00:13
that is, there are large
01:00:16
density fluctuations, for example, there is such a large
01:00:18
density fluctuation from a tractor Shepley
01:00:21
Shepele remember we met in the Great
01:00:23
Disk Curtis Shepele This is the same one
01:00:28
and because somewhere Yes here the Great
01:00:31
Attractor was once considered such an
01:00:33
amazing mystery but there is a
01:00:35
Shepley attractor he is even more a
01:00:38
local group somewhere here we
01:00:40
are
01:00:41
accordingly here here our
01:00:43
supercluster is growing, here is Perseus Pisces
01:00:46
supercluster, here it is Persia Pisces, here is
01:00:49
ours
01:00:52
somewhere here And all this is involved in an even
01:00:56
larger movement, but naturally
01:00:58
if somewhere it is added somewhere it
01:01:00
is decreased, that is, the area
01:01:02
from which the substance flows out. There was not
01:01:05
enough mass here, well and accordingly,
01:01:07
its people love beautiful names. If this is a
01:01:10
great attractor, then it is
01:01:13
called a dipole repeller, but naturally there is
01:01:14
no repulsive force,
01:01:17
that is, if a brick falls on your head,
01:01:19
not because the sky pushed it away;
01:01:21
the sky did not accept it, but then they accidentally came out. That’s
01:01:25
not how it works, but We can
01:01:29
study the dynamics on this scale
01:01:31
precisely through observation,
01:01:34
not quite directly of course, but still
01:01:37
through observation and this is important. Once
01:01:41
again, here is the skeleton of the Universe
01:01:44
assembled from dark matter and it is clear
01:01:48
that the matter flows along the fibers to areas
01:01:50
where these brighter areas are brighter also
01:01:55
gravitationally interact with each
01:01:57
other, so there may be some kind
01:01:58
of complex large-scale movement
01:02:01
and, accordingly, from the dark areas
01:02:04
the matter, if there is something left there, it
01:02:06
can flow away, that is, the size of the warriors
01:02:09
will grow over time, these Bubbles voids
01:02:13
naturally increase in the expansion of the Universe size we
01:02:16
were talking about these dark
01:02:17
matter fibers just now so I scrolled through
01:02:19
pretty quickly this is another picture
01:02:22
that we didn’t have yet
01:02:24
[music] a
01:02:26
fiber was discovered near a quasar
01:02:30
quite distant Z2 and 3 This is several
01:02:33
billion light years away from us several
01:02:37
light years under 10 almost it turns out that a
01:02:40
lot was discovered, a gas filament with a
01:02:43
length of more than a million light
01:02:45
years was discovered, that is, a Quasar cannot
01:02:47
throw one out, it is too large,
01:02:49
it is too large, obviously, but still
01:02:52
it is an element of a large-scale
01:02:54
structure for once registered by
01:02:55
ordinary matter, the observations were carried out
01:02:57
in the hydrogen line,
01:03:03
remember that we
01:03:06
we observe the
01:03:08
dynamics in the chemical composition of the Universe,
01:03:10
we can study the chemical evolution
01:03:12
of our galaxy, identify stars there of
01:03:15
different ages of different populations,
01:03:18
study how the chemical composition has changed, and we can
01:03:21
study the chemical composition of the gas between the
01:03:25
Arctic clouds at high
01:03:27
redshifts and we see that there is gas there of a
01:03:32
very low-metal personality. That is, this is a
01:03:34
completely separate Aspect of evolution, we
01:03:36
looked at the Aspect of evolution
01:03:37
associated with the formation of galaxies with
01:03:40
the formation of different structures there, from
01:03:42
clusters to spheres of clusters, there is
01:03:43
chemical evolution. The Galaxy from this
01:03:45
point of view, the Universe also appears as
01:03:48
evolving people are constantly looking for
01:03:51
more and more metallic
01:03:53
Clouds there large redshifts
01:03:55
to finally discover clouds of
01:03:58
primary composition where there was no
01:04:01
injection of heavy elements at all due to the
01:04:04
vital activity of stars, in this case
01:04:07
Z7 is already less than one billion
01:04:11
years after the big bang and a
01:04:14
cloud of very
01:04:15
low metallicity was discovered,
01:04:18
as a result we see that the entire universe
01:04:21
is evolving and this very diverse
01:04:23
independent data
01:04:25
another piece of data is very interesting
01:04:28
related to the cosmic microwave background radiation I once
01:04:31
mentioned that the discovery of the cosmic microwave background radiation
01:04:33
This is a rather dramatic
01:04:35
story because it was discovered
01:04:37
several times and was not recognized
01:04:40
was not recognized because it looks like noise
01:04:43
Well, often Well there are Noises are it doesn’t
01:04:46
interfere much, let’s write down that there is such noise,
01:04:51
we won’t analyze the reasons for its occurrence, but there was another interesting
01:04:55
result, people discovered the radiation of the
01:04:58
molecule, quite strangely, in my opinion, a very
01:05:04
strange level of
01:05:06
vibrations was excited from the cyanide molecules by unknown means. And only
01:05:10
after the fact it became clear that it was excited by the
01:05:12
relic radiation, that is,
01:05:15
molecules are also like detectors of
01:05:17
external radiation, and the
01:05:21
presence of cosmic microwave background radiation was noticed through
01:05:23
the radiation of molecules, but the Universe
01:05:25
is expanding and the temperature of the relic
01:05:27
radiation is falling, that is, once at the
01:05:30
moment of recombination it was more than three
01:05:32
thousand degrees since then the Universe
01:05:33
has expanded approximately
01:05:35
the temperature has dropped 1100 times and now the temperature of the
01:05:38
relict is 2.7 tails.
01:05:41
Accordingly, it turns out that at different
01:05:44
epochs the relict radiation should
01:05:46
excite different levels of different molecules, it
01:05:48
seemed that this is an observable thing and we
01:05:52
can observe in this way
01:05:54
that the temperature of the relict
01:05:56
radiation in the past of the Universe was higher,
01:05:59
there is even more understandable specifically on it I
01:06:03
want to say a method for measuring the
01:06:04
temperature of the cosmic microwave background radiation in
01:06:07
different eras of the life of the Universe,
01:06:08
but it is important that there are at least
01:06:11
two methods and they are absolutely independent of each
01:06:13
other; according to the methodology, they do not
01:06:14
overlap in any way; they use different
01:06:16
observational data in different ranges of
01:06:18
different objects; this is an effect Sineva
01:06:21
Zeldovich second in excitation of lines, I
01:06:23
said to you and I. We
01:06:24
have profited a little, which means we have
01:06:28
Galaxies, there is a cluster of galaxies. This is a
01:06:30
cluster of these
01:06:31
worms, this is a separate Galaxy, these are
01:06:33
clusters, as you remember, a cluster of
01:06:35
galaxies is filled with hot gas, the gas is
01:06:38
implemented for a separate Galaxy, we
01:06:41
counted there 10- 12 solar masses and 100
01:06:44
kilo parsecs gives 2 million Kelvin. And
01:06:46
if we took the parameter of
01:06:48
galaxy clusters, we would get more than two 20 million,
01:06:50
respectively, there is hot gas,
01:06:53
this is realized hydrogen plasma in the
01:06:56
first place. This means there are many
01:06:57
electrons with high energy and all these
01:07:00
electrons are immersed in the radiation field
01:07:03
associated with the relict radiation, that is, continuously
01:07:06
photons of the cosmic microwave background radiation enter the
01:07:08
Galaxy cluster. These
01:07:10
photons are everywhere and interact with the electrons of
01:07:13
this cluster, respectively, you
01:07:15
have a Comptoon effect, you have a
01:07:18
cold Phantom in this case, it takes
01:07:20
energy from the hot electron, this
01:07:23
leads to the fact that the spectrum of the cosmic
01:07:25
microwave background radiation changes direction towards
01:07:28
the cluster Well, the
01:07:31
X-ray spectrum of the cluster itself changes for
01:07:34
the relic,
01:07:36
its blackbody distribution changes, the radiation
01:07:39
in the direction of the cluster seems to
01:07:40
become hotter And this is a well-
01:07:44
understood effect there in the article by Syun his
01:07:47
Zeldovich, this is 80. If I’m not mistaken,
01:07:50
accordingly we receive
01:07:53
a radio signal, we receive
01:07:58
scattered radiation on hot electron
01:08:00
clusters the cluster we see is important that
01:08:03
we know Which cluster we are studying we
01:08:05
can study it and we can directly
01:08:07
determine its mass there sometimes by
01:08:09
weak lensing and then we can
01:08:12
estimate a fairly good temperature of the
01:08:14
gas considering that it is realized in the end we
01:08:17
can learn everything about cluster by
01:08:19
X-ray observations, for example,
01:08:21
using radio observations Determine
01:08:24
the temperature of the relic exactly there, that is,
01:08:26
we see a cluster of galaxies at
01:08:28
Redshift 1
01:08:30
This is how many 5 billion years ago 6
01:08:33
approximately and we measure the temperature of the
01:08:36
relic and a lot of clusters, we can
01:08:38
do this operation for a large number of
01:08:40
clusters Well, graph from work almost
01:08:43
ten years ago, the
01:08:46
temperature of the relict
01:08:48
radiation is plotted vertically horizontally, the red
01:08:49
shift is logarithmic to
01:08:51
better expand everything z0, let me remind you that we have the
01:08:55
current temperature of the relict,
01:08:58
approximately 2.7. But this measurement and
01:09:02
the curveball that describes everything perfectly
01:09:03
and the curveball comes to us from
01:09:07
standard cosmological model We
01:09:10
have complete independence physically. A
01:09:12
clear, understandable way to measure the
01:09:15
temperature of the cosmic microwave background radiation at
01:09:17
fairly large redshifts, you see,
01:09:19
but for one it goes even for two, and
01:09:23
this was 10 years ago, that is, that is
01:09:26
why we have a huge complex of
01:09:28
observational data associated with
01:09:31
evolution of the universe and all this needs to be
01:09:33
crammed into one cosmological picture,
01:09:35
that is, it is very important to understand that when
01:09:38
we come across a cosmological picture,
01:09:40
we will naturally have a very simple
01:09:42
sketch, look at this picture, there are
01:09:45
some basics, but it is important to understand that behind
01:09:47
this, on the one hand, there is a large
01:09:49
complex of theories some But on the other
01:09:52
hand, there is a large complex of real
01:09:54
observations that can test the most
01:09:57
diverse aspects of these models and there are
01:10:02
no catastrophic inconsistencies at the moment. People already want some
01:10:05
inconsistencies and there they are seizing on the problem of
01:10:09
measuring the Hubble constant, different
01:10:10
methods will be time, maybe in
01:10:13
a week, you can say a few words about this well,
01:10:16
but the most important thing is where our
01:10:19
understanding of the fact that the Universe is
01:10:20
evolving began, this is the expansion of the universe,
01:10:23
so I would say that this is the most
01:10:25
beautiful scientific picture of all times and
01:10:27
peoples,
01:10:28
I don’t know, maybe someday
01:10:30
something will be obtained - something more beautiful but this is
01:10:33
the most beautiful this is the expansion of the Universe
01:10:35
this is one of the original ones with all the
01:10:38
typos the speed is just kilometers
01:10:40
even a second forgot to register
01:10:44
Hubble again as sophiids was not the first
01:10:49
who learned to determine the distance to the
01:10:53
Galaxy the speed of movement but he did
01:10:56
it very systematically and somehow
01:10:59
correctly understood, it’s important to pose the
01:11:01
right question, it’s important to solve the
01:11:03
right problem. I may have told you
01:11:06
if I didn’t tell you, but if I said it anyway. There
01:11:10
is such a wonderful theorist
01:11:13
Mikhail Sewer, he was once
01:11:15
asked on Facebook what he considers the most
01:11:17
important for a scientist. Well, they expected him to be
01:11:21
famous accordingly there are a
01:11:23
lot of such technical skills,
01:11:25
let’s say, and there is a wide knowledge of the Field, and
01:11:29
after thinking, he gave an absolutely
01:11:30
wonderful answer that I like,
01:11:31
he said that for really strong
01:11:33
scientists it is important to know what is important with some kind of
01:11:36
technology you always have something you
01:11:38
always know but or will you
01:11:40
apply it to important tasks or will you
01:11:42
do some kind of nonsense, you can
01:11:43
have some absolutely amazing technology
01:11:45
and do some kind of nonsense.
01:11:47
Well, for example, there, I think that there are some
01:11:50
people there who are calibrators with
01:11:52
soccer balls, so amazing
01:11:55
circus level but these are not
01:11:58
national team players If you watched Brazil
01:12:01
Argentina yesterday, in the sense of these two matches, it’s clear
01:12:04
what we’re talking about, these are completely different problems
01:12:07
being solved
01:12:08
So Hubble had this, which means that
01:12:12
we see In this picture the speed of
01:12:13
galaxies along the vertical axis Hubble
01:12:15
simply determined them through the Doppler effect,
01:12:18
we will talk to you separately physically.
01:12:19
This is wrong. Hubble did not know about this, but
01:12:21
surprisingly, numerically the answer
01:12:23
will be correct.
01:12:25
That is, this is really the speed of
01:12:27
galaxies where for distant ones it is the
01:12:30
cosmological contribution that dominates the day before.
01:12:32
Let's go back And horizontally, we
01:12:34
had to learn how to determine the
01:12:35
distance to galaxies, and in the days of
01:12:39
Hubble, at two megaparsecs, the sophiites
01:12:43
were not visible now at two megaparsecs.
01:12:46
No problem, with the help of the Hubble
01:12:47
telescope, everything is accurately measured by the pacifidae. The
01:12:50
sophiids could only be used
01:12:53
for the closest ones. The Galaxy is here if we
01:12:55
leave this, for example, then no
01:12:57
beautiful straight line will work
01:13:02
through this pile. points, draw a straight
01:13:04
line and say that this is true. This requires
01:13:07
a lot of civil property. If you
01:13:09
remember yourself in the First and second year.
01:13:12
Good. So, How does it work?
01:13:15
On the one hand, it seems that all the
01:13:17
Galaxies are moving away from us, and the
01:13:20
farther it is, the faster they are moving away. Therefore,
01:13:23
there is a feeling that you are not you give a
01:13:25
finger that something is wrong with us, that’s why
01:13:27
they all run away, maybe we are the center of
01:13:29
the Universe, the answer is no. If you observe
01:13:32
such a picture and now fly to a
01:13:35
neighboring Galaxy, then you will see
01:13:36
the same thing
01:13:38
and therefore the analogy with an
01:13:41
inflating balloon is used to complement you
01:13:44
I will propose another analogy that does not
01:13:46
cancel the first one, but it complements it, that is,
01:13:48
accordingly, from any Galaxy this is an
01:13:50
important statement, an observer would see the
01:13:52
same thing, astronomers in all galaxies
01:13:54
see the same law, but not everywhere
01:13:57
they call it Hubble’s law.
01:13:59
Apparently, although the Galaxy can
01:14:01
be in many places something is called the law
01:14:05
accordingly Everything looks as
01:14:08
if we have a ball but on which
01:14:10
Galaxies are not drawn because they
01:14:13
themselves would stretch when expanding and
01:14:16
Galaxies they are like, I don’t know
01:14:17
the jokes when the
01:14:19
surface of the ball is glued The ball
01:14:22
inflates and the galaxies become
01:14:24
further away from each other from whichever you
01:14:26
observe you will see the same
01:14:28
effect
01:14:30
the question arises naturally where is the center
01:14:32
of expansion
01:14:34
right people in this are still this
01:14:36
question about some suffer for some reason
01:14:39
short answer It is certainly correct
01:14:42
to observe the observable Universe
01:14:44
Nikol-center of expansion no,
01:14:47
because otherwise we would not see the
01:14:49
isotropic Hubble law throughout the entire sky, but we would
01:14:52
see some kind of throughness.
01:14:53
Galaxies from somewhere would fly past us
01:14:57
so, apparently, the
01:15:00
expansion center No, well, maybe we can set up
01:15:02
some strange models with the
01:15:04
expansion center at in another dimension, you can
01:15:05
slowly build strange models, they say
01:15:07
that we are in the center, but this is very strange and
01:15:10
cannot be explained at all. Why are we in the center?
01:15:12
Accordingly, there is no center and each
01:15:15
observer, due to the finite age of
01:15:17
the Universe, has a
01:15:19
finite area of ​​observation, that is, our
01:15:23
visible Universe, no matter what telescope we use they
01:15:26
didn’t build or there’s no telescope other
01:15:28
instruments we can learn to
01:15:30
register primary neutrinos
01:15:32
primary gravitational waves we will
01:15:35
register
01:15:38
Particles that have traveled a finite
01:15:41
distance in a finite time because the
01:15:43
propagation speed is finite and the
01:15:46
lifetime of our observable
01:15:48
Universe as we know it is also finite
01:15:52
but at the same time we know that
01:15:55
our visible part is not the entire universe
01:15:57
since we do not see any strange
01:15:59
edge effects, that is, we can see
01:16:01
some Galaxy; a
01:16:04
distant observer can also see it
01:16:07
now, but he sees some other
01:16:09
Galaxies that we do not see and, on the contrary,
01:16:11
we see some then Galaxies that are not
01:16:13
visible to him because the light did not have time to
01:16:15
overcome this distance, but taking into account the
01:16:17
accelerated expansion of the Universe, in
01:16:19
some cases it will not have time to overcome.
01:16:20
We will talk about this later, that is,
01:16:23
this is a fundamentally important statement,
01:16:25
also that we must draw all conclusions about the Universe in general
01:16:28
according to observation of a finite
01:16:31
region which certainly does not
01:16:34
exhaust everything, this of course
01:16:36
complicates any global conclusions and
01:16:39
therefore global conclusions in many
01:16:41
cases are either extrapolation or
01:16:44
some individual hypotheses not
01:16:47
directly related to observations, it is
01:16:49
only important that they do not contradict
01:16:51
observations in this finite region,
01:16:54
respectively Of course, the Universe or not,
01:16:56
we don’t know, that is, here we are, we see
01:16:59
some observer at the edge, he sees
01:17:02
some observer further on, and so
01:17:04
we can cover it up for quite a long time, apparently with
01:17:07
observers,
01:17:10
we proceed naturally from the
01:17:12
Copernican principle that our
01:17:14
picture is not isolated, that is
01:17:18
after all, that we are not at the center of
01:17:20
the universe and, accordingly, the question of whether
01:17:23
the universe is true or not, we by and large
01:17:25
cannot answer, we can only
01:17:27
say that the universe is definitely
01:17:28
larger than the observable one
01:17:33
and there are problems with the ball, so I want to
01:17:36
offer you another illustration,
01:17:38
which, among other things, is connected with
01:17:41
one of the interesting technological
01:17:42
scenarios, a scenario most likely
01:17:45
not related to reality,
01:17:48
but this is not significant, in fact, I want to
01:17:51
replace the ball with a plane, an
01:17:55
infinite plane is easier to imagine
01:17:57
than a ball of infinite size, perhaps,
01:18:00
accordingly, imagine an
01:18:02
infinite plane
01:18:05
Well, I don’t know, I want an infinite ball
01:18:08
somewhere, but it’s unclear hop and disappeared
01:18:11
Imagine a ball, you inflate it,
01:18:12
inflate it, inflate it, it went on for infinity I
01:18:15
don’t know It’s hard for me to imagine, but an
01:18:16
infinite plane is easier to imagine
01:18:18
Well, I don’t know Maybe I’m like that, if it’s
01:18:22
easier for you to imagine a ball, imagine a ball here
01:18:25
Imagine an infinite plane, now let’s
01:18:27
imagine that it’s metal
01:18:30
It’s all loosened into cells Now let’s
01:18:33
imagine that we are standing on them in galoshes,
01:18:36
just in case, we’ll start passing the
01:18:39
same current through this plane everywhere,
01:18:42
well, in general, it’s more or less clear How
01:18:44
to do it While there’s nothing wrong with it, the
01:18:47
current flows through the metal What happens
01:18:49
to the metal,
01:18:52
it heats up and expands, it heats up correctly
01:18:55
and expands, that is, our entire plane
01:18:57
will expand everywhere at every point
01:19:00
equally
01:19:04
and we will see that each cell
01:19:07
increases in size Imagine that
01:19:09
we have there in the center of the cell at the nodes
01:19:12
of the cell, as you like, there are
01:19:14
some reference points Poles and we
01:19:17
measure the distance between at their speed of
01:19:19
moving away from each other, I see the nearest
01:19:21
branch, for example, it is moving away from me
01:19:24
by a millimeter per second, but the second one is
01:19:27
already moving away by 2 millimeters per second
01:19:29
because there are two cells between me and
01:19:32
each is expanding at the same
01:19:34
speed, I see the third one, it is moving away at a
01:19:36
speed of 3 millimeters per second 4 mm per
01:19:40
second 5 millimeters per second obviously
01:19:42
since the infinite plane
01:19:45
will be a twig that is moving away from me
01:19:48
at a speed of 10 to 13 mm per second,
01:19:52
which is greater than the speed of light, and there will be
01:19:54
some kind that is moving away at 10-14 mm per
01:19:57
second 10 15 10 16 10 164 mm per second
01:20:01
if the plane is infinite, that is,
01:20:04
here
01:20:05
we get a very clear image that there is
01:20:08
nothing terrible in the fact that we have
01:20:12
clear, understandable knowledge that some
01:20:13
object is moving away from us at the speed
01:20:15
of light, this in no way contradicts the
01:20:17
special theory of relativity
01:20:18
special theory of relativity
01:20:20
essentially prohibits the fact that something will fly by here in front of
01:20:21
your surprised gaze at a
01:20:23
speed greater than the speed of light, and the
01:20:26
fact that you have something there somewhere that is
01:20:27
moving away due to the fact
01:20:29
that this plane
01:20:31
is expanding is of no interest to anyone has
01:20:33
nothing to do with one hundred
01:20:35
in general, a local theory. Naturally, a
01:20:39
person standing on that branch that is
01:20:43
moving away from us at a speed of 10-14
01:20:45
millimeters per second sees that the neighbors are
01:20:48
moving away from him now at the moment,
01:20:49
imagine that we all have the same clock is
01:20:52
now moving away from him at a speed 1
01:20:54
mm, that is, no local fast
01:20:57
movement occurs. Here is
01:21:00
the scenario that was sort of discussed, this
01:21:03
scenario of two branes, respectively, let's
01:21:06
imagine two Well, in
01:21:10
fact, three-dimensional manifolds, so it wo
01:21:11
n't be possible to imagine, but we have
01:21:13
two branes, let's imagine two-dimensional
01:21:29
yes yes, but with a plane this is not the case was She
01:21:32
always This is important, we will come to this later the
01:21:34
plane can always be
01:21:35
infinite Let’s imagine that we
01:21:38
have two branes Let’s imagine that these are
01:21:40
two planes immersed in the three-dimensional
01:21:42
world and we can imagine that they are
01:21:45
infinite but they experience
01:21:47
interaction with each other and in
01:21:49
in particular, they can, for example, collide,
01:21:51
that is, it turns out that you have spots on our
01:21:55
brane, let’s say, this is our marriage on
01:21:57
our brane in the past, at every point everywhere at the
01:21:59
same time something happened that
01:22:02
can be called a big bang, and at
01:22:04
that moment our brane began to stretch everywhere like that,
01:22:06
it could immediately be
01:22:08
infinite if you want
01:22:10
Well, at least in this
01:22:12
imaginary world of ours, and in a remarkable
01:22:14
way, the question from the center about
01:22:17
how it was all compressed into a point, not the entire
01:22:20
non-infinite Universe was not compressed
01:22:22
into a point, and our visible part of the Universe
01:22:25
occupied a small volume at the
01:22:27
corresponding moment corresponding to the
01:22:29
big bang That is, it seems to me that
01:22:31
such an illustration at least how
01:22:32
this restores mental health,
01:22:37
as far as I know No,
01:22:42
well, that is, so that one concentrically
01:22:44
fits the other I have never heard, but
01:22:48
yes, the question for me is why would you say
01:22:51
that this cannot be done be she I don’t know why
01:22:56
it’s good the
01:22:58
second water part We have finished and we
01:23:01
must start today the third part So that
01:23:03
next time we can calmly
01:23:04
talk everything out slowly
01:23:06
in cosmology, some features arise
01:23:11
associated with this very expansion of
01:23:13
the universe,
01:23:16
it is convenient to draw such a two-dimensional graph
01:23:18
where we have time from we
01:23:20
can’t get away from it and one spatial
01:23:23
axis is horizontal, the
01:23:24
spatial axis moment 0 is not
01:23:27
very good for us, but it’s not that it’s very
01:23:28
interesting to us, even but we’ve forgotten about it for now,
01:23:32
we’ve forgotten about it for now. We have two
01:23:35
objects, they naturally can
01:23:38
constantly radiate there but we are interested in
01:23:42
the emission of a specific photon there
01:23:44
sometime in the past by one object and the
01:23:48
photon was released towards another object.
01:23:50
During this time the Universe expanded and the
01:23:53
Photon got into this object, that is, we are the
01:23:57
object. We are sitting here to observe,
01:23:59
we registered photons released in
01:24:02
the past by this object now this
01:24:04
object is here,
01:24:06
that is, the objects have changed the physical
01:24:08
distance between them due to the expansion of
01:24:10
the Universe, these are two distant objects,
01:24:14
so we have a question:
01:24:18
What is the distance between the objects we need to
01:24:20
say because there are several
01:24:22
answer options, the first answer option
01:24:25
is the distance between two objects,
01:24:27
now
01:24:29
this is very important clear distance,
01:24:31
a certain problem is that now we do
01:24:34
n’t see this object,
01:24:36
we don’t know what’s happening to it and the
01:24:38
distance to it now acquires a certain
01:24:40
formal meaning
01:24:42
is the distance that was between
01:24:45
objects when the Photon was released,
01:24:49
this is another important distance, it is
01:24:51
used in cosmology, there is a third
01:24:54
distance is the path traveled by the photon,
01:24:56
there is such a simple illustration that you can see that
01:24:59
all three distances are different if the Universe is
01:25:02
fast enough, then the greatest
01:25:04
distance is this, then this is the path of
01:25:07
the photon and then this is this distance,
01:25:09
so don’t be surprised when you read there and
01:25:13
hear that
01:25:17
astronomers showed an image of the Galaxy
01:25:20
that is now are located at a distance of
01:25:22
35 billion light years
01:25:30
Well, I didn’t even bother here, but
01:25:33
here if it was constant then the exponential would be It
01:25:37
looks like something, yes, well, I kind of drew how
01:25:41
PowerPoint draws me So I won’t
01:25:45
say that this is
01:25:46
just an exponential, some kind of crookedness
01:25:50
Well, that means I’ll repeat myself don’t be alarmed
01:25:52
If you hear that
01:25:54
this is an image of the Galaxy, the distance
01:25:56
to which is now say 35 billion
01:25:58
light years, despite the fact that the Universe is
01:26:00
less than 14 billion years old, the light would not have time to
01:26:04
travel 35 billion light years,
01:26:06
of course This is understandable, but this is not necessary 35
01:26:09
billion is the distance from all to of these
01:26:11
and this distance can be large,
01:26:13
it can be in particular more than 14
01:26:15
billion Okay, let's
01:26:18
get acquainted with different types of distances,
01:26:20
we will continue to encounter them in the form of
01:26:21
formulas, including for a bunny, so the first
01:26:25
distance is called the accompanying
01:26:27
distance, its beauty is that it does not
01:26:30
change with expansion This is a
01:26:33
very convenient quantity for the Universe, with which it can be
01:26:35
compared, let’s imagine that our inflating
01:26:37
ball is a Globe and you can set the
01:26:40
distance from I don’t know Madrid to Tripoli
01:26:44
in degrees
01:26:46
and no matter how you inflate the ball, you
01:26:49
still have a geographic grid, the distance
01:26:51
in degrees between points does not change
01:26:54
and accordingly, the same thing You can
01:26:57
enter into cosmology you number the
01:27:00
Galaxies, the distance is actually
01:27:02
not X, it’s a
01:27:04
Greek letter just like that PowerPoint usually writes it, its
01:27:08
own distance is indicated by
01:27:11
the letter X, respectively, the Universe
01:27:13
is expanding, but the Galaxies remained the same,
01:27:16
their order has not changed due to the
01:27:19
expansion of the Universe and we can each
01:27:22
attribute the
01:27:23
coordinate of such an expanding grid and the
01:27:27
distance will be of the expanding grid
01:27:28
is called the accompanying distance, I
01:27:30
repeat, it does not change. This is very convenient, the
01:27:33
next distance is the proper
01:27:36
distance. Let me jump over
01:27:40
this. The distance that is measured at a
01:27:43
given moment in time. Well, let’s
01:27:44
physically imagine in our minds that
01:27:46
instantly some kind of roulette has been laid out, it
01:27:49
has spun between us and a
01:27:52
distant galaxy,
01:27:54
and then this will be its own distance;
01:27:58
it naturally changes
01:28:02
due to the expansion of the Universe; it can be
01:28:04
characterized by one single
01:28:06
quantity, since the Universe is fortunately
01:28:07
homogeneous isotropically on a large scale;
01:28:09
we write all these formulas for a
01:28:11
homogeneous isotropic a universe that
01:28:13
is expanding equally everywhere and this
01:28:18
value is the scale factor, designated
01:28:19
here by the letter K the scale factor depends
01:28:22
on time, respectively, the proper
01:28:25
distance between galaxies depends on
01:28:28
time, this accompanying
01:28:31
distance changes and the scale factor changes, it is
01:28:33
convenient to set in absolute values ​​it
01:28:36
is possible to make the proper distance
01:28:38
in such a way that accompanying so
01:28:41
that now at the moment
01:28:43
the coefficient A is equal to one so
01:28:46
often they use it conveniently and then you
01:28:50
will easily recalculate all this
01:28:53
accordingly
01:28:57
as the Universe expands, our own
01:29:00
distance grows Our Universe
01:29:01
has only been expanding all its life and therefore the
01:29:04
own distance in the Universe has
01:29:07
only grown
01:29:12
for its own distance there are all sorts of
01:29:16
simple formulas to formulas, I’ll come back later,
01:29:19
I just don’t want to waste time now on
01:29:21
what is alpha What is h0,
01:29:24
we’ll get to that later, we can at least
01:29:27
get to the law
01:29:29
Hubble’s law. Probably somehow we’ll deduce it
01:29:31
quickly and next time here from this
01:29:33
place approximately Let's start well So
01:29:38
Well, let's just say what is written
01:29:40
here, I'll
01:29:42
write it on the board
01:29:46
What exactly to look at so as not to
01:29:49
change the distance So we have a
01:29:51
Metric, that is, we start from here
01:29:54
We have a very simple Metric
01:29:58
DS square
01:30:00
in squared minus And in the square I have
01:30:07
Dail in the square marked And this function of time
01:30:11
now So let's jump over here
01:30:14
we can enter our
01:30:18
own Distance that is
01:30:20
interesting to us, that is, the Hubble law is important
01:30:22
enter the own distance
01:30:25
accordingly, we enter it in this simple
01:30:27
way
01:30:30
DD
01:30:32
this is a
01:30:37
Here
01:30:38
accordingly, to determine the
01:30:40
proper distance, we need to
01:30:42
integrate, we believe that we
01:30:45
are integrating instantly,
01:30:47
the roll turned instantly, so the scale
01:30:49
factor we have is what it is.
01:30:51
Let's put here that this is a function of
01:30:54
time, but D proper from we can add here.
01:31:00
But according to Dail, we integrate
01:31:04
the integral presented this just an
01:31:06
accompanying distance hi, so I
01:31:09
get a nahi,
01:31:12
respectively, the distance from anakhi, but
01:31:15
as we entered. That is, it’s like Everything
01:31:17
is clear now, the speed of the speed, as we
01:31:19
will see, can also be defined in different ways,
01:31:21
that is, the speed is a change in some
01:31:23
distance over time, time y us
01:31:25
Let one thing we don’t
01:31:27
bother with the distance yet We choose
01:31:28
actually and therefore we say that
01:31:31
the speed is D in
01:31:36
time and substitute what we know Well, that
01:31:39
is, this equals d a h
01:31:43
pdt and this in turn will equal
01:31:49
Yes according to DT on a
01:31:53
derivative of the
01:31:58
derivative archi is equal to zero,
01:32:00
the corresponding distance does not change,
01:32:01
so it will be to the traffic rules by Hi
01:32:07
So, accordingly, I can
01:32:12
divide and multiply by and that is, I
01:32:15
will have to the traffic rules
01:32:16
divided by
01:32:19
and will be Ahi This is the proper
01:32:22
distance
01:32:23
[music]
01:32:24
and this thing I call constant hub
01:32:27
constant hub this is a function of time as
01:32:30
you see because before traffic rules and And this is a
01:32:32
function of time Therefore the
01:32:34
hubble constant is changing all the time here is the constant
01:32:36
Hubble Let's separately
01:32:38
And with the point on where the point is the derivative with respect to
01:32:41
time here the
01:32:43
constants change and usually
01:32:47
write the icon 0 this is constant Hubble
01:32:52
now the
01:32:54
present time is like a directly
01:32:57
immeasurable parameter, by and large,
01:32:59
that is, there is no instrument for measuring
01:33:01
constants, you recalculate it through
01:33:04
some quantities,
01:33:06
but this is a very important cosmological
01:33:08
parameter that characterizes the
01:33:11
modern model of the Universe; constants
01:33:14
change as the
01:33:15
Universe expands; it is convenient to write it as the
01:33:19
Hubble constant depends from red shift
01:33:20
red shift But we will probably
01:33:22
next time introduce
01:33:25
accordingly, it is important for us that there
01:33:28
may be 4 main
01:33:31
ingredients in the Universe. Let me not
01:33:34
detain you next time, this is where we
01:33:35
will start from here and on the right of the outer corner we will talk
01:33:37
about all these ingredients just
01:33:40
more- less We'll have time next time
01:33:41
thank you
01:33:42
[music]

Description:

На этой лекции уважаемый Сергей Борисович, наконец-то, завершит тему ГАЛАКТИК и ТЁМНОЙ МАТЕРИИ! А точнее расскажет про СКЕЛЕТ ВСЕЛЕННОЙ, ВОЛОКНО ТЁМНОГО ВЕЩЕСТВА, "МОСТ" между ГАЛАКТИКАМИ, познакомит со СТАНДАРТНОЙ МОДЕЛЬЮ ЭЛЕМЕНТАРНЫХ ЧАСТИЦ и ответит, какая ЭЛЕМЕНТАРНАЯ ЧАСТИЦА отвечает за ТЁМНУЮ МАТЕРИЮ, и как найти эту ЧАСТИЦУ, и какие методы ПОИСКА ТЁМНОЙ МАТЕРИИ астрофизики уже используют на практике! Зрители узнают об АННИГИЛЯЦИОННОМ СИГНАЛЕ, ФОРМИРОВАНИИ ГАЛАКТИК, ILLUSTRIS, КРУПНЫХ и ВЗАИМОДЕЙСТВУЮЩИХ ГАЛАКТИКАХ, СЛИЯНИИ 2-х ЧЁРНЫХ ДЫР, их ПЕРИОДЕ ОБРАЩЕНИЯ и ИЗЛУЧЕНИИ СВЕРХМАССИВНЫМИ ЧЁРНЫМИ ДЫРАМИ ГРАВИТАЦИОННЫХ ВОЛН! Сергей Борисович также на доске сделает выводы ОЦЕНОК массы ГАЛАКТИКИ, температуры ГАЗА в ГАЛО ГАЛАКТИКИ и ВРЕМЕНИ ПАДЕНИЯ 2-х ГАЛАКТИК (МЛЕЧНЫЙ ПУТЬ и АНДРОМЕДА) друг на ДРУГА в процессе ГРАВИТАЦИОННОГО ПРИТЯЖЕНИЯ! А на второй части лекции после перерыва слушатели начнут изучать новую тему - КОСМОЛОГИЮ и узнают о ФОРМИРОВАНИИ СКОПЛЕНИЙ и СТРУКТУРЫ ВСЕЛЕННОЙ, ЛАНИАКЕЕ, "ДИПОЛЬНОМ" ОТТАЛКИВАНИИ, СКЕЛЕТЕ ВСЕЛЕННОЙ, СОПУТСТВУЮЩЕМ и СОБСТВЕННОМ РАССТОЯНИИ, а закончат ЗАКОНОМ и ПОСТОЯННОЙ ХАББЛА! Как остывает РЕЛИКТ? Почему ВСЕЛЕННАЯ РАСШИРЯЕТСЯ и как ЭТО РАБОТАЕТ? Где ЦЕНТР РАСШИРЕНИЯ и СУЩЕСТВУЕТ ли ОН? И КОНЕЧНА ли ВСЕЛЕННАЯ? Вы сможете ответить на эти вопросы, прослушав лекцию! Наши соцсети: паблик ВК: https://vk.com/public212939391 Инстаграм канала "МГУ 112" (признана запрещённой социальной сетью на территории РФ): https://www.facebook.com/unsupportedbrowser YouTube канал Сергея Борисовича: https://www.youtube.com/channel/UCGk5wyYgpGKuu5Wkjg0WIzQ ВК Сергея Борисовича: https://vk.com/id6382040 Социальные сети оператора (Всеволод Наумов): ВК: https://vk.com/piiv0_seva_tri_k0mpa Инстаграм (признана запрещённой социальной сетью на территории РФ): https://www.facebook.com/unsupportedbrowser

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