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0:00
I'm Dr Karl, coming to you from the lands
0:02
of the Gadigal people of the Eora Nation.
0:04
I acknowledge Aboriginal and Torres Strait Islander
0:07
peoples as the first Australians and
0:09
traditional custodians of the lands where we
0:11
live, learn and work.
0:14
G'day,
0:15
Dr Karl here, Shortlandism Sciences, part two
0:18
of The Early Universe Ran Slower,
0:20
with my wonderful colleague Professor Geraint Lewis.
0:22
Welcome back. Good morning, Karl. How are you doing? I
0:25
said Geraint wrong again. No, no, no. Have I lost
0:27
the proper way? Yeah, you're fine there, Karl.
0:29
So you were talking about the damped
0:31
drunkard's walk. Yes. So by the way, just
0:34
to give the audience time to speed up,
0:36
albatrosses find their food by something
0:38
different, a Levi walk, where
0:41
in a drunkard's walk it's always the same
0:43
size of step, but in a random
0:45
direction. In a Levi walk, the step
0:47
can be different. And this turns out to be more
0:50
efficient for them to find food. Okay, now
0:52
you've had a chance, beloved audience, we went
0:54
through supernovas and they're relatively
0:56
easy to deal with, with a clock, because
0:59
they were damp and down from their brightness
1:01
at a certain fixed rate. And in the early universe
1:03
it was happening earlier, and then you were saying, ah, but quasars,
1:07
they're really out there, but we're not seeing
1:09
it in quasars. And then you went into
1:11
random walks to take it away. Yeah, if you
1:13
look at the variations of quasars,
1:15
said it's up and down and up and down, etc. In
1:17
this new sample of data that the American
1:20
team released, they were able to characterize
1:23
the light curves and found something
1:25
that we could use for a tick, this timescale
1:27
for the damping of that random
1:29
walk, the drunkard's walk in the light curve. Out of the
1:32
millions of quasars, of which
1:35
we've characterized or numbered probably tens of thousands,
1:38
they focused on a couple of hundred. This
1:41
was at the end of 2022. And so
1:43
I had this sample of
1:45
quasars. And the question is, can
1:47
we find this expected
1:49
signature that the universe appears to run slower
1:52
when we look through our telescopes? So you need
1:54
a statistician, a Bayesian statistician. So
1:57
look up Bayesian statistics on Wikipedia.
1:59
out of the way. So you got your mate
2:02
who can help you with statistics, right? The key
2:04
problem that we have is I've got these
2:06
quasars. Some of them are big, some
2:09
of them are small in terms of their mass, they're not identical.
2:12
And there's another added complication is
2:14
that when I look through my telescope
2:17
at a quasar, I tend to look at it through
2:19
a filter. So I would look
2:21
at it in blue light, or green
2:24
light, or red light. If
2:26
I see red light today, this
2:28
doesn't mean that when it was emitted it was
2:30
red because the expansion of the universe stretches
2:33
the light. And the bigger the wavelengths,
2:35
the different the colour. Yeah. So I could
2:37
be looking at some object and I'd
2:40
be seeing material which is very close to the black
2:42
hole, so that could be varying rapidly.
2:44
Or I could be seeing material which
2:46
is further out where it's quieter
2:48
and would be varying less rapidly. There's
2:51
complications, there's always complications. But
2:54
with this sample what we were able to do is start to group
2:58
quasars together. You want to get something
3:00
you can deal with. Yeah. So we were able to group
3:03
them and so we said, oh, this
3:05
group, we expect their variability
3:07
to be very similar. The only
3:09
difference between them should be their
3:12
distance and their time. The expansion
3:14
of the universe, right? Some of them are nearby, some
3:16
of them are further away and the only difference that we should see
3:18
in their timescales is due to the expansion
3:21
of the universe, the time dilation effect.
3:23
Did I actually make a correct guess? You did.
3:26
For what's in my life? Yeah. Jeez.
3:28
Okay, go on. So we went through and we did this and
3:31
again, I'm personally a big fan of Bayesian statistics.
3:33
I do love them. I don't understand them. That's
3:36
another thing for another time. But it means that you
3:38
make your prediction
3:40
based on past events,
3:43
but more than that. And Bayes was a minister
3:45
who rode around on a horse in the 17 or 1800s or something. Yes.
3:49
So we had a very interesting notion about how you should treat data
3:52
and how you should test hypotheses,
3:55
which is what science is all about. So what
3:57
we did is we said, oh, What
4:00
if we assume that there is no cosmological
4:02
time dilation? What does the data say
4:04
about that? What if we say that there is? What
4:06
does the data say about that? So we proposed
4:09
our hypotheses and said, does
4:11
the data support that or not support
4:13
it? And what we did is we turned the handle.
4:16
And again, it's a topic
4:18
I love, but clearly it was not
4:20
for the discussion here today. As we
4:23
did our comparison, and what popped out is
4:25
that the best hypothesis to
4:27
explain the data in front of us is
4:29
that there's a cosmic time dilation, that
4:32
the more distant quasars are varying
4:35
more slowly than the nearby quasars. Is
4:37
it easy to describe what you're looking at? No.
4:41
Unless you've done basic statistics. It's
4:43
like looking at the stock market, right? Because
4:45
you can zoom in and zoom in, and there's always
4:47
variability going on. The time scale
4:49
is hidden in that variability, but
4:51
it's there. We can get a handle on statistics. People should read
4:53
your paper. And by the way, I'd like to point out that
4:56
even your brain wasn't enough, that you had to team
4:58
up with somebody who specialised in that subset
5:01
of knowledge called Bayesian statistics, and
5:03
then subspecialise again related to
5:05
astronomical events, and then subspecialise again related
5:08
to quasars. Very rarely is science
5:10
done by individuals anymore, right? You work with people
5:12
that have expertise, and you bring their expertise
5:15
together to answer the big questions.
5:17
There was somebody about 20 or 30 years ago who
5:20
looked at quasars and said, nah. I found
5:22
their paper. What did they do wrong? Or did
5:24
they have Bayesian stuff happening? This is an astronomer
5:26
at Edinburgh called Mike Hawkins. And Mike
5:29
was collecting data actually in Australia.
5:32
So just aside Cunha Barabran,
5:34
he's signed in Springs Observatory. And there's a
5:36
special telescope there called the Schmidt Telescope.
5:39
And so Schmidt telescopes are famous because in
5:41
the old days, they allowed you to get
5:44
in-focused view of a large chunk
5:46
of sky. So it'd be sort of like a wide-angle-y
5:49
thing. Yeah. So large chunk
5:51
means a couple of times bigger than the full moon, but
5:53
not that much bigger. OK. Moon is half a degree.
5:56
Yeah. So you could collect data
5:58
on photographic films. because that's what
6:00
they had back then. And then those
6:02
films were scanned by machines back
6:04
in the UK, one in Cambridge, one in Edinburgh. And
6:07
they could identify quasars in these scans.
6:10
So Mike had been collecting data for a number of years
6:13
and he had identified quasars and so he had
6:15
like 20 to 30 years worth of light
6:18
curves, the variations that you see in quasars.
6:21
But they were poorly
6:24
sampled. And what I mean by that is
6:26
that he was getting data every once a
6:28
year or once every six months, etc.
6:30
So if you look over 30 year span, you see
6:33
a bunch of points, but you've got gaps,
6:35
which could be fatal if you look at something like the stock market
6:38
to make money quickly. Exactly. If you were trying
6:40
to do the stock market and you only got a stock price
6:42
once every year, and you were trying to work
6:44
out the behavior, then there's lots of stuff going on in
6:46
between. Firstly, the data wasn't
6:49
very well sampled. But also he was
6:51
working at a time before people had gotten good
6:53
enough data to even get a statistical
6:55
handle on how quasars varied.
6:58
Ah, so he was a very early person doing the best
7:00
he could with what was available back then. Basically,
7:02
he did the statistical tests that he could
7:04
do with the data. And it came back and it was
7:06
like, no, it probably was
7:09
just is not the handle in the data to
7:11
get a measure of the time scale. So
7:13
it's just not well sampled enough. Okay,
7:16
before we dive into the other objects, so I want to talk
7:18
about, did you use a lot of computing
7:20
power or was it relatively minor?
7:22
This was relatively minor in today's
7:25
world. So one of Brendan's things
7:27
that he's done in his research, he's written a special
7:29
program called D-NEST4.
7:32
D? D-NEST4, Diffusive
7:34
Nested Sampling Version 4. Oh,
7:36
we have three was. Yeah,
7:39
okay. And so what this does is it
7:41
does your Bayesian analysis, it goes around probability
7:44
space and checks your hypothesis, etc.
7:47
And it turns out that for this size of problem,
7:49
we can actually do this on a relatively
7:52
small computer. So I did most of the calculations on my
7:54
desktop computer, which is a computer
7:57
compared to something 15 years ago. Yes, yes.
8:00
The bigger problems we do need to do
8:02
the calculations on actual supercomputers
8:04
that exist today because you
8:06
essentially have to interrogate the
8:08
data many millions of times
8:10
with your hypotheses and then from
8:13
that you draw out the answers. Okay getting back to
8:15
your paper the detection of the cosmological
8:17
time dilation of high redshift quasars,
8:20
you and your mate Dr Brendan J. Brewer
8:23
managed to do something with the complicated things called
8:26
quasars. That
8:28
leads us to other objects gamma
8:30
rays which are very energetic
8:33
and fast radio bursters which
8:35
I don't understand either. So normally astronomers
8:37
look at the sky right and you get your images and you do
8:40
your work and all that kind of stuff. One of the
8:42
things that we haven't really looked at in detail
8:44
is how much the sky changes on a
8:47
relatively short time scale. Things
8:49
that vary quickly are still relatively
8:52
new. So gamma ray bursts have been known for
8:54
a little while. The Vila satellites
8:56
by the Americans discovered something that the
8:58
South Africans were setting off nuclear weapons. Then
9:01
they finally discovered that there were gamma rays coming from space
9:03
not just from nuclear weapons. Exactly. And
9:06
so people found that there are gamma ray bursts. Things
9:08
that explode release these high energy
9:10
gamma rays. Huge amount of energy. Huge amount of energy
9:12
and we found that they are at huge distances,
9:14
cosmological distances. Yeah this was bothering
9:17
the American spy satellite. Billions of layers
9:19
and more recently we discovered that when we look
9:21
at the radio sky we find something similar,
9:24
fast radio bursts. Something goes
9:26
bang and releases radio waves and
9:28
then those radio waves spill out into the universe
9:30
again. They appear to be coming from cosmological
9:33
distances. So these must be powered
9:35
by very energetic, probably
9:37
quite violent events. So like a gamma
9:39
ray burst might be neutron stars colliding.
9:42
Oh yeah. And fast radio bursts must
9:44
be something similar as well. There is
9:46
one hypothesis that the gamma ray bursts might
9:48
be neutron stars colliding. Yeah. And
9:50
be able to tie them in with gravitational
9:53
wave detection if the frequency wavelength is
9:55
right? Yes. So I mean this is
9:57
what people are trying to do. When they detect a gravitational wave
9:59
they... They take a look to see if they can pick up light
10:02
from those objects, so optical light or gamma
10:05
rays or radio waves. So by light, you
10:07
as an astronomer mean anything from gamma rays
10:09
all the way up to the other end? Yes,
10:11
electromagnetic radiation. So again, we
10:13
don't quite understand the physics of what's powering
10:16
these, but we know that they go bang and we
10:18
know that they're at large distances. So
10:20
they too should show this cosmic
10:22
time dilation. A place where
10:25
we are is playing this same game
10:27
again. How do I know that this gamma
10:29
ray burst and that gamma ray burst are
10:31
intrinsically similar objects? Because
10:34
Type 1A supernovas are what we call a standard
10:36
candle and they're essentially the same. You're
10:38
saying there could be many different types of gamma ray burst,
10:41
many different types of fast
10:43
radio burst. Yes. Imagine
10:45
that you've got one fast radio burst that's created
10:47
by an object of this mass and an object
10:49
of that mass interacting. But you change the
10:51
masses and you still get a fast radio burst, but maybe
10:54
it puts out twice as much power or
10:56
half as much power. It's a different time scale. By
10:58
the way, how much slower was the universe
11:00
running back then? With the measurements that we
11:03
made, instead of looking back on the half
11:05
the age of the universe, with these quasals,
11:07
because they're so bright, we looked back over 90% the
11:10
age of the universe. So how
11:12
many billion years after the Big Bang or how many billion
11:14
years back is that? A billion or so. After the
11:16
Big Bang. A billion. So
11:18
at three minutes you get the nuclei
11:20
cooling down. At three, 80,000 years
11:23
you get the electrons joining up and the
11:25
first stars are around 400 million. Is
11:27
that what we still think? Yes,
11:30
something like that. They keep pushing these numbers back. Stars
11:32
seem to form quite early in the universe. Thank
11:34
you. Just wonderful space telescope, I guess. Yes. Yes.
11:38
Okay. So at point two or three or four
11:40
of a billion, you get the first stars somewhere there and then you're
11:42
picking up stuff at a billion years. Between
11:45
a billion and two billion, roughly, how did
11:47
it get so big, so powerful, so fast? Well,
11:49
the universe was very different to the universe
11:51
today, right? It was a lot denser, so
11:53
material gathered together very, very quickly.
11:56
These massive stars, they lived their lives
11:58
very fast. They're born very massive
12:01
and they live for a few million years.
12:04
So like twice the mass of our sun or ten or
12:06
a hundred? A hundred times. A hundred.
12:08
That is big. A hundred times and pure
12:11
hydrogen and helium. Oh because there's no debris
12:13
from nuclear reactions in
12:15
stars making energy because they're the first
12:17
generation of stars. The universe
12:19
was a different place. Massive stars
12:22
could have been the seeds for the new black holes
12:24
because when they die they create black holes. Nuclear
12:27
could flow in very very quickly so you
12:29
can form these quasars in the very
12:31
very early universe. When we saw them
12:34
basically the time scales back
12:36
then from our viewpoint here the universe
12:38
was running at about a fifth the
12:40
speed that we see it today. If
12:43
we were magically able to go in a time machine
12:45
and a distance machine and go back then would we
12:47
notice? No because we'd be
12:50
obeying the laws of the universe. We'd be
12:52
looking at our watches just going one second per second
12:54
everything is fine but if I spied you through
12:56
my telescope and I could see your watch
12:58
I would see it tick five of my seconds
13:01
for your watch to tick one second.
13:03
Now I'm thinking of a question from
13:07
a nine year old intelligence student
13:09
at primary school can we use this to make a
13:11
time machine? We can use time
13:13
dilation to make a time machine but you
13:15
can't use the cosmological time dilation because it
13:17
would mean that it would have to go into the past anyway.
13:20
Right so they would need a time machine but
13:22
we can make a time machine using gravity. What?
13:25
Because another consequence of Einstein's equations
13:28
is that the rate at which clocks
13:30
tick is relative based upon where you are in a
13:32
gravitational field and we know this works because
13:34
GPS needs to correct for this. So
13:37
if you go down near a black hole
13:39
and hang out near the event horizon
13:41
the point of no return your
13:44
clock down there ticks really slowly
13:46
compared to a clock somewhere else hanging
13:48
out in the universe. So you can go
13:50
down into a black hole
13:52
hang out there and come back out. Hang around
13:55
to be precise hang out just outside
13:57
the event horizon. Definitely not inside. And
14:00
definitely not into the black hole itself which has zero size
14:02
which is inside the event horizon but you go very
14:05
close and you might hang out there for
14:07
months and the universe has aged
14:10
by ... We've all seen Interstellar, right? Come out
14:12
and his daughter's now an old woman. Yeah,
14:15
that kind of thing can happen. So you can time travel
14:17
into the future. Time travel into the future is easy.
14:20
Yep. Right? We haven't cracked time
14:22
travel into the past. Wasn't there
14:24
the one from John Wheeler where you get a neutron star
14:26
and you fashion it into a cylinder one kilometer in diameter
14:28
and 20 kilometers long and spin it at a thousand
14:31
rivers per second. The outside is moving at half the speed of light
14:33
and you go back in time to when it was created you go into a tidal
14:35
over around it.
14:36
Yes,
14:37
but that's an engineering problem, right?
14:39
A major engineering problem. So look, theoretically
14:42
we can work out time travel. That's definitely
14:44
true. The question about whether or not it's
14:47
ever physically realizable
14:49
is it something that we could ever build? We
14:52
don't know. We don't know. And of course
14:54
people have conjectures. They say time
14:56
travel is impossible because essentially I don't like
14:58
it. There was this famous story that Stephen
15:00
Hawking decided that there was no time travel because
15:02
he had a party and invited time
15:05
travelers from the future to come to his party and
15:07
nobody turned up. That's where he sent out invitations
15:09
saying, come to my party four weeks ago. Yeah. Maybe
15:12
time travel has got something better to do than hang out with
15:14
Stephen Hawking at a party, right? He did
15:16
like pizza apparently. This is one of the things that
15:19
I love about Einstein's general relativity.
15:22
Time is malleable. It is definitely
15:24
malleable. And we have the equations that tell us how
15:26
to shape and bend and warp it. What
15:29
we've got to do of course is ask, can
15:31
we ever actually manipulate gravity
15:34
in that kind of way? Because if we can
15:36
and the equations are right
15:38
then time travels possible as
15:41
our warp drives to travel at any speed through
15:43
the universe. At this stage we have to bring it
15:45
to a halt. So you
15:47
and your colleague, Dr. Brendan J.
15:50
Brew, who's a student who's an astro
15:52
statistician, which I didn't even know
15:54
existed until today, you have shown
15:57
that the early universe ran
16:00
one-fifth slower, somewhere between one and
16:02
two billion years after the universe began. Forget
16:04
the universe is 5,000 years old thing. How
16:07
can people follow you and your fine work? So I have a website
16:09
which I update very regularly at garintflewis.com.
16:23
And you like me are still stuck on X or Twitter
16:25
or whatever Elon calls it today depending on
16:27
what he had for breakfast. Yes, but as soon as he introduces
16:29
a charge, I'm gone. Me too. Yeah.
16:33
Thank you so much. We had so much fun.
16:35
Professor Garin? Yeah, that'll do. See
16:37
you next time. Bye. Thanks,
16:39
Carl. It's getting hotter. Our population's
16:42
aging. We're glued to our screens
16:45
and AI, well, it's
16:47
changing the world as we speak. We're
16:50
facing big challenges. We
16:52
need big solutions. I'm
16:56
Mark Scott, the Vice Chancellor at the University
16:58
of Sydney, and I've got a backstage
17:01
past to the people making
17:03
change happen. The solutionists.
17:05
Look for it in your favorite podcast app.
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