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The universe is falling apart. | 0:00:02 | 0:00:04 | |
Something is forcing galaxies | 0:00:04 | 0:00:06 | |
to rush away from each other at ever increasing speeds. | 0:00:06 | 0:00:10 | |
Ever since this alarming discovery, | 0:00:11 | 0:00:14 | |
physicists have struggled to understand what might be causing it. | 0:00:14 | 0:00:17 | |
So far, they've come up with a name. | 0:00:19 | 0:00:22 | |
They've called it dark energy. | 0:00:23 | 0:00:25 | |
Dark energy is basically our name for that thing | 0:00:28 | 0:00:32 | |
that we don't understand. | 0:00:32 | 0:00:33 | |
It's not the colour dark, | 0:00:36 | 0:00:38 | |
it's just the expression of our ignorance as to what is this stuff. | 0:00:38 | 0:00:42 | |
The discovery of dark energy really surprised theoretical physicists | 0:00:42 | 0:00:47 | |
and remains a deep mystery of nature. | 0:00:47 | 0:00:49 | |
Until dark energy, we had every reason to be as confident | 0:00:52 | 0:00:56 | |
in Einstein's theory of general relativity | 0:00:56 | 0:00:58 | |
as he was himself. | 0:00:58 | 0:00:59 | |
In the last few days, I've completed one of the finest papers of my life. | 0:01:01 | 0:01:05 | |
But now things are less certain. | 0:01:07 | 0:01:10 | |
Einstein doesn't explain dark energy and, so far, | 0:01:10 | 0:01:14 | |
neither has anyone else. | 0:01:14 | 0:01:17 | |
We are absolutely still lacking great ideas. | 0:01:17 | 0:01:20 | |
So, it is crying out for some new breakthrough, new thinking. | 0:01:20 | 0:01:26 | |
Because it might be that dark energy is not a thing at all, | 0:01:26 | 0:01:30 | |
but simply evidence that the physics itself is wrong, | 0:01:30 | 0:01:34 | |
that we need another Einstein. | 0:01:34 | 0:01:36 | |
What Einstein did was he actually came out | 0:01:39 | 0:01:42 | |
and looked at the bigger picture | 0:01:42 | 0:01:43 | |
and put all these different elements together | 0:01:43 | 0:01:46 | |
to come up with the theories that he had. | 0:01:46 | 0:01:48 | |
It might be time for the bigger picture to be re-evaluated. | 0:01:48 | 0:01:53 | |
There's definitely room for another Einstein to come in | 0:01:53 | 0:01:55 | |
and shake everything up and tell us | 0:01:55 | 0:01:58 | |
that we've been looking at things completely wrong up until now. | 0:01:58 | 0:02:01 | |
Would-be latter-day Einsteins the world over are on the hunt | 0:02:03 | 0:02:06 | |
for answers to modern science's most enduring problem - | 0:02:06 | 0:02:10 | |
to paint the biggest picture of all, | 0:02:10 | 0:02:13 | |
to finally solve the mystery of dark energy. | 0:02:13 | 0:02:16 | |
Energy is all around us. | 0:02:32 | 0:02:34 | |
It comes from the sun, from chemical reactions, from electricity. | 0:02:35 | 0:02:41 | |
Energy powers our vehicles, heats our homes, lights our nights. | 0:02:41 | 0:02:46 | |
Understanding energy has transformed our planet and our lives. | 0:02:47 | 0:02:51 | |
Dark energy is something altogether different. | 0:02:53 | 0:02:56 | |
It seems to serve no useful purpose at all, except to show us | 0:02:56 | 0:03:01 | |
that we understand less than we thought we did. | 0:03:01 | 0:03:03 | |
Dark energy arrived wholly unexpectedly | 0:03:09 | 0:03:13 | |
at the very end of the 20th century. | 0:03:13 | 0:03:15 | |
In 1998, a young scientist called Saul Perlmutter was thinking | 0:03:17 | 0:03:22 | |
some very big thoughts indeed. | 0:03:22 | 0:03:24 | |
As a graduate student, I really wanted to find a project that | 0:03:24 | 0:03:28 | |
would answer some, or that would at least be looking at some, | 0:03:28 | 0:03:31 | |
very philosophical questions, something that felt like it | 0:03:31 | 0:03:34 | |
was meaningful about the world we live in | 0:03:34 | 0:03:37 | |
in some, you know, deep way. | 0:03:37 | 0:03:39 | |
The question that's been really exciting me is | 0:03:46 | 0:03:50 | |
whether the universe will last for ever. | 0:03:50 | 0:03:52 | |
Do we live in a universe that is infinite, | 0:03:52 | 0:03:55 | |
or, some day, will it come to an end? | 0:03:55 | 0:03:57 | |
The two big options at that time | 0:03:59 | 0:04:01 | |
were that the universe could expand for ever, | 0:04:01 | 0:04:04 | |
but just slow and slow and slow, | 0:04:04 | 0:04:06 | |
but forever be expanding. | 0:04:06 | 0:04:08 | |
Or, if there was enough stuff in the universe | 0:04:08 | 0:04:10 | |
to gravitationally attract it, | 0:04:10 | 0:04:12 | |
it could slow to a halt and then collapse and come to an end. | 0:04:12 | 0:04:16 | |
Saul was measuring the way the universe was expanding | 0:04:16 | 0:04:19 | |
by observing exploding stars called supernovae. | 0:04:19 | 0:04:23 | |
One particular kind of supernova always explodes the same way | 0:04:27 | 0:04:30 | |
because it waits until just a critical amount of mass has fallen | 0:04:30 | 0:04:33 | |
on it and then it explodes, so they all look very similar to each other. | 0:04:33 | 0:04:38 | |
They brighten as a firework and fade away, and they reach the same | 0:04:38 | 0:04:42 | |
brightness and you can then use that as an indicator of how far away | 0:04:42 | 0:04:46 | |
it is, by just looking to see how bright it appears to you. | 0:04:46 | 0:04:49 | |
Because they explode with exactly the same intensity, | 0:04:53 | 0:04:57 | |
these supernovae are known as standard candles. | 0:04:57 | 0:05:01 | |
By comparing their relative brightnesses, | 0:05:01 | 0:05:03 | |
relative distances can be calculated. | 0:05:03 | 0:05:07 | |
Saul expected the stars to show what everyone thought | 0:05:07 | 0:05:10 | |
at the time - that the universe was slowing down. | 0:05:10 | 0:05:13 | |
Fainter ones are further | 0:05:14 | 0:05:16 | |
and just like when you watch a car recede into the distance, | 0:05:16 | 0:05:19 | |
you can tell how far away it is by how faint the tail-lights look. | 0:05:19 | 0:05:23 | |
If you can use the brightness of the supernova | 0:05:24 | 0:05:26 | |
to tell you how far away it is, | 0:05:26 | 0:05:28 | |
that's really telling you how long ago the explosion occurred | 0:05:28 | 0:05:30 | |
because you know how long it takes for light to travel | 0:05:30 | 0:05:33 | |
that great distance. | 0:05:33 | 0:05:35 | |
So, now we have an object where it explodes | 0:05:35 | 0:05:38 | |
and its brightness tells you when it exploded, | 0:05:38 | 0:05:41 | |
how far back in time it exploded. | 0:05:41 | 0:05:43 | |
No matter how good the theory, the practical problem of catching | 0:05:43 | 0:05:47 | |
an exploding star at just the right time is immense. | 0:05:47 | 0:05:52 | |
But Saul and his team applied the very latest computer technology | 0:05:52 | 0:05:56 | |
to the problem. | 0:05:56 | 0:05:58 | |
Yeah, we think it may be the scuzzy chain is too long. | 0:06:02 | 0:06:06 | |
Now there's two switches on the back of it. | 0:06:06 | 0:06:08 | |
We had the computers go down, the computers came back up again, | 0:06:10 | 0:06:13 | |
but now, finally, we have the analysis completed, | 0:06:13 | 0:06:15 | |
at least the computer's part of the analysis, and it's beginning | 0:06:15 | 0:06:18 | |
to show us on the screen what it thinks might be a supernova. | 0:06:18 | 0:06:22 | |
Eventually, after the team had identified 42 such dying stars, | 0:06:25 | 0:06:31 | |
the calculations began. | 0:06:31 | 0:06:32 | |
What Perlmutter discovered shocked him. | 0:06:34 | 0:06:36 | |
The data was telling the wrong story. | 0:06:38 | 0:06:40 | |
The universe didn't appear to be slowing down. | 0:06:41 | 0:06:44 | |
We thought that that's what we would see | 0:06:44 | 0:06:46 | |
and it looked like the opposite was taking place | 0:06:46 | 0:06:49 | |
and, in fact, the universe was speeding up in its expansion. | 0:06:49 | 0:06:53 | |
These distant supernovae were fainter than you would have thought | 0:06:53 | 0:06:58 | |
and fairly significantly fainter. | 0:06:58 | 0:07:00 | |
They were probably 20% or more | 0:07:00 | 0:07:04 | |
and that's the hallmark of a universe | 0:07:04 | 0:07:07 | |
that's actually speeding up in its expansion. | 0:07:07 | 0:07:09 | |
To say that this result was a surprise | 0:07:13 | 0:07:16 | |
would be a masterclass in understatement. | 0:07:16 | 0:07:19 | |
It was so unexpected that the initial reaction was disbelief. | 0:07:19 | 0:07:23 | |
Everybody knew Saul and everybody knew the experiment | 0:07:26 | 0:07:28 | |
he was doing and I remember sitting in the audience and Saul | 0:07:28 | 0:07:31 | |
getting up and expecting him to present an update on the results | 0:07:31 | 0:07:36 | |
he'd given a year ago, | 0:07:36 | 0:07:38 | |
that actually the universe was slowing down. | 0:07:38 | 0:07:41 | |
And so, I was absolutely amazed that, | 0:07:41 | 0:07:44 | |
based on only twice as many objects as he had the year before, | 0:07:44 | 0:07:49 | |
that suddenly he was saying | 0:07:49 | 0:07:51 | |
that we lived in a universe that was accelerating. | 0:07:51 | 0:07:54 | |
I remember it just being just incredible. | 0:07:54 | 0:07:57 | |
I mean, all the astronomers walking around scratching their heads | 0:07:57 | 0:08:00 | |
saying, "This can't be right. Surely it can't be right?" | 0:08:00 | 0:08:03 | |
It was not the result that people had been expecting | 0:08:05 | 0:08:08 | |
and such an extraordinary claim demands extraordinary evidence, | 0:08:08 | 0:08:13 | |
more than a few data from a handful of stars. | 0:08:13 | 0:08:16 | |
So, here we are on a beach where there is about a billion pebbles | 0:08:17 | 0:08:21 | |
and if you think you're trying to understand this beach, | 0:08:21 | 0:08:24 | |
you wouldn't think you could understand it from 42 pebbles. | 0:08:24 | 0:08:28 | |
But Saul was right. | 0:08:28 | 0:08:29 | |
He was able to work out that the universe was accelerating | 0:08:29 | 0:08:32 | |
just from 42 supernovae, | 0:08:32 | 0:08:34 | |
which is quite incredible when you think about it. | 0:08:34 | 0:08:37 | |
On the one hand, this was a good result. | 0:08:41 | 0:08:44 | |
It was new science and produced a Nobel prize for Saul Perlmutter. | 0:08:44 | 0:08:48 | |
On the other, it raised an obvious question. | 0:08:49 | 0:08:52 | |
Once you know that the universe is actually speeding up, | 0:08:55 | 0:08:58 | |
then you're faced with the question of - | 0:08:58 | 0:09:00 | |
well, what could make it speed up? | 0:09:00 | 0:09:02 | |
So far, the only real progress on that question has been | 0:09:04 | 0:09:08 | |
to give the phenomenon a name. | 0:09:08 | 0:09:11 | |
It's become known as dark energy. | 0:09:11 | 0:09:13 | |
Dark energy is just the term we use to describe whatever it is | 0:09:15 | 0:09:19 | |
that makes the universe accelerate in its expansion, | 0:09:19 | 0:09:22 | |
what makes it expand faster and faster. | 0:09:22 | 0:09:25 | |
We don't know what that is. | 0:09:25 | 0:09:27 | |
It's a mystery and so we call it dark to reflect our ignorance, | 0:09:27 | 0:09:30 | |
not because the colour is dark. | 0:09:30 | 0:09:33 | |
The mystery is so deep, so beguiling, | 0:09:37 | 0:09:40 | |
that wherever there are physicists, there are people hoping | 0:09:40 | 0:09:43 | |
that they will solve the mystery of dark energy. | 0:09:43 | 0:09:47 | |
People safe in the infuriating knowledge | 0:09:49 | 0:09:52 | |
that what they're looking for, if it's there at all, | 0:09:52 | 0:09:55 | |
is all around them. | 0:09:55 | 0:09:56 | |
But the fact that no-one has yet been able to identify | 0:09:58 | 0:10:01 | |
what the dark energy might actually be | 0:10:01 | 0:10:04 | |
has opened a can of worms not seen in science since the last time | 0:10:04 | 0:10:08 | |
a physicist got involved in cosmology. | 0:10:08 | 0:10:10 | |
In 1915, it seemed that the work of physics was nearly at an end. | 0:10:14 | 0:10:19 | |
Everything made sense. | 0:10:19 | 0:10:22 | |
Newton had explained the heavens by invoking gravity | 0:10:22 | 0:10:25 | |
and atoms had been identified as the smallest indivisible units | 0:10:25 | 0:10:29 | |
of matter. | 0:10:29 | 0:10:31 | |
Job done. | 0:10:31 | 0:10:32 | |
But then, a German man, given to musing on trains, | 0:10:37 | 0:10:41 | |
turned up with a totally new set of ideas. | 0:10:41 | 0:10:44 | |
I very rarely think in words at all. | 0:10:47 | 0:10:50 | |
A thought comes... | 0:10:50 | 0:10:51 | |
..and I might try to express it in words afterwards. | 0:10:55 | 0:10:58 | |
Einstein called these little flights of fancy | 0:11:00 | 0:11:04 | |
his "thought experiments" and they would lead him | 0:11:04 | 0:11:08 | |
to develop his theory of general relativity, | 0:11:08 | 0:11:11 | |
which totally changed how the workings of the universe | 0:11:11 | 0:11:14 | |
were understood. | 0:11:14 | 0:11:16 | |
I sometimes ask myself how did it come that | 0:11:16 | 0:11:18 | |
I was the one to develop the theory of relativity? | 0:11:18 | 0:11:22 | |
The reason, I think, is that a normal adult | 0:11:22 | 0:11:25 | |
never stops to think about problems of space and time. | 0:11:25 | 0:11:28 | |
These are things which he had thought of as a child. | 0:11:28 | 0:11:31 | |
But I began to wonder about space and time | 0:11:32 | 0:11:35 | |
only when I had already grown-up. | 0:11:35 | 0:11:37 | |
Einstein's theory held that Newton's ideas about gravity, | 0:11:40 | 0:11:44 | |
though empirically correct in most cases, | 0:11:44 | 0:11:47 | |
were, in fact, conceptually wrong. | 0:11:47 | 0:11:49 | |
Gravity, said Einstein, | 0:11:51 | 0:11:53 | |
was not some nebulous attracting property of mass as Newton supposed, | 0:11:53 | 0:11:58 | |
but was, in fact, a consequence of mass interacting with space-time - | 0:11:58 | 0:12:03 | |
the gaps around stars and planets previously known as space. | 0:12:03 | 0:12:07 | |
According to Einstein, space isn't simply a void. | 0:12:09 | 0:12:13 | |
It's more like a four-dimensional fabric | 0:12:13 | 0:12:16 | |
woven from both space and time. | 0:12:16 | 0:12:19 | |
The mass of planets can warp and distort the fabric, | 0:12:21 | 0:12:25 | |
gathering other celestial objects, like moons, around them. | 0:12:25 | 0:12:29 | |
And it's this bending of space-time that creates the effect | 0:12:30 | 0:12:35 | |
we experience as gravity. | 0:12:35 | 0:12:37 | |
So, Einstein's theory of general relativity | 0:12:38 | 0:12:40 | |
is a beautiful theory. | 0:12:40 | 0:12:42 | |
It's incredibly elegant and has been now around for 100 years. | 0:12:42 | 0:12:45 | |
It's very predictable. | 0:12:45 | 0:12:47 | |
You can write things, make predictions of what the universe | 0:12:47 | 0:12:49 | |
should look like and what objects should look like in the universe, | 0:12:49 | 0:12:52 | |
and we can test those, and as far as we can tell, it's passed every test. | 0:12:52 | 0:12:57 | |
The power of general relativity is that, like Newton's | 0:13:01 | 0:13:04 | |
version of gravity before it, | 0:13:04 | 0:13:06 | |
it's predictive. | 0:13:06 | 0:13:08 | |
Bizarre as the curvature of space-time may sound, | 0:13:08 | 0:13:11 | |
it's eminently testable - | 0:13:11 | 0:13:14 | |
a fact not lost on Einstein himself. | 0:13:14 | 0:13:18 | |
I have now come to realise that one of the most important consequences | 0:13:18 | 0:13:21 | |
of that analysis is accessible to experimental test. | 0:13:21 | 0:13:24 | |
Accordingly, a ray of light travelling past the sun would | 0:13:24 | 0:13:28 | |
undergo a deflection amounting to 0.83 seconds of arc. | 0:13:28 | 0:13:31 | |
In 1919, that prediction was actually observed. | 0:13:37 | 0:13:40 | |
British astronomer, Arthur Eddington, | 0:13:41 | 0:13:44 | |
pointed his telescope at a patch of sky near the sun | 0:13:44 | 0:13:47 | |
during an eclipse and observed a star, | 0:13:47 | 0:13:50 | |
known to be actually out of view, behind the sun. | 0:13:50 | 0:13:53 | |
Its rays of light had been bent by the distorted space-time | 0:13:54 | 0:13:59 | |
created by the sun's mass. | 0:13:59 | 0:14:01 | |
Einstein's theory had held up. | 0:14:02 | 0:14:05 | |
A paradigm had shifted and the crowd went wild. | 0:14:05 | 0:14:10 | |
Einstein was suddenly famous. | 0:14:11 | 0:14:14 | |
Undoubtedly the cleverest, yet most incomprehensible man on earth. | 0:14:14 | 0:14:19 | |
This strange world is a madhouse. | 0:14:20 | 0:14:22 | |
Currently, every coachman and every waiter is debating | 0:14:24 | 0:14:28 | |
whether relativity theory is correct. | 0:14:28 | 0:14:31 | |
This mass excitement about my theory is to do with the | 0:14:31 | 0:14:34 | |
intriguing mystery of incomprehensibility. | 0:14:34 | 0:14:37 | |
I'm certain that the mystery of not understanding | 0:14:39 | 0:14:42 | |
is what attracts people. | 0:14:42 | 0:14:43 | |
This is what all the fuss was about. | 0:14:46 | 0:14:49 | |
This is the equation that the coachmen and waiters | 0:14:49 | 0:14:52 | |
were discussing. | 0:14:52 | 0:14:53 | |
On the one side, the geometry of space-time. | 0:14:58 | 0:15:02 | |
On the other, the mass and energy of the universe which acts on it. | 0:15:02 | 0:15:06 | |
Not incomprehensible at all(!) | 0:15:06 | 0:15:09 | |
At least, not to its author. | 0:15:09 | 0:15:11 | |
But there was one aspect of general relativity that Einstein himself | 0:15:12 | 0:15:17 | |
didn't understand. | 0:15:17 | 0:15:19 | |
The problem that Einstein had is that | 0:15:23 | 0:15:26 | |
when he solved his equations of general relativity, | 0:15:26 | 0:15:30 | |
what he found was that he predicted that the universe should | 0:15:30 | 0:15:34 | |
actually be expanding. | 0:15:34 | 0:15:37 | |
And that was radically different from the perceived | 0:15:37 | 0:15:40 | |
wisdom at the time, | 0:15:40 | 0:15:41 | |
which was that we lived in a static universe, both static in time | 0:15:41 | 0:15:45 | |
and in space. | 0:15:45 | 0:15:46 | |
So, he put in an extra term into the equation. | 0:15:48 | 0:15:52 | |
He called it the cosmological constant. | 0:15:52 | 0:15:55 | |
He used the Greek variable lambda, but, effectively, it was just | 0:15:55 | 0:15:59 | |
what a physics undergraduate would call a fudge factor. | 0:15:59 | 0:16:02 | |
It was just designed to make the equations come out right | 0:16:02 | 0:16:05 | |
and it would just make the universe sort of stand still. | 0:16:05 | 0:16:10 | |
The problem is is in science, we'd call that fine tuning. | 0:16:10 | 0:16:13 | |
And you only have to change the value of the constant | 0:16:13 | 0:16:16 | |
by a small amount and suddenly, you get back these expanding solutions. | 0:16:16 | 0:16:21 | |
The general theory of relativity requires the universe to be | 0:16:22 | 0:16:25 | |
spatially finite, | 0:16:25 | 0:16:27 | |
but this view of the universe necessitated | 0:16:27 | 0:16:30 | |
an expansion of equations with the introduction of a new | 0:16:30 | 0:16:34 | |
universal constant lambda standing in fixed relation to the | 0:16:34 | 0:16:37 | |
total mass of the universe. | 0:16:37 | 0:16:39 | |
This is gravely detrimental to the formal beauty of my theory. | 0:16:39 | 0:16:43 | |
When you add the lambda term, | 0:16:48 | 0:16:51 | |
it means that the equation is not quite as simple as it was before. | 0:16:51 | 0:16:55 | |
So, in that sense, it's not as beautiful as an equation. | 0:16:55 | 0:16:58 | |
The static universe was restored, | 0:17:01 | 0:17:04 | |
but Einstein always felt he'd added lambda against his better judgment. | 0:17:04 | 0:17:09 | |
Dear Egrenfest, | 0:17:15 | 0:17:18 | |
I have perpetrated something in gravitation theory which | 0:17:18 | 0:17:21 | |
exposes me a bit to the danger of being committed to a madhouse. | 0:17:21 | 0:17:25 | |
Despite the fudge factor, lambda, the cosmological constant, | 0:17:30 | 0:17:35 | |
Einstein continued to be celebrated as the world's cleverest man. | 0:17:35 | 0:17:40 | |
Until, in 1929, he became even cleverer. | 0:17:40 | 0:17:44 | |
In America, astronomer Edwin Hubble was about to get | 0:17:49 | 0:17:52 | |
a reputation for scientific cleverness himself. | 0:17:52 | 0:17:56 | |
He'd been using the world's largest telescope at Mount Wilson in | 0:17:56 | 0:18:00 | |
California to peer deeper into space than anyone had ever looked before. | 0:18:00 | 0:18:05 | |
What he discovered completely changed the meaning of the word | 0:18:08 | 0:18:12 | |
"universe". | 0:18:12 | 0:18:15 | |
Until Hubble, it had been thought that the universe was our galaxy. | 0:18:15 | 0:18:20 | |
What Hubble saw was that in fact our galaxy is just one of countless | 0:18:20 | 0:18:25 | |
millions, but more importantly, | 0:18:25 | 0:18:28 | |
that all these galaxies were moving apart from each other. | 0:18:28 | 0:18:33 | |
The universe wasn't static after all. | 0:18:33 | 0:18:36 | |
This had huge implications. | 0:18:36 | 0:18:39 | |
It introduced the notion of a beginning | 0:18:39 | 0:18:42 | |
and an age for the universe. | 0:18:42 | 0:18:45 | |
But more importantly for Einstein, | 0:18:45 | 0:18:48 | |
it meant that he could ditch his fudge factor, the cosmological | 0:18:48 | 0:18:52 | |
constant, and return general relativity to its former glory. | 0:18:52 | 0:18:57 | |
The lambda that he added to create a static universe | 0:18:57 | 0:19:01 | |
was no longer required, | 0:19:01 | 0:19:03 | |
once it was observed by Slipher and Hubble | 0:19:03 | 0:19:07 | |
that the universe, in fact, was expanding, | 0:19:07 | 0:19:11 | |
so if, in an expanding universe, | 0:19:11 | 0:19:14 | |
at the time, the observations could be described | 0:19:14 | 0:19:18 | |
without the lambda term and so he removed it. | 0:19:18 | 0:19:22 | |
Einstein was cock-a-hoop. | 0:19:25 | 0:19:28 | |
In 1931, he went to Mount Wilson to shake Hubble's hand | 0:19:28 | 0:19:32 | |
and thank him for putting beauty back into his equation. | 0:19:32 | 0:19:35 | |
Lambda, he later confessed, was the biggest blunder in his career. | 0:19:35 | 0:19:41 | |
I think that the reason that he said that it was a blunder was | 0:19:43 | 0:19:49 | |
because if he had just not introduced that term, | 0:19:49 | 0:19:53 | |
then he would have said that the universe must be expanding | 0:19:53 | 0:19:58 | |
and done that 14 years before the discovery of the expansion of | 0:19:58 | 0:20:03 | |
the universe by Edwin Hubble, which would have been a great achievement. | 0:20:03 | 0:20:08 | |
But despite Einstein's blunder, | 0:20:08 | 0:20:11 | |
general relativity has stood the test of time. | 0:20:11 | 0:20:14 | |
It is perhaps the single most successful scientific theory yet. | 0:20:14 | 0:20:19 | |
Every observation we make of gravity, from the smaller scales | 0:20:19 | 0:20:26 | |
to solar system scales to galactic scales, | 0:20:26 | 0:20:30 | |
all the way to the universe, all of that can be described using | 0:20:30 | 0:20:34 | |
the single theory that Einstein created. | 0:20:34 | 0:20:37 | |
So, it's the most successful | 0:20:37 | 0:20:40 | |
and beautiful theory we have of our universe. | 0:20:40 | 0:20:45 | |
Or at least, it was. | 0:20:45 | 0:20:47 | |
For all its beauty and simplicity, | 0:20:47 | 0:20:51 | |
general relativity doesn't account for the effects of dark energy. | 0:20:51 | 0:20:55 | |
Expansion, as reported by Hubble, works fine, | 0:20:55 | 0:20:59 | |
but the accelerated expansion of the universe | 0:20:59 | 0:21:02 | |
that Saul Perlmutter found isn't part of the deal. | 0:21:02 | 0:21:05 | |
That it's there at all is bad enough, but worse still, the way | 0:21:08 | 0:21:12 | |
that dark energy seems to work is unlike anything that's been | 0:21:12 | 0:21:16 | |
observed before. | 0:21:16 | 0:21:18 | |
The density of anything is the amount of stuff you have | 0:21:18 | 0:21:23 | |
within a given volume | 0:21:23 | 0:21:24 | |
and dark energy is an unusual phenomenon, | 0:21:24 | 0:21:27 | |
in that even though the volume of the universe is increasing | 0:21:27 | 0:21:31 | |
as it expands, the density is staying the same, constant. | 0:21:31 | 0:21:37 | |
So, imagine you had say like half a cup of black coffee, | 0:21:37 | 0:21:40 | |
and then you started adding milk to it, | 0:21:40 | 0:21:44 | |
and as we pour more and more milk into that cup, | 0:21:44 | 0:21:48 | |
then the volume of the liquid's getting larger and larger, | 0:21:48 | 0:21:52 | |
but the density of the coffee is going down, so the coffee | 0:21:52 | 0:21:55 | |
would be getting lighter and lighter as you added more and more milk. | 0:21:55 | 0:21:59 | |
But dark energy doesn't behave that way, | 0:21:59 | 0:22:02 | |
so it's almost as if there's new dark energy being created | 0:22:02 | 0:22:05 | |
all the time, as the universe expands, | 0:22:05 | 0:22:08 | |
meaning that its density remains the same. Constant. | 0:22:08 | 0:22:13 | |
So, you can think of it, as you get more space, | 0:22:13 | 0:22:16 | |
you actually get more dark energy, which is | 0:22:16 | 0:22:19 | |
like getting something for nothing, which is clearly ridiculous. | 0:22:19 | 0:22:22 | |
It's clearly against all our training as physicists. | 0:22:22 | 0:22:27 | |
There is one way to adapt general relativity to cope with this | 0:22:30 | 0:22:34 | |
magically constantly self-replenishing force | 0:22:34 | 0:22:37 | |
and that is to simply add it to the equation. | 0:22:37 | 0:22:41 | |
100 years after Einstein's "biggest blunder", | 0:22:41 | 0:22:45 | |
the cosmological constant is back. | 0:22:45 | 0:22:48 | |
Lambda is being written once more. | 0:22:48 | 0:22:51 | |
This time, not to keep the universe still, | 0:22:51 | 0:22:55 | |
but to account for its unexplained accelerating expansion. | 0:22:55 | 0:22:59 | |
The values are different, but the concept is exactly the same. | 0:22:59 | 0:23:04 | |
All this leads cosmologists | 0:23:04 | 0:23:07 | |
to one of two equally alarming conclusions - | 0:23:07 | 0:23:11 | |
either we need another Hubble, | 0:23:11 | 0:23:13 | |
or we need another Einstein. | 0:23:13 | 0:23:16 | |
But before we consign Albert to the scientific scrapheap, | 0:23:16 | 0:23:20 | |
there is a branch of physics which might help. | 0:23:20 | 0:23:23 | |
An area where things popping in and out of existence is quite normal. | 0:23:23 | 0:23:27 | |
This is the strange and wonderful world of Clare Burrage | 0:23:33 | 0:23:38 | |
and of quantum mechanics. | 0:23:38 | 0:23:40 | |
Quantum mechanics is the theory of what happens to really, | 0:23:40 | 0:23:44 | |
really small things. | 0:23:44 | 0:23:45 | |
It's a theory of how the fundamental particles in the universe work. | 0:23:45 | 0:23:49 | |
Atoms, electrons, protons. | 0:23:49 | 0:23:52 | |
And quantum mechanics is intrinsically uncertain. | 0:23:53 | 0:23:58 | |
Einstein hated quantum mechanics. | 0:23:59 | 0:24:03 | |
He disliked the probabilistic | 0:24:03 | 0:24:04 | |
"now you see it, now you don't" nature of the idea. | 0:24:04 | 0:24:08 | |
"God," he famously declared, "does not play dice." | 0:24:08 | 0:24:12 | |
In 1930, he paid a visit to Nottingham, | 0:24:12 | 0:24:15 | |
where Clare now does her research. He didn't say much. | 0:24:15 | 0:24:18 | |
He probably didn't say anything about quantum mechanics. | 0:24:23 | 0:24:26 | |
He came to give a talk on general relativity. | 0:24:26 | 0:24:30 | |
His actual chalk writing is preserved for devotees to marvel at. | 0:24:30 | 0:24:35 | |
But even though Einstein didn't like it, | 0:24:35 | 0:24:38 | |
quantum mechanics could shed light on dark energy | 0:24:38 | 0:24:42 | |
and come to the aid of his once-more-under-fire theory. | 0:24:42 | 0:24:46 | |
In theory. | 0:24:46 | 0:24:48 | |
Quantum mechanics tells us | 0:24:50 | 0:24:52 | |
that particles can come in and out of existence in the vacuum. | 0:24:52 | 0:24:55 | |
And the fact that those particles have mass | 0:24:55 | 0:24:58 | |
and potentially are moving around, they have a little bit of energy. | 0:24:58 | 0:25:02 | |
And so, when they pop into existence, | 0:25:02 | 0:25:06 | |
they give a little bit of energy to the vacuum and yes, | 0:25:06 | 0:25:08 | |
they disappear again, but the fact that that process is going | 0:25:08 | 0:25:12 | |
on all of the time means that there is some energy stored in the vacuum. | 0:25:12 | 0:25:16 | |
And because Einstein told us that energy | 0:25:16 | 0:25:18 | |
and mass are the same thing, | 0:25:18 | 0:25:20 | |
having lots of energy stored in space affects space-time | 0:25:20 | 0:25:23 | |
that cause the expansion of the universe to accelerate. | 0:25:23 | 0:25:28 | |
So, it seems that quantum mechanics should, in theory, | 0:25:28 | 0:25:32 | |
be able to explain how the cosmological constant works. | 0:25:32 | 0:25:36 | |
And how dark energy appears in the vacuum of space | 0:25:36 | 0:25:40 | |
and is driving the acceleration of the universe. | 0:25:40 | 0:25:44 | |
But there's a problem. | 0:25:44 | 0:25:47 | |
When they came to calculate this vacuum energy, | 0:25:47 | 0:25:50 | |
they discovered how spectacularly wrong they were. | 0:25:50 | 0:25:54 | |
If you were to say there was one pebble on this beach, | 0:25:54 | 0:25:57 | |
you'd be wrong by one part in a billion. | 0:25:57 | 0:26:00 | |
If you were to say there was one particle in the universe, | 0:26:00 | 0:26:04 | |
you'd be off by ten to the 80. | 0:26:04 | 0:26:07 | |
But the vacuum energy was calculated to be off by ten to the 120. | 0:26:07 | 0:26:13 | |
That is a google. | 0:26:13 | 0:26:15 | |
That is spectacularly wrong. | 0:26:15 | 0:26:18 | |
The fact that our predictions are so far off from what we see | 0:26:21 | 0:26:24 | |
tells us that there's something fundamentally missing | 0:26:24 | 0:26:27 | |
in the way that we understand physics, that we understand | 0:26:27 | 0:26:31 | |
the world around us, so there's still a mystery, | 0:26:31 | 0:26:34 | |
still a puzzle there. | 0:26:34 | 0:26:35 | |
It might be tempting to simply ignore dark energy. | 0:26:35 | 0:26:39 | |
You could argue that the apparent accelerated expansion | 0:26:39 | 0:26:43 | |
is, in fact, a trick of the light, that it | 0:26:43 | 0:26:45 | |
may be a function of other inaccessible dimensions at play. | 0:26:45 | 0:26:50 | |
That it just looks like dark energy, but is actually...something else. | 0:26:50 | 0:26:56 | |
But dark energy isn't just an irritating threat | 0:26:56 | 0:27:00 | |
to Einstein's beautiful equations. | 0:27:00 | 0:27:03 | |
It's also a very practical solution to a fundamental | 0:27:03 | 0:27:06 | |
question in cosmology, namely - what is the universe made of? | 0:27:06 | 0:27:12 | |
When Einstein was busy thinking about gravity on trains, | 0:27:12 | 0:27:16 | |
the answer was simple. | 0:27:16 | 0:27:18 | |
The universe was made of the same stuff that you | 0:27:18 | 0:27:21 | |
and I are made of, the stuff of stars, planets, Coke cans, | 0:27:21 | 0:27:26 | |
tennis rackets, atoms, | 0:27:26 | 0:27:28 | |
made, in turn, from electrons, protons and neutrons. | 0:27:28 | 0:27:33 | |
But physics was about to get a shock. | 0:27:33 | 0:27:37 | |
It turned out that there was something else out there | 0:27:37 | 0:27:41 | |
that the universe was also made of, | 0:27:41 | 0:27:45 | |
matter of a different kind. | 0:27:45 | 0:27:47 | |
In 1975, an astronomer called Vera Rubin made an unexpected discovery. | 0:27:47 | 0:27:52 | |
If we plot | 0:27:54 | 0:27:56 | |
the velocity of the planets as a function of distance from the sun, | 0:27:56 | 0:28:02 | |
Mercury, Venus, Earth, Mars, | 0:28:02 | 0:28:07 | |
Jupiter, Saturn, Uranus, Neptune, Pluto, | 0:28:07 | 0:28:13 | |
and you can see that Mercury orbits much more rapidly | 0:28:13 | 0:28:18 | |
than Pluto. | 0:28:18 | 0:28:21 | |
The graph is called a rotation curve. | 0:28:23 | 0:28:26 | |
It is the embodiment of the law of gravity. | 0:28:26 | 0:28:29 | |
The further away you travel from the sun, | 0:28:29 | 0:28:31 | |
the weaker its gravitational force. | 0:28:31 | 0:28:34 | |
Galaxies work in the same way as our solar system. | 0:28:34 | 0:28:39 | |
Except that instead of planets orbiting a central sun, | 0:28:39 | 0:28:43 | |
in a spiral galaxy, | 0:28:43 | 0:28:45 | |
stars are held in orbit by a gravity-providing black hole. | 0:28:45 | 0:28:49 | |
Vera decided to plot the rotation curves in galaxies. | 0:28:50 | 0:28:55 | |
She trained her telescopes on Andromeda, | 0:28:55 | 0:28:58 | |
the galaxy closest to our own. | 0:28:58 | 0:29:01 | |
I came out with sets of numbers | 0:29:01 | 0:29:03 | |
and I plotted them on pieces of paper and | 0:29:03 | 0:29:05 | |
I discovered that the stars as you went further and further out | 0:29:05 | 0:29:09 | |
did not slow down, | 0:29:09 | 0:29:10 | |
they were moving just as fast as the stars near the centre. | 0:29:10 | 0:29:14 | |
We find that the velocities remain flat all the way to the | 0:29:16 | 0:29:21 | |
edge of our observations. | 0:29:21 | 0:29:23 | |
And that was a surprise. | 0:29:23 | 0:29:26 | |
And a surprise that had to be explained. | 0:29:26 | 0:29:28 | |
By rights, the stars should have flown off into space, | 0:29:29 | 0:29:33 | |
but they didn't and wherever spiral galaxies were measured, | 0:29:33 | 0:29:37 | |
the same flat curves appeared. | 0:29:37 | 0:29:40 | |
It was decided that the only explanation | 0:29:40 | 0:29:43 | |
was that there must be more stuff out there that we couldn't see, | 0:29:43 | 0:29:46 | |
providing the extra gravity, | 0:29:46 | 0:29:49 | |
holding the galaxies together | 0:29:49 | 0:29:51 | |
and flattening the curves. | 0:29:51 | 0:29:53 | |
They called this stuff | 0:29:58 | 0:30:01 | |
dark matter. | 0:30:01 | 0:30:02 | |
The new dark matter was a shock, in more ways than one. | 0:30:08 | 0:30:12 | |
The very fact of its existence was almost overshadowed | 0:30:12 | 0:30:16 | |
by the fact that when the calculations were made, this new | 0:30:16 | 0:30:20 | |
form of matter outweighed the atomic form of stuff by about 90 to one. | 0:30:20 | 0:30:26 | |
In the 1980s, | 0:30:28 | 0:30:30 | |
when new ways of measuring dark matter were developed, | 0:30:30 | 0:30:34 | |
it was discovered that there simply wasn't enough of it | 0:30:34 | 0:30:37 | |
to make the universe work as it clearly does. | 0:30:37 | 0:30:41 | |
The universe was short of stuff | 0:30:41 | 0:30:44 | |
to the tune of about 70%. | 0:30:44 | 0:30:47 | |
Cosmology scratched its head. | 0:30:48 | 0:30:50 | |
Then, in 1998, | 0:30:51 | 0:30:53 | |
a young scientist called Saul Perlmutter | 0:30:53 | 0:30:57 | |
was thinking some very big thoughts indeed. | 0:30:57 | 0:31:00 | |
Something that felt like it was | 0:31:00 | 0:31:02 | |
meaningful about the world we live in, in some deep way. | 0:31:02 | 0:31:07 | |
The universe was speeding up in its expansion. | 0:31:07 | 0:31:10 | |
The dark energy that earned Saul his Nobel Prize was an interesting | 0:31:10 | 0:31:14 | |
and troubling concept, | 0:31:14 | 0:31:16 | |
but it also had a number | 0:31:16 | 0:31:18 | |
and that number was highly significant. | 0:31:18 | 0:31:22 | |
We know from Einstein - him again - | 0:31:22 | 0:31:24 | |
that energy and mass are related, | 0:31:24 | 0:31:27 | |
that energy, E, equals mass times the speed of light squared. | 0:31:27 | 0:31:31 | |
E = MC2. | 0:31:31 | 0:31:34 | |
Plug dark energy into that equation and you get the missing mass | 0:31:35 | 0:31:39 | |
that dark matter couldn't account for. | 0:31:39 | 0:31:42 | |
The universe was complete. | 0:31:45 | 0:31:48 | |
It was made about 4% baryonic matter, | 0:31:48 | 0:31:51 | |
the stuff that we're made from, | 0:31:51 | 0:31:54 | |
25% dark matter | 0:31:54 | 0:31:55 | |
and the gaping 70%-sized hole was filled with dark energy. | 0:31:55 | 0:32:00 | |
So far, despite heroic efforts to find it, and overwhelming | 0:32:09 | 0:32:14 | |
evidence that it exists, no-one has identified what dark matter is. | 0:32:14 | 0:32:18 | |
And, of course, dark energy, both useful and confounding, | 0:32:24 | 0:32:28 | |
is barely in its infancy when it comes to a convincing explanation. | 0:32:28 | 0:32:32 | |
There's radiation damage. | 0:32:32 | 0:32:35 | |
We may not be quite there with the shielding yet to provide | 0:32:35 | 0:32:40 | |
the right radiation environment. | 0:32:40 | 0:32:42 | |
But there is an idea in cosmology that dark matter | 0:32:42 | 0:32:47 | |
and dark energy may be linked by more than just a common | 0:32:47 | 0:32:50 | |
adjective and if they are, a new European spacecraft called | 0:32:50 | 0:32:55 | |
Euclid may shed light on what that link might be. | 0:32:55 | 0:32:59 | |
The Euclid Consortium is staffed by 1,200 scientists from 14 countries. | 0:33:00 | 0:33:06 | |
These are some of them | 0:33:06 | 0:33:08 | |
having their picture taken at their annual conference in Lausanne. | 0:33:08 | 0:33:12 | |
They're hoping that by taking pictures of the universe, | 0:33:14 | 0:33:17 | |
they'll be able to work out how it's expanded over its lifetime and | 0:33:17 | 0:33:22 | |
that by determining that, the nature of dark energy will become clearer. | 0:33:22 | 0:33:26 | |
The way we think about it is that it's either some new | 0:33:28 | 0:33:32 | |
stuff in the universe, | 0:33:32 | 0:33:34 | |
some particle or even just a new field that you | 0:33:34 | 0:33:39 | |
put in to the universe to explain the properties of the universe. | 0:33:39 | 0:33:43 | |
Alternatively, you could say that the equation you wrote down | 0:33:45 | 0:33:49 | |
is not correct. It's not wrong, | 0:33:49 | 0:33:52 | |
but we like to say it's "incomplete". | 0:33:52 | 0:33:54 | |
So, you could sort of fiddle with the mathematics of the equation, | 0:33:54 | 0:33:58 | |
so actually what you could do is maybe come up with a natural | 0:33:58 | 0:34:01 | |
explanation for it. | 0:34:01 | 0:34:04 | |
So, Euclid should be able to tell us which of those alternatives it is. | 0:34:04 | 0:34:09 | |
The satellite will launch and start sending data back to Earth in 2020. | 0:34:10 | 0:34:15 | |
The all-important camera for the Euclid space telescope is being | 0:34:19 | 0:34:23 | |
built and tested in the UK, in this country house in the Surrey Hills. | 0:34:23 | 0:34:28 | |
These are going to be the biggest images that come down from in orbit. | 0:34:34 | 0:34:39 | |
You have an image of 625 megapixels, | 0:34:39 | 0:34:43 | |
so that's roughly 300 HD | 0:34:43 | 0:34:46 | |
television screens full of data and that comes down every ten minutes. | 0:34:46 | 0:34:50 | |
This imager takes roughly the same amount of data that Hubble | 0:34:51 | 0:34:55 | |
has taken and will take in its entire lifetime in one day. | 0:34:55 | 0:34:58 | |
It's an astonishing leap forward, | 0:35:03 | 0:35:05 | |
given what's available from current space telescopes. | 0:35:05 | 0:35:09 | |
The huge data sets will provide information from the universe | 0:35:09 | 0:35:12 | |
in almost every direction. | 0:35:12 | 0:35:14 | |
The Hubble space telescope is the biggest | 0:35:16 | 0:35:19 | |
and best telescope we have available at the moment | 0:35:19 | 0:35:22 | |
and the amount of sky that's covered is about the size | 0:35:22 | 0:35:25 | |
of your little fingernail, if you held it up at arm's length. | 0:35:25 | 0:35:28 | |
And Euclid will do the same type of imaging as the Hubble space | 0:35:28 | 0:35:32 | |
telescope, but instead of just covering that small patch | 0:35:32 | 0:35:35 | |
of sky, it will cover practically every bit of sky that you can see. | 0:35:35 | 0:35:40 | |
Not only will Euclid be able to measure the historic | 0:35:41 | 0:35:45 | |
acceleration of stars and galaxies in all directions, | 0:35:45 | 0:35:49 | |
it's hoped it will also provide data about how dark matter | 0:35:49 | 0:35:52 | |
around galaxies has expanded over time. | 0:35:52 | 0:35:56 | |
This is possible because of an effect called gravitational lensing. | 0:35:56 | 0:36:02 | |
So, in general relativity, mass bends space and time | 0:36:02 | 0:36:08 | |
and then light is bent around large massive objects, | 0:36:08 | 0:36:12 | |
just like Eddington measuring the star behind the Sun, | 0:36:12 | 0:36:15 | |
and so, we used the same technique for Euclid. | 0:36:15 | 0:36:18 | |
I can illustrate it using this wine glass | 0:36:18 | 0:36:20 | |
and this image of the universe, | 0:36:20 | 0:36:22 | |
so as we draw the wine glass across the image, | 0:36:22 | 0:36:27 | |
what you see is that the galaxies behind the wine glass | 0:36:27 | 0:36:32 | |
get distorted and that distortion is caused by the lens. | 0:36:32 | 0:36:37 | |
In general relativity, the lens is mass, because it bends the light. | 0:36:37 | 0:36:42 | |
And that can be shown in this picture. | 0:36:42 | 0:36:45 | |
You have a large clump of mass here, which is like the lens, | 0:36:45 | 0:36:49 | |
like the bottom of the wine glass, | 0:36:49 | 0:36:51 | |
and what you can see are all the distorted galaxies behind that lens. | 0:36:51 | 0:36:56 | |
And what you could do with an image like this is you can | 0:36:56 | 0:36:59 | |
calculate how much mass would I need within the lens to create | 0:36:59 | 0:37:04 | |
the distortions that I see and what you find is quite remarkable. | 0:37:04 | 0:37:07 | |
What you find is that there is about 100 times more mass here | 0:37:07 | 0:37:12 | |
than you see from the light in the image and that missing mass, | 0:37:12 | 0:37:16 | |
that mass you cannot see, is what we call dark matter. | 0:37:16 | 0:37:20 | |
So, Euclid will make an image of the whole sky at this resolution | 0:37:23 | 0:37:28 | |
and it will find all these distorted background galaxies | 0:37:28 | 0:37:33 | |
and from that, it can infer | 0:37:33 | 0:37:35 | |
the distribution of dark matter in the universe. | 0:37:35 | 0:37:38 | |
Euclid will compare lensing all over the universe and by doing so, | 0:37:38 | 0:37:44 | |
will help paint an accurate picture of how the universe is | 0:37:44 | 0:37:47 | |
tearing itself apart under the influence of dark energy. | 0:37:47 | 0:37:51 | |
So, Euclid may tell us that it's the cosmological constant | 0:37:51 | 0:37:57 | |
and then we have to explain that, | 0:37:57 | 0:38:00 | |
it might tell us that our theory | 0:38:00 | 0:38:04 | |
of gravity is not complete, | 0:38:04 | 0:38:08 | |
and we'd have to explain that, | 0:38:08 | 0:38:11 | |
it could tell us that actually the dark matter | 0:38:11 | 0:38:14 | |
and dark energy are two sides of the same coin and that actually there | 0:38:14 | 0:38:20 | |
might be a unified dark sector, but we'd have to explain that. | 0:38:20 | 0:38:24 | |
It could be another theory that we haven't even come up with yet. | 0:38:24 | 0:38:30 | |
And so Euclid will give us | 0:38:30 | 0:38:32 | |
a coherent data set that we can test all these theories against. | 0:38:32 | 0:38:36 | |
Whatever the case, the devil's in the detail, and these days, | 0:38:39 | 0:38:43 | |
the detail can be interrogated to degrees not thought possible | 0:38:43 | 0:38:47 | |
when Einstein first reluctantly inserted his cosmological | 0:38:47 | 0:38:51 | |
constant into general relativity. | 0:38:51 | 0:38:55 | |
Cosmology is one of the fields that is actually pushing | 0:38:55 | 0:38:59 | |
the boundaries of cosmology itself, but also statistics and computing. | 0:38:59 | 0:39:04 | |
It is the frontier, I think. | 0:39:04 | 0:39:07 | |
Euclid will be pushing the boundaries like never before. | 0:39:07 | 0:39:10 | |
It will stream more data from space than has ever been | 0:39:10 | 0:39:14 | |
processed in the past. | 0:39:14 | 0:39:15 | |
In the end, it will have about one and a half billion galaxies. | 0:39:15 | 0:39:19 | |
It will observe one and a half billion galaxies, so it's huge. | 0:39:19 | 0:39:23 | |
And a lot of the time, your eyes cannot just pick up patterns, | 0:39:23 | 0:39:27 | |
so this cannot be possible without computers and statistics. | 0:39:27 | 0:39:31 | |
The computer-aided searches should give unprecedented clarity | 0:39:31 | 0:39:35 | |
on how science should be thinking about dark energy. | 0:39:35 | 0:39:39 | |
There will be winners and losers. | 0:39:39 | 0:39:42 | |
The amount of data that we have on dark energy hasn't been enough | 0:39:42 | 0:39:46 | |
to be able to tell us which path we have to go down, | 0:39:46 | 0:39:49 | |
so we have lots of theories | 0:39:49 | 0:39:51 | |
and hundreds of models that could still fit our data. | 0:39:51 | 0:39:55 | |
When Euclid comes, lots of these can be thrown away and it could | 0:39:55 | 0:39:59 | |
narrow down the possibilities of what this dark energy is. | 0:39:59 | 0:40:02 | |
Euclid is not the only show in town | 0:40:12 | 0:40:14 | |
when it comes to mapping the expansion of the universe. | 0:40:14 | 0:40:18 | |
At Kit Peak in Arizona, Risa Wechsler is hoping to use | 0:40:19 | 0:40:24 | |
the proposed dark energy spectroscopic instrument, | 0:40:24 | 0:40:27 | |
DESI, to make a map of part of the universe, like this one. | 0:40:27 | 0:40:31 | |
But 100 times more accurate, | 0:40:35 | 0:40:38 | |
so that she can check the validity of computer | 0:40:38 | 0:40:41 | |
simulations of the universe that she's created. | 0:40:41 | 0:40:44 | |
One of the things that I do is try to simulate the entire universe | 0:40:46 | 0:40:51 | |
and tie what we think about the physics of the evolving | 0:40:51 | 0:40:55 | |
universe to what we actually see with surveys like DESI. | 0:40:55 | 0:40:58 | |
What we're trying to do in these simulations is take a whole | 0:41:01 | 0:41:05 | |
bunch of hypothetical universes, some of them | 0:41:05 | 0:41:07 | |
will have a cosmological constant, some of them | 0:41:07 | 0:41:11 | |
will have a different time evolving dark energy, some of them | 0:41:11 | 0:41:14 | |
will have more or less amount of dark matter, | 0:41:14 | 0:41:16 | |
and then when we compare that to what we actually see, | 0:41:16 | 0:41:20 | |
we can rule out a lot of these ideas, | 0:41:20 | 0:41:23 | |
so some of them will not be consistent with what we measure | 0:41:23 | 0:41:26 | |
and then we can determine that that's not the universe we live in. | 0:41:26 | 0:41:30 | |
When DESI starts producing data in 2020, | 0:41:30 | 0:41:34 | |
it might be that one of Risa's simulations strikes gold. | 0:41:34 | 0:41:38 | |
It'll be up against a lot of competition. | 0:41:38 | 0:41:42 | |
In the absence of hard data, this is boom time for theories. | 0:41:42 | 0:41:47 | |
Multi-Galileons, ghost condensates, | 0:41:47 | 0:41:50 | |
and the higher co-dimensional brane worlds theory | 0:41:50 | 0:41:53 | |
jostle for attention in the race to explain dark energy. | 0:41:53 | 0:41:58 | |
Many of these theories usually try to provide a global solution | 0:41:58 | 0:42:03 | |
to the dark energy problem, a fix to general relativity, | 0:42:03 | 0:42:08 | |
but Clare Burrage is working on an idea | 0:42:08 | 0:42:10 | |
that says that Einstein may have been both | 0:42:10 | 0:42:13 | |
right and wrong at the same time, | 0:42:13 | 0:42:16 | |
depending on where you are. | 0:42:16 | 0:42:19 | |
We know that Einstein's theory works very well on Earth | 0:42:19 | 0:42:23 | |
and in the solar system. | 0:42:23 | 0:42:24 | |
We've tested it and it works phenomenally well. | 0:42:24 | 0:42:27 | |
But we don't have ways of testing that theory on the kinds | 0:42:27 | 0:42:30 | |
of distance scales that are relevant to cosmology | 0:42:30 | 0:42:34 | |
and so it could be that whilst relativity is a good description | 0:42:34 | 0:42:37 | |
of what's happening around us, it doesn't work as a description of | 0:42:37 | 0:42:42 | |
the universe as a whole system and maybe you need to change the theory. | 0:42:42 | 0:42:46 | |
Clare's solution involves something called a chameleon, | 0:42:48 | 0:42:54 | |
a particle that tries to blend in not by changing colour, | 0:42:54 | 0:42:57 | |
but by changing how it exerts its force. | 0:42:57 | 0:43:00 | |
There are two types of particles in the universe. | 0:43:02 | 0:43:04 | |
There are the ones that make up matter, like electrons and protons | 0:43:04 | 0:43:08 | |
and neutrons and quarks, and then there's another set | 0:43:08 | 0:43:11 | |
of particles, and those are the ones that transmit forces. | 0:43:11 | 0:43:13 | |
So, for example, the photon, which makes up light, | 0:43:13 | 0:43:16 | |
also carries the electro-magnetic forces. | 0:43:16 | 0:43:19 | |
It's exactly like what we're doing with the ball and the magnet. | 0:43:20 | 0:43:23 | |
We don't see the photons transmitting the force directly | 0:43:23 | 0:43:26 | |
but we see the fact that the magnet makes the ball move. | 0:43:26 | 0:43:29 | |
In physics, the greater a particle's mass, the smaller the distance | 0:43:29 | 0:43:33 | |
over which it's able to exert any force or field it might have. | 0:43:33 | 0:43:38 | |
The mass of a particle tells you how far it can carry information. | 0:43:38 | 0:43:43 | |
If a particle that's transmitting a force is heavier, | 0:43:43 | 0:43:45 | |
it only transmits the force over a shorter distance scale. | 0:43:45 | 0:43:48 | |
So the range that you can transmit the force over changes | 0:43:48 | 0:43:51 | |
depending on where you're looking. | 0:43:51 | 0:43:53 | |
The idea is that when the chameleon comes into contact with other stuff, | 0:43:55 | 0:43:59 | |
it interacts with it and becomes heavy | 0:43:59 | 0:44:02 | |
and its force-transmitting capability all but disappears. | 0:44:02 | 0:44:07 | |
But in regions of deep space where there's very little in the way | 0:44:07 | 0:44:11 | |
of anything, the chameleon has no stuff with which to interact and | 0:44:11 | 0:44:15 | |
so is very light and can transmit its force over vast distances. | 0:44:15 | 0:44:21 | |
It's a neat idea, but evidence is hard to come by. | 0:44:21 | 0:44:26 | |
Then, in 2014, Clare came up with an experiment | 0:44:26 | 0:44:31 | |
that might unmask the chameleon. | 0:44:31 | 0:44:35 | |
The experiment that we proposed last year is that you'd | 0:44:35 | 0:44:39 | |
specifically design your experiment to look for chameleons, | 0:44:39 | 0:44:42 | |
which means that you look in a very high vacuum | 0:44:42 | 0:44:45 | |
and you use tiny, tiny particles, so we're using individual atoms. | 0:44:45 | 0:44:49 | |
But wrangling individual atoms isn't easy. | 0:45:00 | 0:45:04 | |
It takes an enormous amount of scientific hardware, | 0:45:06 | 0:45:09 | |
specially configured in a highly precise way. | 0:45:09 | 0:45:13 | |
Just six months after Clare's paper was published, | 0:45:14 | 0:45:17 | |
atomic physicist Holger Muller got in touch. | 0:45:17 | 0:45:21 | |
As it happened, he explained, he had exactly the right equipment needed | 0:45:21 | 0:45:25 | |
to perform Clare's experiment, right here in Berkeley. | 0:45:25 | 0:45:29 | |
From where, in 1998, Saul Perlmutter's group | 0:45:29 | 0:45:33 | |
discovered dark energy in the first place. | 0:45:33 | 0:45:36 | |
It might be that the conundrum could be solved at the same | 0:45:36 | 0:45:39 | |
institution that it was discovered. | 0:45:39 | 0:45:42 | |
We've been setting up this experiment for several years | 0:45:45 | 0:45:48 | |
when my post-doc colleague came across Clare Burrage's paper | 0:45:48 | 0:45:52 | |
on the pre-print server and we read the paper | 0:45:52 | 0:45:54 | |
and we found that, "Wow, they're describing | 0:45:54 | 0:45:57 | |
"exactly the experiment we've been building for all these years." | 0:45:57 | 0:46:01 | |
And we got excited about it so we stopped doing our original | 0:46:01 | 0:46:04 | |
experiment and started doing the dark energy measurement. | 0:46:04 | 0:46:07 | |
It's an amazing feeling to have that kind of quick response | 0:46:08 | 0:46:11 | |
because it almost never happens like that in science. | 0:46:11 | 0:46:14 | |
Things take a long time to go | 0:46:14 | 0:46:16 | |
from theory to somebody actually doing an experiment. | 0:46:16 | 0:46:20 | |
To have a measurement of something | 0:46:20 | 0:46:22 | |
we proposed in the space of six months is phenomenal. | 0:46:22 | 0:46:25 | |
The experiment involves using a vacuum chamber | 0:46:25 | 0:46:28 | |
and a cunning chameleon trap. | 0:46:28 | 0:46:31 | |
The animal, the chameleon, changes its colour in order to hide, right? | 0:46:31 | 0:46:35 | |
And in the same sense, the chameleon particle | 0:46:35 | 0:46:38 | |
changes its mass in order to hide. | 0:46:38 | 0:46:41 | |
At the centre of the vacuum chamber is a marble-sized sphere. | 0:46:43 | 0:46:48 | |
If there are chameleon particles around, | 0:46:48 | 0:46:51 | |
they will interact with the mass of the ball | 0:46:51 | 0:46:53 | |
and produce very little in the way of force but perhaps just | 0:46:53 | 0:46:58 | |
enough to affect something very small like an individual atom. | 0:46:58 | 0:47:02 | |
The heart of the experiment is this little sphere inside there | 0:47:02 | 0:47:08 | |
and so the experiment works by first collecting a cloud of caesium atoms | 0:47:08 | 0:47:13 | |
on top of the sphere so here's the sphere and about one centimetre | 0:47:13 | 0:47:17 | |
on top there's a little cloud of about 100 million caesium atoms. | 0:47:17 | 0:47:22 | |
The machine contains the atom cloud using infrared lasers, | 0:47:24 | 0:47:28 | |
invisible to the naked eye. | 0:47:28 | 0:47:30 | |
The beams need to be very precisely controlled, so they're sent around | 0:47:30 | 0:47:34 | |
a complicated series of mirrors | 0:47:34 | 0:47:36 | |
on what's known as an optics table. | 0:47:36 | 0:47:39 | |
We use lasers to control the atoms | 0:47:40 | 0:47:43 | |
and so to do that, we need to pass them through this table of optics. | 0:47:43 | 0:47:46 | |
The laser beam kind of takes a snake-like path throughout | 0:47:46 | 0:47:50 | |
all these optics but eventually gets into something like this, | 0:47:50 | 0:47:54 | |
an optical fibre. | 0:47:54 | 0:47:55 | |
The light can then travel through here | 0:47:55 | 0:47:58 | |
and is brought over to interact with the atoms. | 0:47:58 | 0:48:00 | |
So, you see here the sphere | 0:48:02 | 0:48:05 | |
and we trap the cloud of atoms just on top of the sphere, | 0:48:05 | 0:48:09 | |
and then we release the trap and the atoms are free to fall | 0:48:09 | 0:48:13 | |
subject only to the Earth's gravity | 0:48:13 | 0:48:16 | |
and the potential chameleon force. | 0:48:16 | 0:48:18 | |
When the atoms are released, | 0:48:20 | 0:48:22 | |
they will fall towards the ball, which will contain chameleon | 0:48:22 | 0:48:25 | |
particles, if they exist, and if they do exist, they will be | 0:48:25 | 0:48:30 | |
busy interacting with the mass of the ball, making themselves | 0:48:30 | 0:48:34 | |
heavy and reducing the distance over which their force can be felt. | 0:48:34 | 0:48:39 | |
Which isn't to say that the force is completely non-existent. | 0:48:39 | 0:48:43 | |
According to chameleon theorists, there'll be a tiny region | 0:48:43 | 0:48:47 | |
on the surface of the sphere where the force is active | 0:48:47 | 0:48:51 | |
and given that the atoms are so tiny, | 0:48:51 | 0:48:54 | |
they will be affected by that force. | 0:48:54 | 0:48:58 | |
If it exists at all. | 0:48:58 | 0:49:00 | |
All the team need to do is to precisely measure the difference | 0:49:00 | 0:49:04 | |
between the speed the atoms fall with and without the ball in place. | 0:49:04 | 0:49:09 | |
Now we want to measure the chameleon only | 0:49:16 | 0:49:18 | |
and not the combination of gravity and the chameleon, | 0:49:18 | 0:49:21 | |
so what we do is we will move this sphere out | 0:49:21 | 0:49:25 | |
and then do the measurement again, this time measuring gravity only. | 0:49:25 | 0:49:29 | |
The experiment is set up to compare the difference between how | 0:49:30 | 0:49:33 | |
fast the atoms fall towards the ball | 0:49:33 | 0:49:36 | |
and how fast they accelerate through empty space. | 0:49:36 | 0:49:40 | |
If the tracking reveals an unexplained acceleration, this | 0:49:40 | 0:49:43 | |
could be due to the force associated with the chameleon particle. | 0:49:43 | 0:49:48 | |
The experiment has now been running for over six months | 0:49:48 | 0:49:52 | |
and they're starting to get their first results. | 0:49:52 | 0:49:54 | |
Right now we have seen no evidence for chameleons, which means | 0:49:54 | 0:49:59 | |
they either don't exist or they hide | 0:49:59 | 0:50:01 | |
in a region of the perimeter space | 0:50:01 | 0:50:04 | |
that we can't yet measure. So, what does that mean? | 0:50:04 | 0:50:07 | |
If either the chameleon force is extremely weak | 0:50:07 | 0:50:11 | |
or it's even heavier than we thought, then we can't see them. | 0:50:11 | 0:50:15 | |
The team at Berkeley are now adjusting the experiment to rule out | 0:50:15 | 0:50:18 | |
any theoretical nooks and crannies where the chameleon might be hiding. | 0:50:18 | 0:50:24 | |
Well, if we make the experiment more and more and more sensitive, | 0:50:24 | 0:50:28 | |
we will either discover the particle | 0:50:28 | 0:50:31 | |
or rule it out once and for all. | 0:50:31 | 0:50:33 | |
A scientist might be like a drunk who lost his keys | 0:50:35 | 0:50:38 | |
and is now looking for it under the next lamppost... | 0:50:38 | 0:50:42 | |
..and it's not because he knows that the key is there, | 0:50:43 | 0:50:47 | |
but because it's hopeless to look in the dark anywhere else. | 0:50:47 | 0:50:50 | |
People have searched for dark energy in cosmology and in astrophysics, | 0:50:50 | 0:50:55 | |
and now we start looking for it under the atomic physics lamppost. | 0:50:55 | 0:51:00 | |
Whether this is a good idea or not, we will know in a couple of years | 0:51:00 | 0:51:03 | |
when it has either been found or not, but it's always exciting to | 0:51:03 | 0:51:08 | |
have... It's like a new window that you can open and look through | 0:51:08 | 0:51:11 | |
and you don't know what you will see before you've tried to do it. | 0:51:11 | 0:51:14 | |
Having more information is always a good thing | 0:51:20 | 0:51:22 | |
so ruling out possibilities. Although on a personal level | 0:51:22 | 0:51:26 | |
maybe it's a little bit upsetting because it's a nice theory | 0:51:26 | 0:51:29 | |
but it means that you've got more information and you can go | 0:51:29 | 0:51:32 | |
on from there and build something better, build a better theory. | 0:51:32 | 0:51:36 | |
With all these theories, it's really a question of taste. | 0:51:39 | 0:51:43 | |
You either like a cosmological constant or you can explain | 0:51:43 | 0:51:47 | |
it through a chameleon effect. | 0:51:47 | 0:51:49 | |
None of these as yet give us the elegant solution | 0:51:49 | 0:51:55 | |
that we are looking for and that's what really we're looking for. | 0:51:55 | 0:51:58 | |
We're looking for this simple, elegant solution to this strange | 0:51:58 | 0:52:02 | |
accelerated universe and nothing yet has given us that. | 0:52:02 | 0:52:07 | |
Chameleon? Yeah, maybe, but as yet, there's no evidence for it. | 0:52:07 | 0:52:12 | |
Dark energy? Yeah, we can sort of understand it, | 0:52:12 | 0:52:16 | |
but we can't get the number right | 0:52:16 | 0:52:18 | |
so we're still grasping in the dark | 0:52:18 | 0:52:21 | |
for an elegant, simple solution to what we see. | 0:52:21 | 0:52:24 | |
Where that simple solution will eventually come from | 0:52:28 | 0:52:31 | |
is anyone's guess. | 0:52:31 | 0:52:35 | |
That is one of the infuriating things about science. | 0:52:35 | 0:52:39 | |
It can't always produce the rabbit from the hat on time and on budget. | 0:52:39 | 0:52:44 | |
Sometimes it takes an unexpected turn of events, or what the | 0:52:46 | 0:52:51 | |
media like to call a "genius". | 0:52:51 | 0:52:55 | |
Though the geniuses themselves have | 0:52:55 | 0:52:57 | |
a rather different take on their exploits. | 0:52:57 | 0:53:00 | |
I'm not more gifted than anybody else. | 0:53:03 | 0:53:06 | |
I'm just more curious than your average person | 0:53:06 | 0:53:09 | |
and I will not give up on a problem | 0:53:09 | 0:53:11 | |
until I have found the proper solution. | 0:53:11 | 0:53:14 | |
I think that curiosity is what drives...what drives most | 0:53:14 | 0:53:17 | |
cosmologists and physicists, a curiosity about the universe - why? | 0:53:17 | 0:53:22 | |
What is the universe made out of? Why are we here? | 0:53:22 | 0:53:25 | |
How did the universe begin? | 0:53:25 | 0:53:27 | |
What will happen to the universe in the future? | 0:53:27 | 0:53:29 | |
All of these are questions which are driven by curiosity. | 0:53:29 | 0:53:32 | |
I have no special talent. | 0:53:37 | 0:53:39 | |
I am only passionately curious. | 0:53:39 | 0:53:42 | |
Curiosity, I think, is... | 0:53:43 | 0:53:46 | |
Well, it's the best motivating force, OK? | 0:53:46 | 0:53:50 | |
Working hard doesn't necessarily get you to an answer. | 0:53:50 | 0:53:55 | |
Working too hard can actually stifle creativity. | 0:53:55 | 0:53:59 | |
With our work, you know it's a mixture of inventiveness | 0:54:00 | 0:54:03 | |
and persistence in the hard work. | 0:54:03 | 0:54:05 | |
It's a combination. | 0:54:05 | 0:54:07 | |
It's the end of the Euclid conference in Lausanne. | 0:54:13 | 0:54:17 | |
The conference organisers have laid on a social evening, | 0:54:17 | 0:54:20 | |
cruising around Lake Geneva. | 0:54:20 | 0:54:23 | |
It's a chance for the delegates to unwind | 0:54:23 | 0:54:25 | |
and maybe even think a little about the biggest picture of all. | 0:54:25 | 0:54:30 | |
Yeah, so Einstein's theory was motivated for a reason, right? | 0:54:30 | 0:54:34 | |
He had an equivalence principle. | 0:54:34 | 0:54:36 | |
Yeah, and, I mean, we're going to measure | 0:54:36 | 0:54:37 | |
a lot of things about the nature by looking at how it evolves, | 0:54:37 | 0:54:40 | |
how dark energy actually evolves with red shift. | 0:54:40 | 0:54:42 | |
But the problem is the zero-point energy, | 0:54:42 | 0:54:44 | |
the vacuum energy, the quantum | 0:54:44 | 0:54:46 | |
mechanical part that you add there. | 0:54:46 | 0:54:48 | |
Try and study the nature of dark energy | 0:54:48 | 0:54:50 | |
and at the same time, try and test if general relativity works. | 0:54:50 | 0:54:53 | |
So, there's like a lot of work | 0:54:53 | 0:54:54 | |
and a lot of discoveries that are going to happen down the road. | 0:54:54 | 0:54:57 | |
-Exactly. -And I'll drink to that. | 0:54:57 | 0:54:59 | |
Exactly that. | 0:54:59 | 0:55:01 | |
The process of scientific discovery sometimes makes progress | 0:55:08 | 0:55:11 | |
through sheer hard work | 0:55:11 | 0:55:13 | |
and sometimes it needs someone to take an inspired alternative view. | 0:55:13 | 0:55:18 | |
We learned an awful lot about animals | 0:55:19 | 0:55:22 | |
and plants by simply observing them, but it took Darwin, | 0:55:22 | 0:55:25 | |
with a radical idea, | 0:55:25 | 0:55:27 | |
to give us a context to understand life itself. | 0:55:27 | 0:55:31 | |
And in our efforts to understand the wider world | 0:55:31 | 0:55:34 | |
and even the universe, observations are critical. | 0:55:34 | 0:55:38 | |
The ideas of dark matter and dark energy come courtesy of people | 0:55:39 | 0:55:43 | |
watching stars but just as Einstein musing on his train managed | 0:55:43 | 0:55:49 | |
to take all the known science and | 0:55:49 | 0:55:51 | |
see it from a different, more useful, angle, | 0:55:51 | 0:55:55 | |
it might be that to solve the dark energy problem, someone needs | 0:55:55 | 0:55:58 | |
to pull off a similar trick | 0:55:58 | 0:56:01 | |
and come up with an even better idea. | 0:56:01 | 0:56:05 | |
There are an awful lot of very smart people in the world. | 0:56:05 | 0:56:08 | |
I wouldn't be surprised if we end up with another Einstein, you know, | 0:56:08 | 0:56:11 | |
somewhere along the line here. | 0:56:11 | 0:56:13 | |
I don't know whether it'll be in our lifetime but we... | 0:56:13 | 0:56:16 | |
I think we have a good shot at it. | 0:56:16 | 0:56:19 | |
We need teams like Euclid. | 0:56:19 | 0:56:21 | |
That's the only way you can get the data that you need. | 0:56:21 | 0:56:24 | |
But to understand that data, to give it some interpretation, | 0:56:24 | 0:56:28 | |
to give it an idea, | 0:56:28 | 0:56:30 | |
could come from one person. | 0:56:30 | 0:56:32 | |
That could be the next Einstein. | 0:56:32 | 0:56:34 | |
A genius could come up and put all the observations that we have | 0:56:35 | 0:56:38 | |
so far, put it together, and come up with a new theory. | 0:56:38 | 0:56:41 | |
Yeah, it is quite possible. | 0:56:41 | 0:56:44 | |
I'm kind of hoping it's me. | 0:56:44 | 0:56:46 | |
The tantalising truth is that all it might take to solve | 0:56:52 | 0:56:55 | |
the mystery of the dark energy is one big idea, | 0:56:55 | 0:56:59 | |
for someone out there to see things differently, | 0:56:59 | 0:57:04 | |
someone perhaps like you. | 0:57:04 | 0:57:08 | |
And if that new Einstein is you, | 0:57:08 | 0:57:11 | |
if you manage to solve the mystery of dark energy, | 0:57:11 | 0:57:15 | |
you're likely to become very famous indeed, | 0:57:15 | 0:57:18 | |
as famous as the original Einstein. | 0:57:18 | 0:57:21 | |
Wherever I go and wherever I stay, | 0:57:23 | 0:57:27 | |
there's always a picture of me on display. | 0:57:27 | 0:57:30 | |
On top of the desk or out in the hall, | 0:57:30 | 0:57:34 | |
tied round a neck or hung on a wall. | 0:57:34 | 0:57:37 | |
Women and men they play a strange game, | 0:57:37 | 0:57:40 | |
asking, beseeching, "Please, sign your name." | 0:57:40 | 0:57:43 | |
From the erudite fellow they brook not a quibble, | 0:57:43 | 0:57:46 | |
but firmly insist on a piece of his scribble. | 0:57:46 | 0:57:50 | |
Sometimes, surrounded by all this good cheer, | 0:57:50 | 0:57:53 | |
I'm puzzled by some of the things that I | 0:57:53 | 0:57:56 | |
and wonder, my mind for a moment not hazy, | 0:57:56 | 0:58:01 | |
if I, and not they, could really be crazy. | 0:58:01 | 0:58:05 |