NEIL DEGRASSE TYSON: [APPLAUSE] Thank you
all for attending this, the 25th or so— I’ve lost count— annual Isaac Asimov Panel
Debate. I’m Neil deGrasse Tyson, your personal astrophysicist. And I also, after that, I serve as the Frederick
B. Rose Director of the Hayden Planetarium. And this is our annual event. This was started in the year 2000, with interest
from the family of Isaac Asimov at the time, the late Isaac Asimov. Something I didn’t know until I was told
is that of his 600 books that he’s written, most of them were researched at our research
library here at the museum. [APPLAUSE] And so the legacy— it’s quite
a legacy to leave. And we wanted to make sure we had a living
memorial to him. And that is this event. Are we all aware of the topic this evening? I met some people outside, they said, “Oh,
what are we doing tonight?” And I said, “That’s love.” Because you’re coming without even knowing
what the subject is. It is “The James Webb’s Space Telescope’s
Cosmic Revolution.” There’s observations made in the early universe
that were very difficult to explain, given our prior understandings of how the universe. should have worked back then. And we figured that was the right time and
place to make that the subject of this year’s panel. I will be introducing the panel. You will get to hear their voices initially,
just to— you can warm up to them. Then we’ll get into our conversation. This event, you should think of it as, you
are eavesdropping on a conversation we are having in the breakout lounge of a scientific
conference. Okay? That’s how you should think about what we’re
about to do. And I’m a little bit of an interlocutor. So if there’s something that I think you
might not understand, I’ll break in. But mostly, it’s scientists being scientists
among other scientists. And this is what we all look forward to. So thank you. [APPLAUSE] Let me bring out the panel, and we’ll learn
about all their expertise shortly thereafter. First, a very longtime friend and colleague. We came up through the system of astrophysics
together. Wendy Freedman, from the University of Chicago. Wendy, come on out. [APPLAUSE] From the University of Texas at
Austin, Michael Boylan-Kolchin. I think I pronounced— Kolchin. Yes, Michael. [APPLAUSE] And next, right from the CCA, right
downtown— we’ll learn more about that institution in a minute— is Rachel Somerville. Rachel, come on out, neighbor. [APPLAUSE] And from Georgia Tech, Georgia
in the house, John Wise. John, come on out. And fifth on our panel is from Yale University
right up there in New Haven, Connecticut, Priya Natarajan. Priya, come on out. [APPLAUSE] Everyone here is an expert in some
way regarding data, simulations on a computer, and observations of the early universe, especially
with regard to galaxies. And we’re going to find out why that matters
in a minute. So Priya, tell us, what is your professional
interest and specialty? NATARAJAN: So, my expertise and interest is
really in the invisible universe. So, the dark components that we have to infer
about dark matter, dark energy, and black holes. TYSON: So when you say invisible, you don’t
mean just that your— a telescope doesn't— you don’t mean that the human eye doesn't
see it. NATARAJAN: No, I mean more than that. TYSON: Yeah. NATARAJAN: There is no light in any wavelength
that is emitted by these entities. And so you infer their presence indirectly. And it turns out that they play a very important,
if not starring role, in the universe. TYSON: Maybe more of a role than the stuff
we can see. NATARAJAN: Absolutely. And I— TYSON: That’s kind of spooky, you know. NATARAJAN: Yeah. TYSON: You say you’re an expert on stuff
we can't see. NATARAJAN: Right. TYSON: That’s more important than the things
we can see. NATARAJAN: Yeah. TYSON: Okay. I just want you to remember how weird. that is. NATARAJAN: Well, the hidden is always more
important than what is right in front of your eyes. TYSON: That’s poetic. The hidden is always more important than what’s
in front of your eyes. Thank you for that. So John, up from Georgia Tech. WISE: That’s right. TYSON: Peach country. WISE: Yeah, the Peach State. TYSON: The Peach State. So, your expertise lands where? WISE: I do computer simulations on some of
the largest supercomputers in the nation of the first stars and galaxies in the universe,
trying to see how they actually form from scratch. TYSON: Okay. Because you can't observe that. You have to simulate it. WISE: That’s right, yeah. Not even James Webb’s space telescope can
see the smallest galaxies. TYSON: Okay. So we have to trust that you’re putting
the right input— WISE: That’s right, yes. TYSON: Okay. We’ll get back to that. WISE: Okay. [LAUGHTER] TYSON: Rachel. You’re from the CCA, right on— SOMERVILLE: Correct. TYSON: Downtown. So just— that’s a new institution. Just give us a minute on what that institution
is, and what brought you to them. SOMERVILLE: So, the CCA stands for the Center
for Computational Astrophysics, and we are one of five centers that are part of the Flatiron
Institute. And the Flatiron Institute is supported by
the Simons Foundation, which was started by Jim and Marilyn Simons. And each of those centers works on a different
aspect of computational science. TYSON: So I think biology is one of them as
well, is that right?..... SOMERVILLE: Biology, neuroscience, math, quantum
physics, and— am I forgetting one? TYSON: Astrophysics. [LAUGHTER] SOMERVILLE: And astrophysics. There we go. TYSON: Okay. And so your specialty is? SOMERVILLE: So, I like to say that I make
galaxies on the computer. And I also make some supermassive black holes
to make things interesting. And I was also part of one of the teams that
planned some of the first observations that James Webb took. TYSON: Okay. So you helped to guide the— you have some
of the— you have the steering wheel. SOMERVILLE: We had some say into where Webb
pointed when it was first switched on. TYSON: Interesting. Okay. We’ll get back to that. SOMERVILLE: All right. TYSON: Definitely. Michael, up from Texas. BOYLAN-KOLCHIN: Yes, sir. TYSON: How you doing? So what do you— where do you come— what’s
your cosmic interest here? BOYLAN-KOLCHIN: Well, I also work on dark
matter. I’m a theorist. I use computational— big computation simulations. I also do pencil and paperwork, as much as
possible. And my interest is in the sort of descendants
of the first galaxies that John is studying. So, I look around us at maybe their fossil
remnants. TYSON: Wait, he just said he made galaxies. He didn’t say he made the first galaxies. Or is that the same thing? BOYLAN-KOLCHIN: Well, John, I think, studies— WISE: I make the first galaxies. TYSON: Okay. [LAUGHTER] All right. BOYLAN-KOLCHIN: The first galaxies, yeah. Some of the earliest galaxies to form, so
we can't see them directly when they’re forming with JWST, even. But we can see them around us today, the fossil
remnants. And so we can study them very well around
us in the Milky Way. So I study those galaxies to tell us about
dark matter, and what was happening at the earliest phases. TYSON: Okay. And Wendy, we go way back, Wendy. Wow. FREEDMAN: Don’t tell. [LAUGHTER] TYSON: No— no, it’s an important piece
of history, because we pre-date the Hubble Telescope when it was launched, and you had
a big say in what the Hubble Telescope would do first. Where we pointed it first, and why. Because at the time, our understanding of
the age of the universe. was uncertain by a factor of two. That’s— that should have been more embarrassing
to us than we had felt at the time. [LAUGHTER] But you were going to do something
about that. So tell me, just give me a back story there. What happened with Hubble, and your role in
it? FREEDMAN: So, back story, that’s right. We didn’t know the age of the universe better
than a factor of two. Was the universe 10 billion years old, or
20 billion years old? And there were heated debates. TYSON: But were you yet confident that it
was somewhere in between the 10 and the 20?.... FREEDMAN: It would have been unlikely that
it was outside, but not out of the realm of possibility, given our ignorance at the time. And so one of the primary reasons that the
Hubble Space Telescope was built, in fact, was to resolve this problem. Solve the debate. And the— TYSON: So the motivation for Hubble. FREEDMAN: The motivation for building Hubble. And in fact, the size of the primary mirror
was set to be able to observe the stars that we used to measure distances, called cepheids,
with the Hubble Space Telescope at the Virgo Cluster. TYSON: Wait, wait. I saw the size of the mirror was set by the
payload bay of the shuttle. FREEDMAN: That was another factor. [LAUGHTER] But— TYSON: No, if they weren’t— FREEDMAN: No, no, no. TYSON: If we made it an inch bigger, it wouldn't
fit in the shuttle. FREEDMAN: True. But if— you could have made it smaller,
and it would have been cheaper. And the reason it wasn’t made smaller was
to be able to resolve this debate. TYSON: Got it. FREEDMAN: So the director at the time of the
Space Telescope Science Institute put together a panel of people that said, what are the
most important projects Hubble can do? Resolving this problem was number one. And he made what he called “Key Projects.” Big telescopes, he said. Big projects. If Hubble were to fall in the ocean and it
hadn’t done something, we’d never know what the answer was. So, what were those projects? And measuring this Hubble Constant, the expansion
rate of the universe, was the highest priority... TYSON: I hadn’t thought about it that way. So the key projects were— if something unforeseen
bad happens to the telescope on orbit, the first things— we would have the first and
most important projects resolved. FREEDMAN: Yeah. And he was afraid that if he put together
a committee to decide who got the time, the committee would slice it into small pieces
to give more people time. And so some problems required more time. And so he designated those as key projects,
with a lot of time. TYSON: And you got a key project. FREEDMAN: I got a key project. TYSON: You got a key project. So you are— you are on the main paper that
established, that settled that argument. And so where did the age of the universe show
up on that paper, back then? FREEDMAN: 13.7 billion years. TYSON: You— it sounds like you nailed it. FREEDMAN: We nailed it. And it’s held for, you know, the 20 years
since, 23 years now, since we published our final paper. That’s the value— using that method that
we used with Hubble, it has not changed... TYSON: Michael, do you agree with that age
of the universe? BOYLAN-KOLCHIN: Well, I think that there’s
an alternate way you can measure that age, and that’s with the cosmic microwave background—
light from the earliest phases of the universe. And studying its properties statistically
tells you about the components of— TYSON: Wait, so how did you get the age of
the universe, if you didn’t use the microwave background? What did you do?. FREEDMAN: So, we’re measuring galaxies nearby,
and we’re measuring how far away they are and what velocities they’re moving at. TYSON: At the expansion of the universe. WEINDY: And that’s expansion of the universe,
which, you can extrapolate backwards, essentially, using a cosmological model, and determine
the age of the universe. TYSON: In fact, that’s what Edwin Hubble
first did back in the 1920s. Did that have something to do with why they
named that telescope after him? FREEDMAN: It did indeed. It wasn’t an accident. [LAUGHTER] TYSON: It wasn’t an accident. Okay. Okay. All right. So now, you’re going to not look at galaxies. You’ve got a back door to the age of the
universe. BOYLAN-KOLCHIN: That’s right. We’re looking, actually, the other edge
of the universe, as far away as we can see. The very first light in the universe. And that tells us properties of the universe
at the very earliest times. And that, combined with the cosmological model,
also gives us an age. And that age is 13.8 billion years, with an
uncertainty of only 20, 25 million years on it. TYSON: So you want us to care that her answer
is 13.7, your answer’s 13.8. But that difference matters to the two of
you? BOYLAN-KOLCHIN: Well, I think that difference— TYSON: I grew up— I came up with, it was
a factor of two difference. BOYLAN-KOLCHIN: Well, what’s 100 million
years between friends, I get you. But. [LAUGHTER] You know. But I think there’s a bigger issue that,
the way we measure the Hubble Constant locally, that Wendy has really worked on and been an
expert in and pioneered— there are different numbers that the different groups get sometimes. And there can be a number that would give
a different age, a younger age of the universe. More like 12.8 billion years. And so a billion is starting to get to be
an issue, perhaps. TYSON: So there’s tension in the early universe. BOYLAN-KOLCHIN: There may be. [LAUGHTER] FREEDMAN: Agreed. TYSON: Rachel, do you have any reflections
on the age of the universe? Or you’re cool with whatever they tell you? SOMERVILLE: I’m pretty much cool with whatever
they tell me. [LAUGHTER] Galaxies don’t— don’t care
that much. TYSON: Yeah. SOMERVILLE: As long as the stars are younger
than the universe, I’m good. TYSON: Oh! SOMERVILLE: Yeah. We have a problem if that’s not the— yeah. That was a problem back when I was— yeah. So it’s cool. TYSON: Yeah. So you’re telling me there was— I think
I remember this. There was a time when someone discovered stars
that were older than the age of the universe you all were telling us. And this was, like, big headlines. SOMERVILLE: That was just— TYSON: That’s embarrassing. SOMERVILLE: Yeah. TYSON: So how was that resolved? FREEDMAN: That was resolved by discovering
that the universe is accelerating and getting better measurements with Hubble. Those two things. TYSON: Oh. This is not about the accelerating— it might
be. We might learn more about this from Priya
in a minute. So this age— so where should we take the
age right now? Just tell me, who do we believe? No, let me not cause a fight. Let me just say, these are two methods that
in and of themselves are sound. Yet they give two different answers that do
not overlap in their uncertainties. So something has to give. BOYLAN-KOLCHIN: Right. TYSON: Who’s going to yield here? FREEDMAN: Well, I think the interesting part
of this— so, there are at least a couple possibilities, right? There might be something wrong with the data
that is misleading us. Or, it could be that there’s something missing
in our model, our standard model that has the dark energy and dark model we’ve been
talking about, and that there’s another physical something that we have not yet discovered. And this might point to that. And so the question is, can we find something
in the data that might be misleading us? Or, this more exciting possibility— I think
all of us would be very excited at the idea that we could learn something fundamental
about the early universe, by comparing these values. Because there’s only— you know, we live
in one universe right now. And these numbers are not matching. They should match. We’re coming from high red shift, coming
from low red shift. And it’s like, we’re, you know, digging
a tunnel on opposite sides of a mountain, and we missed. [LAUGHTER] So, is it important, or not? And that’s what we’re trying to— TYSON: So, Michael. You sounded more confident about your answer
than Wendy sounded about her answer. BOYLAN-KOLCHIN: Well, you know, as a good
theorist, I could argue any of the answers, hopefully. [LAUGHTER] And whichever the answer— TYSON: That’s a good theorist, arguing any
answer. BOYLAN-KOLCHIN: Yes, that’s right. TYSON: Not a bad theorist. BOYLAN-KOLCHIN: Well, I think that one angle
that I’m very interested in, and I think is becoming interesting again, is this question
of the oldest objects in the universe. Since there is this discrepancy, we can go
back and ask, now with better instruments. JWST, other observatories. Can we do better in age-dating stars and star
clusters? Because if we can say, “The oldest star
clusters are definitively older than that younger age of the universe,” then we’re
back to saying that is probably the wrong answer. TYSON: Got it. So Rachel, in the early universe, what is
it that the James Webb Telescope found, that sent everyone into a tizzy? SOMERVILLE: So, I think there are two things
that have sent us into a tizzy. One is that Webb found a lot of very luminous
galaxies, at very, very early times, pumping out huge amounts of ultraviolet light. And the theories that had been published before
Webb launched did not predict that large a number of such bright galaxies. So that caused a big fuss. And then a little bit later, we started to
find evidence for super-massive black holes that were also much larger, much more massive,
and at much earlier times than theory had predicted. So— and maybe those two things go together. Right? But, so the problem is sort of too many, too
bright, too massive. How did we make these things so big? TYSON: So we under-predicted how— the energetics
of the early universe. Is that a fair characterization? SOMERVILLE: I like that way of characterizing
it, actually. So one of the first analysis, which was done
by our friend here, was based on how massive we thought these objects were. And the masses are actually quite uncertain. TYSON: Masses of the black holes, or of the
galaxies? SOMERVILLE: So now I’m talking about the
galaxies. So the mass of stars in the galaxy is not
something we can observe directly, right? We observe the light. And specifically, we observe the ultraviolet
light, primarily, for these early, early objects. Because the light is red-shifted as it travels
to us. So— TYSON: Wait, just to clarify that. The James Webb Space Telescope is exquisitely
tuned to see infrared light. SOMERVILLE: Ah. TYSON: And you’re speaking glibly about
the emission of ultraviolet light in the early universe. SOMERVILLE: Yes. That’s a great point, Neil. Yes............ TYSON: So what’s going on here? SOMERVILLE: So what’s going on is that as
we have discussed, the universe is expanding. And as light travels to us for the 13.6 billion
years and change— TYSON: 13.6? I— SOMERVILLE: From— [LAUGHTER]. No, no, no. Remember— FREEDMAN: It took some time. TYSON: Oh, just the galaxy— that’s the
whole universe. SOMERVILLE: This is the galaxy. TYSON: Just the galaxy, thank you. SOMERVILLE: So it took a couple hundred million
years for the galaxy to form. TYSON: Couple hundred million years. SOMERVILLE: Right? And then that light, as it travels to us,
the wavelength is what we call red-shifted. That’s why it’s called a red shift, right? So the wavelength gets longer, so it’s emitted
in the ultraviolet. But by the time it gets to the Webb, it’s
in the infrared. TYSON: So we knew this in advance. SOMERVILLE: We knew this in advance. This is fundamental physics. TYSON: So the James Webb Space Telescope— SOMERVILLE: It’s almost like they planned
it, right? TYSON: -- was conceived to be exquisitely
sensitive to the formation of galaxies, knowing that they emit copious ultraviolet light. SOMERVILLE: And in fact, this is one reason
that Hubble was not able to push beyond a certain red shift. So there was sort of a red shift limit, if
you like, a hard limit that Hubble could not push beyond, partly because it’s smaller. Its mirror is smaller, so it can't collect
light as well, so it couldn't see the faint, faint objects. But also because it couldn't see far enough
into the infrared, which now Webb is allowing us to do. TYSON: John, tell me about black holes in
galaxies. Why are they important at all? WISE: Yeah. So, today, we see black holes, mass, supermassive
black holes at the center of all galaxies. But— TYSON: All galaxies we’ve looked at. WISE: Yeah. Most massive galaxies we’ve looked at. But in the early universe, that’s not always
the case. And it’s a big question of which galaxies
form supermassive black holes, and which ones don’t. And what kind— where did these supermassive
black holes actually come from? And we call these the seeds of the supermassive
black holes. So, you know, it’s a big question, whether
they start big or small. Because when you look with JWST, back then,
the supermassive black holes might be nearly as big as the stars that— in the galaxy
that contains it. But nowadays, it’s one part in 1000. So it’s— they’re so much more massive. TYSON: Today. WISE: Today. But fractionally, compared to the galaxies
back then, they’re much larger in relationship to their stars. TYSON: Oh, I get it. I get it. So Priya, I think what he’s saying here
is that the— we’re still forming things. NATARAJAN: Yeah. TYSON: So you can get a black hole not as
massive, then, as today, but a much bigger fraction of the mass that would be collected
to become a galaxy. NATARAJAN: That’s right. TYSON: So is it fair to say the black holes
are seeding the galaxies? NATARAJAN: I think that’s the big open question,
as to which comes first. I think the question, though, is that we know
that they grow in tandem. But occasionally, you could start out with
a small black hole seed and stars forming around it and the host— we believe that
all black holes actually need a host galaxy. There are not sort of naked black holes floating
around. TYSON: Oh. Okay. So the galaxy comes first. NATARAJAN: I think it remains to be seen. There— TYSON: You just said! [LAUGHTER] NATARAJAN: Well, there is a class of black
holes that you could make, potentially, in the very early universe, the infant universe,
called primordial black holes. And those would supersede the formation of
anything material that we know. So— but we don’t know if they exist yet. SOMERVILLE: But we don’t think that those
are the seeds of the black holes. NATARAJAN: No, but they could exist, though. Right? SOMERVILLE: Yeah. NATARAJAN: They may not be the seeds of the
black holes that we are seeing in the centers of all galaxies nearby. But they could have been seeds of some very
early galaxies, for example. We don’t— that remains to be seen. The problem is that once you see a black hole,
you have no idea what it— where it came from. Because there is no information about what—
where the mass that fed this black hole came from, and how it formed. So the only way we understand where a black
hole could have come from— and as Rachel said, they’re much more ubiquitous, so there
have to be multiple ways to form them— is the relationship between the mass of the black
hole seed and its host galaxy, its parent galaxy. TYSON: Because the galaxy is going to feed
it, ultimately. NATARAJAN: The gas— yes. The gas from the galaxy is going to feed it. But stars form from the same gas. TYSON: Okay. NATARAJAN: So as John mentioned, in the very
early universe, if there is a special way to form black holes— and a bunch of us predicted
several. years ago that there has to be more than one
way to make these black holes— you could make some black holes that were really massive
from the get-go. Massive seeds. And we happened to find evidence for that
from JWST. TYSON: All right. But John, how do you just create a supermassive
black hole? Is that just a knob you turn in your software? And then say, “Oh, it matches, so I must
be right.” [LAUGHTER] Wait, wait. How many knobs are in your software? WISE: I have many, many knobs, but it takes
an expert. TYSON: I’m just saying, if one of them is
the temperature, the age, the size, the this, the mass distribution, and everything is an
adjustable parameter, and you adjust it until it matches, what confidence should any of
us have that your configuration of knobs is the actual universe? WISE: No, that’s a great— TYSON: And you’re just not over-supplied
with ways to match what you have to match? WISE: Yeah. Because you— TYSON: Because you’re not publishing papers
where you say, “My models don’t match this. Here’s my”—no. It’s gonna match it, because that’s why
you’re publishing the paper. WISE: That’s right. TYSON: But why should I have confidence at
all? WISE: Yeah. I mean, I— TYSON: You could do some of this, too. NATARAJAN: Yeah, I do. TYSON: Don’t you do— it’s a question
for both of you. NATARAJAN: Yes. TYSON: Okay. What? Right here. WISE: No, I have to build my own confidence. TYSON: Okay, go. WISE: I have to build my own confidence in
the simulation. Because— I mean, the universe. is a very complex place. And so are our simulations. So we do these test simulations, in which
we can actually compare our results from our simulations. Say a single supernova, right? We have one injection of an energy. You have a star dying, and you see how it
expands. And we do many of these tests in which we
can actually compare it to analytical solutions. Because once you put together all these processes,
together in a supercomputer simulation, you can't predict how they’re going to interact. But with— you gain confidence from these
test analytical simulations. TYSON: So you’ve done it in pieces initially. WISE: Uh-huh. TYSON: Before you can gain confidence in the
entire system. WISE: That’s right. Yes. TYSON: Okay. And do you— are your computers as powerful
as his? He said he used supercomputers. NATARAJAN: I use supercomputers occasionally
too. But I also work on the storyline of the universe. So there are patches that you simulate one
patch at a time. Then I use his simulations to tie them all
together, and then I confront the data from every epoch in the universe, with what the
simulation is telling us. TYSON: Okay. So she uses real data. [LAUGHTER] WISE: I compare against data. TYSON: You do? NATARAJAN: He does too, yeah. TYSON: He does too. Okay. All right. Rachel, remind me, what are the dark ages
in the early universe? What is that? SOMERVILLE: Ah. So as Mike mentioned, the first light in the
universe was actually sort of the glow of gas that was left over after the Big Bang. And after that—...... TYSON: Which we observed. We see. SOMERVILLE: Which we observe, as the cosmic
microwave background radiation, exactly. And after that, there were no stars. There were no accreting black holes. There was nothing producing any light. So we call that the dark ages. And the dark ages ended when the first star
in the universe— presumably it was a start— was born and started to emit light. TYSON: About how much time was that delay? SOMERVILLE: We think that was between 100
and 200 million years. We have not yet seen those first stars, we
don’t think. Even JWST is not powerful enough to see them. But our theory predicts it should be around
100 to 200 million years after the Big Bang. TYSON: John, last I read, JWST found galaxies
in the dark ages. WISE: Well, I don’t think there’s any
galaxies in the dark ages that they’ve found. But they found very— TYSON: Wait, so you’re saying you’re right,
and the James Webb Space Telescope was wrong? WISE: The James Webb Space Telescope doesn't
have feelings, so I think it’ll be okay. But— TYSON: Yeah. It’ll survive this assault on its integrity. WISE: Yes. What I think they have found are certainly. galaxies earlier than we’ve ever seen them
before, but not what we really think of as really fundamentally the dark ages, when—
before the first stars in the entire universe formed. We haven’t seen anything that far back. .........
TYSON: So Wendy, if we don’t look at the cosmic microwave background but we have galaxies
back then, can't— doesn't that help figure out the age of the universe, if you’re in
a galaxy mode by doing so? FREEDMAN: So you’re talking about observations
in the early universe that shed light— TYSON: Yeah, yeah. Yeah. And we’ve got some— FREEDMAN: Yes, in principle. TYSON: He— he denies them. He’s in denial, that’s fine. Just the ones declared, the James Webb galaxies
that seem to hail from the dark ages, that gets you data even farther back than you ever
would have used before. Does that help you tighten the age? FREEDMAN: Well, I think as Michael was saying
before, it’s another way of getting at the age. It’s a way of doing this in a very different
way than we do locally. But I think one of the things surfacing in
this conversation is that you need to understand a lot of things, particularly about stars,
which we haven’t gotten into. Right? So there— what you see in the distant universe
is the integrated light from a galaxy. It’s— you don’t have the opportunity
to look at individual stars. TYSON: It’s just too far away to resolve
that? FREEDMAN: Too far away. These are, you know, smudges. They’re not individual stars that you can
see. And so stars might have a very different history
of— in the galaxy— different history of star formation, different metal abundance,
different amounts of reddening, different kinds of dust that are causing the reddening. A different distribution of stars as they
form. TYSON: When you say metal abundance— we’re
in the early universe. How much heavy metal has been made yet, if
it’s all made in supernova? Wouldn’t there be, like, zero heavy elements,
then? FREEDMAN: Well, we’re seeing heavy elements
in the spectra of these objects. TYSON: Okay, let me ask it differently. Why are you seeing heavy elements early in
the universe, before we’ve had a chance to bust out some supernova and spread the
elements that it made into that environment? FREEDMAN: Yeah. And I think that’s the interesting question,
right? I mean, one of the exciting things about JWST
is we had theories of how galaxies formed, but it’s really nice to actually look and
say, “What is happening?” But then you’re looking, and you have to
interpret what you’re seeing. And there are a lot of more knobs, as you
say, that can go into the models, that will give you the same answer if you adjust them
in the way that you can explain the observations. So there’s additional challenge in interpreting
the ages, is what I would say. TYSON: Right. A very big point which I forgot to mention,
John— you adjust your knobs and you get a result. So do you have a way to test what other adjustments
of those knobs gives you the same result?.... WISE: So, we compare against observations. So before James Webb went up, right, we had
to compare against other simulations. And it was like— you know, it was a big
uncertainty. Are our galaxies actually realistic or not? And I guess looking back at it, I was always
worried, because our galaxies were more massive than other groups. And— because we don’t have the luxury
of actually comparing it to observations in the present day. Because a lot of other groups, they run simulations
until the present day. But we really specialize in the first billion
years after the Big Bang. And, like, once these observations of JWST
came out, they’re much more massive, or much brighter than expected. And that kind of matched with our predictions,
and kind of— you know, made me feel good about myself. All that anxiety just weighting on us. TYSON: We— we feel good about you too. That’s fine, John. [LAUGHTER] Priya, I loved what you said where
you— you staple together the various slices of time. NATARAJAN: Yeah. TYSON: And then compare that with the data
that comes to you from those slices of time. I’m still trying to understand, how does
your understanding and research on black holes, how is that touched by anything JWST is finding? Because it’s just finding these— this
pool of light of early galaxies. How does— why do black holes matter back
then? Does it tell you that galaxies formed sooner
or faster? What is the clue that you’re getting? NATARAJAN: Well, it turns out that, you know,
‘til quite recently, ‘til about five, ten years ago, we believed that black holes
were— played a marginal role in galaxy formation, because their masses were tiny compared to
the stars. TYSON: The big— if you fell in, that’d
be a bad day for you. NATARAJAN: That’s right. TYSON: But— but— so, I just read recently,
a month ago, we discovered the highest mass black hole ever in a galaxy? NATARAJAN: That’s right. TYSON: That checked in at— who remembers
that number, what was that number? NATARAJAN: It was like 10 billion solar masses,
yeah........ TYSON: Don’t you love how astronomers—
10 billion. We’re just so casual with astronomically
large numbers. So 10 billion. And how big is the black hole in our galaxy? NATARAJAN: It’s just 4 million times the
mass of the sun. TYSON: Oh, that’s low. NATARAJAN: Yeah. It’s still supermassive, because anything
that’s above a million is called, classified, as supermassive. TYSON: It’s still supermassive, but it’s
pretty lame compared to this other one. NATARAJAN: It’s pretty garden variety, yeah. TYSON: Yeah. Black hole envy in the universe. NATARAJAN: [LAUGHTER] Right. TYSON: Yeah. So— NATARAJAN: So, in the early— TYSON: So you’ve got to deal with that. NATARAJAN: Right. TYSON: This is going to make a difference
in everything you say and think about the formation of galaxies. NATARAJAN: That’s right. So very early on in the universe, because
there’s only one big gas reservoir from which both stars get made from cooling gas,
and the black hole gets fed, there’s sort of a competition for who gets the gas. Right? So, who goes— grows more rapidly, whether
it’s the black hole or it is the stars. So when we see data from the James Webb, we
are seeing the integrated light— TYSON: Of both. NATARAJAN: Of both. But then we also have a spectrum. And so there are very specific spectral signatures. So as a function of wavelength, that’s the
amount of energy that’s coming out. And we know what the features are for a growing
black hole. And so we are seeing these composites. So you know you have a black hole in place
that’s actively growing, and you have starlight. So— however, the key, key thing to discover
a rapidly growing black hole, is x-ray radiation from the black hole. Because the gas gets heated in the vicinity. The dying gasps of the gas, before it falls
into the black hole, it starts to speed up and starts to get heated up, and it starts
glowing and you see x-ray radiation. TYSON: It is glowing so hot— NATARAJAN: Yeah. TYSON: It’s giving off x-rays. NATARAJAN: Yeah. And so you should be able— TYSON: It’s like a million— how many—
how hot is that? NATARAJAN: Ten million. TYSON: Ten million degrees. NATARAJAN: Ten million, 15 million. And so you should be able to see if the object
was bright enough. So that’s the big question here. Can you really reach the first black holes? You should be able to see it with the Chandra
X-ray telescope as well as James Webb Space Telescope. TYSON: So James Webb— so the x-rays back
then are what today? NATARAJAN: They will still be x-rays. Because these are hard x-rays. TYSON: All right. So these are so x-ray-y— NATARAJAN: Yeah. TYSON: Can I use that word? NATARAJAN: That’s right. Yeah, sure. TYSON: They’re so x-ray-y that you can— NATARAJAN: You see through. TYSON: The red shift represented from the—
still puts them in the x-ray part of the spectrum. NATARAJAN: Yeah. Yeah........ TYSON: That just means we don’t have enough
words to divide up the x-ray part of the spectrum, it sounds like. NATARAJAN: Well, there’s hard and soft. So they’ve kind of— you know, hard x-rays
and soft x-rays. TYSON: Which has nothing to do with what they
feel like. [LAUGHTER] Does it have something to do with
how quickly they will kill you? NATARAJAN: Right. How energetic they are, right? How energetic. TYSON: Okay. So, I did not know that. So those are still within their zone. NATARAJAN: Yeah. TYSON: And look at the bias that we experience,
because we see visible light and we have, like, many words to describe all the colors
in this very tiny range of the electromagnetic spectrum. And out here, it’s just x-rays. That’s— NATARAJAN: Well, because, I mean, it’s—
we live in an anthropomorphic— you know, it’s all attuned to our retina, right? TYSON: Yeah. NATARAJAN: We can tell the difference. TYSON: I guess I’m okay with that, but I
just think about— I like words to be precise. NATARAJAN: So, I think one of the— this
is, you know, finding a black hole, a galaxy that’s harboring a black hole, seeing it
both with JWST and Chandra is a surefire indication that you have an actively-growing black hole. Because the complication is, if you don’t
see it in the x-rays, then you have to decode how much of the light is coming from the stars,
and how much is coming from the black hole. TYSON: Got it. Okay. So— NATARAJAN: There’s uncertainty there. TYSON: Let me restate what I think you just
said. If you had x-rays, it’s smoking gun for
black hole. NATARAJAN: Absolutely. TYSON: But x-rays are not a prerequisite for
a black hole. NATARAJAN: Yeah. TYSON: You can have a black hole that— where
the gas is not so hot that it’s going to be giving you x-rays. So then you have to somehow tease that information
out of the other— like, the spectrum or the— NATARAJAN: Yeah. Lines, the features that you see the spectrum. TYSON: Features in the spectrum. NATARAJAN: And the shape of the spectrum. TYSON: Okay. NATARAJAN: And that’s sort of an inherent
uncertainty. And the Chandra Space Telescope, given its
resolut—it’s a fantastic telescope. Given its resolution, it can't quite reach
the farthest edge of the universe, where JWST is reaching right now. So you need some clever tricks to be able
to— you have to look at some very special places in the universe, nature’s telescopes...... TYSON: You’re telling the public that you
perform tricks. In the research. NATARAJAN: Absolutely. TYSON: Okay. NATARAJAN: And magic. [LAUGHTER] TYSON: Okay. But I’m still trying to get to the bottom
of something here. Rachel, what— I’m still trying to understand. If we have galaxies in the dark ages, let’s
get back to— they’re not supposed to be there. So what has to give? Are the data— is there something wrong with
the data? Because that’s happened before. You know this. We’ve had— what, who can remind us of
this experiment, this measurement of the cosmic microwave background that— that was misinterpreted
by the authors? And then everybody saw, “Wow. There’s a new weird feature in the cosmic
microwave background. Let me come up with a theory to explain it.” And they came up with the theory to explain
it, and they were all— yeah. “Yeah, I’m a theorist, I got this.” And it turns out the interpretation of the
original paper was flawed, exposing ambulance-chasing theorists. [LAUGHTER] BOYLAN-KOLCHIN: So, this was the BICEP result. TYSON: BICEP, that’s an acronym. What was it— BOYLAN-KOLCHIN: So, I actually do not remember
what the acronym is. TYSON: Okay. FREEDMAN: It had to do with B-modes, I assume. TYSON: Say that again? Say again? FREEDMAN: It had to do with B-modes. So, going after gravitational waves in the
early universe. TYSON: Okay, B-mode. FREEDMAN: The signature in the microwave background. So what you have to really be careful of is
that there is also dust that causes polarization of the microwave background. TYSON: Dust in our own backyard. In our own galaxy. FREEDMAN: It can be in our own Milky Way galaxy,
that’s right. And so correcting for that is vital. And— TYSON: They didn’t do that correctly. FREEDMAN: Somebody actually read off a slide
at a meeting. This is the lesson. Don’t do that. TYSON: Okay. So— so— so that makes me wonder, do our
models correctly predict galaxies in the dark ages? JOHN [?]: Well, I think— TYSON: That’s a yes or a no question. JOHN [?]: Well, now, or earlier? No. So, my models wouldn't have predicted galaxies. And I don’t think anybody’s models really
predicted how much activity there was then. And so that’s really what people— TYSON: That’s a surprise. JOHN [?]: So I think that’s a surprise to
everybody. So that’s what Rachel was talking about,
that everything’s happening faster. It’s also what Wendy was talking about with
the metals appearing earlier. Everything is happening faster than we thought
in the early universe. And we need to figure out—....... TYSON: And metals are what our people call
anything heavier than helium on the periodic table of elements. JOHN [?]: That’s right. We have a very simple chemistry here. Hydrogen, helium, metals. TYSON: Yeah. So this kind of freaks out chemists when they
hear us speak to each other. JOHN [?]: Yes. TYSON: And we haven’t corrected that over
the decades. JOHN [?]: Not at all. TYSON: [LAUGHTER] Okay. BOYLAN-KOLCHIN: X, Y, and Z. TYSON: Yeah. Okay. So the metals— I interrupted you. I’m sorry. JOHN [?]: Oh, no. I was just saying that it all paints a consistent
and consistently new picture that things are happening faster than the models had previously
said. And we need to understand, is that something
that was missing in our models of how the galaxies are forming at early times? Or is it missing something in our picture
of how the universe was evolving at early times?. TYSON: So Rachel, what has to be adjusted? SOMERVILLE: Yeah. So I wanted to come back to the question you
were asking before about, how do we know our models are correct? Right? And because, as John said— TYSON: Right. Because just because they match doesn't mean
your parameters that went in are correct giving that result. SOMERVILLE: Exactly. TYSON: Because there could be ten other ways
you could put it together to get that result. You agree with that. SOMERVILLE: Exactly. I agree with that. WISE: Yes. BOYLAN-KOLCHIN: Yeah, I agree. TYSON: Good. SOMERVILLE: I think we all agree with that,
absolutely. But the problem is that, especially these
computational models, are very expensive. So you can't run them 1000 times to explore
that large parameter space and see if those degeneracies that you’re talking about are
present. So what was traditional— TYSON: So degeneracy is when two different
models give the same result. So we say those inputs are degenerate to each
other. SOMERVILLE: Correct. TYSON: That’s an interesting word in our
field, to reference that. SOMERVILLE: Yes. Exactly. TYSON: Okay, go on. SOMERVILLE: Yes. TYSON: It has nothing to do with their moral
[LAUGHTER] — SOMERVILLE: Thank you for clarifying. TYSON: Yeah, yeah. I just— SOMERVILLE: We don’t want to get in trouble
here. TYSON: Yeah. Yeah, yeah. Degenerate computer simulations. Yeah, okay. What are you calculating? Right. All right. Okay. SOMERVILLE: So what everyone— what most
people did was to take the nearby universe, where we had lots of observations. We think we know how star formation works. We think we know how, you know, when supernova
explode, how do they affect the next generation of stars? We even know a little bit about how black
holes affect galaxies. TYSON: And we have multiple telescopes working
on it. SOMERVILLE: We have many telescopes, we have
lots of activity. TYSON: It’s nearby. It’s resolved. Everything. SOMERVILLE: Exactly. So we turned all the knobs in our models to
match the nearby universe. And then, at least what many groups did, what
my group did, was to say, “Well, what if we now take those models where all our knobs
are fixed to match the nearby universe, and we predict what James Webb should see?” And you were accusing us of never publishing
papers that disagree with the observations. Well, we did. We published a paper before Webb launched
predicting what it should see. And we disagreed with the observations, right? So we learned something. We learned that the physics we put into our
models— TYSON: You learned that you were wrong. SOMERVILLE: We learned that we were wrong. Which is fantastic, right? That’s science. TYSON: Okay. So— yeah, that’s definitely science. So, but you’re wrong in an interesting way. SOMERVILLE: In an interesting way. TYSON: Yes. So— so, not to deliver your punchline. But that tells you that either James Webb
is flawed in their data its reporting, or you cannot backstrapolate to the early universe. from parameter of the galaxies that are nearby. SOMERVILLE: Or maybe you have to do it in
a smarter way. Right? So, one of the things that we’ve realized
recently is that the environments that are common in the nearby universe. are not typical of the early universe at all. So it’s maybe as though you tried to extrapolate
from New York City, you know, properties of the Sahara Desert, or something. Right? Of course you would get it wrong. So you need to look for environments in the
nearby universe that are similar to the early universe. And what was different in the early universe? It was much denser. Right? So there might be various differences. It was much denser, there were fewer heavy
elements. TYSON: Well, just to be clear, it was denser
because all the same matter was in a smaller volume. SOMERVILLE: Exactly. The universe has been expanding all this time. That means it was much denser in the past. TYSON: And in fact, redshift 11— which I
think is around— to now, how much has the universe. expanded, over redshift 11 to today? NATARAJAN: By a factor of— how do I put
it? TYSON: Is it just linear? Is it just linear? I think it’s just linear. BOYLAN-KOLCHIN: Yeah, just linear. NATARAJAN: Yeah, it’s just linear. TYSON: So it’s either ten times bigger,
11 times bigger, 12. NATARAJAN: Well, yeah, 12 times. TYSON: Oh, plus one. NATARAJAN: Plus one, yes. TYSON: Plus one in the equation. I just remembered that. So— so ten times. So it’s ten times denser back then. SOMERVILLE: Exactly. TYSON: Got you. Okay. SOMERVILLE: Okay. NATARAJAN: Ten to three. Ten to the three times. Its density is over volume. TYSON: Oh, cubed. Oh, excuse me. SOMERVILLE: It’s the cubed. NATARAJAN: Cubed. SOMERVILLE: So it’s thousands of times denser. NATARAJAN: Yeah. TYSON: Got it. SOMERVILLE: Right? TYSON: Ten times ten times ten. SOMERVILLE: So actually, if you look at how
stars form in those kinds of environments, which are rare today— TYSON: But you can find them. SOMERVILLE: You can find them. Star formation is much more efficient. And if we put that into our models, then we
actually reproduce the Webb observations. TYSON: Oh. SOMERVILLE: And we predict that there should
be many more bright galaxies even further away, even at higher redshifts. TYSON: Ooh. So in hindsight, you could have actually predicted
the right answer. SOMERVILLE: That’s the frustrating thing. TYSON: Yeah. [LAUGHTER] 'Cause— I was once dining with
Stephen Hawking, and I asked him a question. Takes him a while to process your question
and then type it out with his blinking eyes, okay. So I asked him a question about, why didn’t
Einstein predict black holes, which come right out of his general theory of relativity. And so, like, it took about ten minutes, and
then the answer came back. “You can't think of everything.” [LAUGHTER] It was like, “Wow. Okay. That’s good.” You can't— and he would be thinking of you. You can't think of everything in that moment. So were you going to say something here? Because I’m going to match you with another
question. Yeah. WISE: Yeah. There is a— oh, like, you’re talking to—... TYSON: No, you. Yeah, John. WISE: Okay. Yeah. So I think another difference in the early
universe is that there were no stars in the galaxy. There was no galaxy. So you have all this gas coming into a dark
matter halo. And it has nothing to compete with. So you get this huge burst of star formation,
and otherwise, if you compare it to, like, today, there’s already all this star formation
that’s going on. Supernova going on. But this was a pristine environment. TYSON: Just a quick question. Priya, the dark matter, he just said it’s
in a dark matter halo. NATARAJAN: Yeah. TYSON: So is dark matter running the show
back then? NATARAJAN: Yeah. It’s in the driving seat. Basically, this dark matter, which is about
20, 25 percent of the overall inventory of the universe, provides the entire scaffolding
in which you form galaxies, all of this gas gets collected, black holes form. This was sort of the cradles where everything
really happens. TYSON: But Priya, you don’t know what dark
matter is. NATARAJAN: Precisely. When I say don’t know what it is, we know
how it manifests. That’s the crazy thing about both dark matter
and dark energy. We don’t know what they are, fundamentally. Like, for dark matter, we don’t know what
particle is a dark matter particle. We’ve been looking for it for decades. TYSON: If it is a particle at all. NATARAJAN: At all. And similarly for dark energy, we don’t
know its nature. But we know exactly how they manifest in the
universe. TYSON: So you get to put it in your models. NATARAJAN: Absolutely. Yeah. TYSON: Okay. Wendy, when you’re calculating the age of
the universe, and the galaxies near and far, does dark matter matter? FREEDMAN: Oh, yeah. I mean, this— TYSON: In what way does it show up in your
calculations? Or, and dark energy, even? FREEDMAN: Yeah. If you’re going to study the expansion of
the universe, it’s changed over time, and it’s reacting to the presence of dark matter
and dark energy. And it folds into the age. If you’re going to determine the age, you
need to know. TYSON: So maybe your wrong age— sorry. [LAUGHTER] Michael. Maybe your age is different because you’re
not properly modeling the dark matter and dark energy? FREEDMAN: So— TYSON: Is that possible?. FREEDMAN: Okay. So step back. What we’re measuring is the— when we’re
measuring the Hubble Constant, we’re measuring the Hubble Constant at the current time, the
current epoch. So we don’t need to know. We don’t need to know that model. But when we’re comparing with the observations
from the early universe, the microwave background observations, that— TYSON: That’s the whole other method coming
in from the back door. FREEDMAN: The whole other method. It fits these tiny little differences in the
temperature of the background radiation, and it fits exquisitely well the standard model
that includes dark matter and dark energy. And so the current tension is between the
fit of this standard model, which predicts what the expansion rate would be today—
it’s a predictive model, will tell us what the expansion rate would be today— given
the amount. of dark matter and dark energy, and what we
see locally. So that’s where it comes in, that possibly,
if both are right, we’re learning something about the standard model. Something fundamental is missing in our current
picture. That’s why it could be very interesting. TYSON: Michael, this sounds pretty tight,
what she’s describing here. BOYLAN-KOLCHIN: That’s right. So I think that actually makes this really
appealing, because it means that there’s not much space to look. We really know what we need to do. TYSON: You really— something’s really
wrong. BOYLAN-KOLCHIN: So, something is really wrong,
and if it’s going to be something that’s cosmological, if we need to change something
in the cosmological model, we know exactly what it kind of has to look like. It has to be some kind of energy that is like
dark energy today but happens just before the microwave background. TYSON: Wait, you’re inventing some other
thing we don’t know anything about? BOYLAN-KOLCHIN: Well, once you— FREEDMAN: We’ve tried everything. We tried everything, and nothing worked. BOYLAN-KOLCHIN: Once you’ve got dark matter
and dark energy, you might as well get a third one, right? [LAUGHTER] No. It’s— but I think that’s what— TYSON: But wait. You’re pulling this out of where? BOYLAN-KOLCHIN: Well, but that’s— I think
that’s the amazing thing, right? Like Priya was saying, we haven’t detected
dark matter directly. We haven’t detected dark energy. But we know so much about observations of
the universe from the earliest times to today, that we can say, “This is how they have
to behave.” So what we’re saying is, the only way out
if it’s not something with our models of galaxies, is observation—. TYSON: Is get another thing that we don’t
know anything about...... BOYLAN-KOLCHIN: That’s right. And we should be able to know if it’s there
or not within the next year or two from observation. NATARAJAN: That’s generally— TYSON: Wait. Priya, what is he saying/ NATARAJAN: I think he— no, no. I think he’s saying the absolutely right
thing. So basically, dark matter and dark energy
set the clock of the universe. So if the setting— if there’s something
different about them, the clock is different. It ticks faster in the early universe, maybe,
slower, later, or vice versa. So if dark energy could be changing with time,
that allows for a clock that is different, that moves and runs differently. And therefore, all the action that happens
in the universe will happen at a different pace. TYSON: He’s saying there’s a whole other
mysterious— you’re adjusting the behavior of dark matter, dark energy, over time, possibly
to explain the discrepancy. NATARAJAN: That’s the first, simplest thing
we can do. TYSON: But Michael is just pulling something
s else out of the ether. BOYLAN-KOLCHIN: That’s kind of you to put
it that way. NATARAJAN: Yeah, right. That is ether. FREEDMAN: But the beauty of all this is that
it’s testable, right? NATARAJAN: Yes. FREEDMAN: If this is correct, it will show
up. And it may show up in the next generation
of microwave background experiments. There’s a prediction. If there is this early dark energy, you’re
going to see a fairly whopping signal. TYSON: Let me jump back a little bit of history
here. Priya, you also studied history of science
and philosophy. In the history of science, there have been
many examples of a prediction of something that kind of had to be there, because first
it was a good theoretical model for it, but also— what am I thinking of? I’m thinking of neutrinos, for example. They were predicted because something else
was happening in the experiment. NATARAJAN: There was a missing energy. TYSON: A missing— NATARAJAN: Energy. TYSON: There was a missing thing. And they said, there’s some mysterious particle
that is nearly impossible to detect, that we invented to explain what happened. And sure enough, it existed. NATARAJAN: Yeah. I think we have these wonderful laws, right? TYSON: Okay. So that means I’ve got to agree with Michael? NATARAJAN: Yeah. I think, you know, all possibilities are open,
right? So the fact that we have conservation laws,
conservation of energy, allowed us to infer the presence of this dark energy. TYSON: Of the neutrino. Yes. NATARAJAN: Right? And I think similarly, it’s quite possible
that it’s going to be the data that is going to show us the way. Right? So future date, better data, more accurate
data, will really show us the way in terms of what are these specific models? There’s tons of models. TYSON: So the James Webb Space Telescope is
not good enough for you. You need another telescope. NATARAJAN: I want more. I want more. FREEDMAN: It’s pretty good. It’s pretty good. NATARAJAN: It’s pretty good, but we want
more. TYSON: This is a tough crowd, I’ll tell
you, here. So John, you say you used super duper computers. Sorry. Just supercomputers? NATARAJAN: Yeah. WISE: I wish I could call it super duper computers. TYSON: I mean, supercomputer has been a term
for the last 40 years, ever since computers got good. WISE: Yeah. TYSON: And at any given moment, there’s
the supercomputer of the year. Is there something you can imagine you would
do with a computer that’s ten or 100 times or 1000 times more powerful than what you
have right now? And of course I’m thinking of quantum computing. It’s still a little bit of a pipe dream,
but what— what simulation is out of reach to you now, that you can't wait to get a super-duper
computer applied to it? WISE: So, I think our problem in cosmology
and galaxy formation is just the disparate length scales that are involved with galaxy
formation. Right? We have everything from the quantum scale,
atomic scale, all the way up to cosmology, in which we have to model. TYSON: And it all matters at some level in
what you’re creating. WISE: That’s right. So you have— even if you want to study how
stars form in the cosmological volume, that’s still huge orders of magnitude difference
in between that. And that’s what takes a lot of time. If I had a computer that was 1000, million
times faster, we could get more statistics. But I think it really takes person power to
actually utilize those supercomputers. Like, we need algorithms and people to actually
write efficient code to use, like millions of computer cores. TYSON: Just get AI to do it. WISE: And yes, I’m very excited with AI. But not— maybe to help the code a little
bit. But to actually use, say— I know, this is
probably when I’ll retire. But if AI and quantum computing could come
together, maybe that will cause us to actually simulate a lot. But— TYSON: You just don’t want it to achieve
consciousness, because then we’re— WISE: Yeah. I don’t want Skynet. TYSON: So I’m intrigued by that. I’m going to repeat, if I understood what
you said. You have to model things on the atomic scale,
or quantum scale, and on the largest cosmological scale. And to do that— NATARAJAN: Simultaneously. TYSON: Simultaneously. Good. So the computer has to know what every atom
is doing in every star in every galaxy. WISE: In principle, yes. NATARAJAN: Yes. We black box it now. WISE: You know, we can't do that, so we have
to have approximation. These are these knobs that we tune......... NATARAJAN: Yeah. TYSON: Okay. So you make approximations. You say, “I think this many atoms in this
volume will have this sort of macroscopic property.” WISE: That’s right. So what I think is to have AI turn the knobs
for us, to actually look for that solution, to— so these are called emulators. It emulates physics. And that’s what we’re basically doing. So we have some physical model. It has to be grounded in fundamental physics,
these AI emulators. But I think once we grapple with that and
make those produce realistic and fundamentally physical results, I think that will be a huge
steppingstone. TYSON: Yeah. Because I remember at any given time that
I plugged in the computer, I always wanted it to be faster than what it was delivering
for me. WISE: Yeah. TYSON: Every time I ever did it, I say, “All
right. I’ll make do with this.” So I felt very greedy at the time. Especially since, you know, my iPhone has
a million times the power of the computer I used back when I was coming up. So we’re just greedy. WISE: Yeah. And now, like— you know, we have— NATARAJAN: Eternally greedy. TYSON: Eternally greedy. Okay. NATARAJAN: I think so, yeah. WISE: And NSF, NASA, they have these huge
computers, but big tech actually outweighs how much computing they actually have, in
generating and training their AI models. TYSON: Okay. WISE: Yeah. So we can partner with them, maybe. TYSON: You see the smile on his face as he
talks about this? Beams of light. WISE: I’m an AI optimism. TYSON: Yeah. It is true, in our field, we love us some
AI, because it makes our jobs easier. It’s the rest of the country that’s just
freaking out. NATARAJAN: Right. TYSON: When journalists found out that AI
could write their articles, out came the headlines, “AI is bad.” WISE: Or make videos now. TYSON: Yeah. Yeah. Yeah. Just wondering. So Michael, let’s go back to your version
of Priya’s, “We need to modify dark matter, dark energy.” You’re going to invent this new other thing
we don’t know anything about. BOYLAN-KOLCHIN: Yeah. TYSON: To account for this. And you feel sure that would reconcile these
two ages. BOYLAN-KOLCHIN: Well— TYSON: Will it bring your number to Wendy’s,
or Wendy’s number to yours? BOYLAN-KOLCHIN: So, that would bring the microwave
background number closer to Wendy’s number. So Wendy would have been right. Yeah. And— but I think— you know— TYSON: I’m going with Wendy on this, just,
I’m saying. BOYLAN-KOLCHIN: Yeah. There you go. TYSON: She’s got more data than you do. [LAUGHTER]la BOYLAN-KOLCHIN: And I think one reason that
we might think this is something interesting to do based on the James Webb observations
is that that same model can predict earlier structure formation. It can help replicate those observations that
we’re seeing in the early universe. And so that’s one reason people find that
to be an attractive model. It was predicted to match up these measurements
of the expansion rate. That was why it was proposed. But it turns out one side effect is that things
happen faster in the early universe, which is exactly what the observations were. And so that’s— you know, like you say,
you don’t want to just invent things to match one observation. But if you invent one thing and it matches
two disparate observations, then you start to think maybe you’re onto something. So it definitely doesn't have to be this. But it leads us to think more about it, I
believe. TYSON: And Priya would agree, there’s plenty
of precedent for just that kind of thing in the history of science. NATARAJAN: Absolutely. And I think as Michael said, one thing we
want to do, there’s some other tensions that are there on very small scales, within
galaxies. The way a matter is heaped in the centers
of galaxies, where all the action is where the supermassive black hole is sitting, and
so on. There’s some tensions with observations. Some have come and gone, and some have stayed. And that model would actually help out some
of them as well. So you could have one little tweak in the
model at very early times, that could actually resolve and bring into harmony many more observations. TYSON: And that gives you huge confidence
that you’re doing the right thing. If it brings into harmony multiply disparate
observations. NATARAJAN: And makes an additional prediction
that can be further tested. Then I’d be a lot happier. TYSON: Because otherwise, you’re making
a post-diction, which is less— NATARAJAN: Less powerful from— TYSON: Less powerful. NATARAJAN: Yeah. BOYLAN-KOLCHIN: Right. TYSON: As Rachel made a post-diction. Atone for this, Rachel. [LAUGHTER] SOMERVILLE: I think it’s important to point
out, too— I mean, some of these models have— they don’t solve both tensions at once. NATARAJAN: Absolutely. SOMERVILLE: They go in the opposite direction.......... NATARAJAN: They go in the opposite direction. SOMERVILLE: And there are also examples from
history where the effects that you see come and go, right? Which is why we have to be very careful to
understand, is this something that’s real, or have we missed something in the observation? NATARAJAN: To just clarify that, as theorists,
right, we always know how to stay in business. So there’s a landscape of models. And, you know, they’re— TYSON: Like I said, ambulance-chasing theorists. Always have got some— WISE: Looking right at me. I remember this very well. TYSON: I was right on your shoulder when I
said that, wasn’t I? WISE: Yeah. SOMERVILLE: But this is, I think, a place
where JWST is going to help us. NATARAJAN: Yes. SOMERVILLE: Because I think we’re getting
to the point where we’re gonna learn something very interesting about whether this is real
or not, and it’s the higher resolution of James Webb, and the higher sensitivity, particularly
in the infrared, and the ability to make these measurements in more than one way, is going
to shed light on this. NATARAJAN: Right. I think multiple, independent lines of evidence,
really, is going to help resolve these tensions. SOMERVILLE: Right. Right. Yeah. TYSON: Let me begin to land this plane that
we’re flying right now. So Wendy, you’re deeply involved in a new
telescope. A Magellan Telescope, one of the most powerful
telescopes the world will have seen. Can you just give me just a brief overview
of that? I’ve read a little bit about it, but I don't
know, why do you need another telescope? [LAUGHTER]a FREEDMAN: Well, we’ve established— TYSON: Hubble wasn’t enough for you, and
you need another telescope. FREEDMAN: Yeah. We’ve established that astronomers are greedy. We want more computing power, and we need
more light. And so when we’re looking at faint objects
or we’re trying to see detail in objects where we need high resolution, then we need
a bigger telescope to do that. So there are three big telescopes that are
being planned in the world right now, and Giant Magellan is one of those. TYSON: That’s the one you’re involved
in. FREEDMAN: Yes. So I led that project. I was the founding leader from 2003 to 2015. And it will be built in the Andes Mountains
in Chile, and it’s— TYSON: Fourteen thousand feet kind of— FREEDMAN: No. No, about 8500 feet. TYSON: Oh. Okay. FREEDMAN: It’s not one of the high-altitude
sites, because it’s optimized for optical. And near-infrared. And it is made— there are seven mirrors
in this telescope. Each one is 8.4 meters in diameter. So there are six in a circle, one in the center,
and the overall resolution is as if it were for a 25-meter telescope. So this is an international collaboration. ...
TYSON: So it’s cheating a little bit, because when we think of the resolution of a telescope,
the bigger the telescope, the higher the resolution. But if it’s one mirror, that’s very hard
to make. So you’re saying, “I’m just going to
make a bunch of little, smaller mirrors.” FREEDMAN: Little. Twenty-seven feet in diameter. Little, yeah. BOYLAN-KOLCHIN: And each of these mirrors
is bigger than James Webb’s mirror. FREEDMAN: Yeah. BOYLAN-KOLCHIN: Each of them. WISE: Yeah. TYSON: Each is bigger than the entirety— BOYLAN-KOLCHIN: The entire James Webb mirror. FREEDMAN: Yes. So, why do we need a bigger telescope? It will have four times the resolution of
James Webb. TYSON: Right. So by the pieces that you’re assembling,
you bring them together in software, or cleverly, and it simulates what would be a single mirror
of that diameter, 25 meters. FREEDMAN: Right. Correct. TYSON: That’s like the size of this— FREEDMAN: It’s, you know, this auditorium. Yeah. It’s a big, big telescope. TYSON: This is huge. FREEDMAN: Yes. TYSON: What are you going to look at with
it? [LAUGHTER] FREEDMAN: Well, we’re going to learn more
about the early universe. We’ve got better resolution and high sensitivity. This telescope will collect a lot of photons. It will tell us, again, about the expansion
rate locally. We’ll be able to go out farther with this
higher resolution and find these variable stars and so on. TYSON: So then what do you need James Webb
for? FREEDMAN: James Webb— so, there are different
things that you can test with different kinds of telescopes. Its infrared sensitivity gets beyond the dust. So, dust makes things look fainter and farther
away. TYSON: So, the— Webb. FREEDMAN: Webb. TYSON: And yours? FREEDMAN: This is optical. TYSON: Optical. So it’s just what— it’s red, orange,
yellow, green, blue, violet. Got it. Got it. FREEDMAN: It’s like Hubble. Right. Right.... TYSON: It’s just a really badass regular
telescope. FREEDMAN: Correct. TYSON: Okay. WISE: They should call it that, yeah. Might be a better name, yeah. SOMERVILLE: And you also have to deal with
the atmosphere, right? So you have to correct for the blurring of
the atmosphere. FREEDMAN: That’s right, yeah. SOMERVILLE: But we think that we can do that. FREEDMAN: But we know how to do that now. TYSON: And it’s named Magellan, because
he hung out in the Southern hemisphere. It’s just a Southern hemisphere telescope? FREEDMAN: It is a Southern hemisphere telescope,
that’s right. That’s right. So— and, you know, exoplanets— we’re
not talking about that tonight, but you’ll have high enough resolution and sensitivity
that you can actually look at the atmospheres of planets and look for biosignatures. Oxygen, methane. TYSON: That’s a whole other thing we’re
going to do. FREEDMAN: Yeah. Whole other. TYSON: Biomarkers, yeah. FREEDMAN: So, lots more to do. We’re not solving all of the problems tonight. You probably couldn't tell that. There’s stuff left to do. TYSON: Exo— and exoplanets. Never-ending, what it is. So Priya, what’s your philosophical view
on— are we ready, is there some paradigm shift? We’ve heard that term before in our understanding
of the early universe. What, of these headlines— “Oh. Astronomers have to go back to the drawing
board and might have to re-think the Big Bang.” Is this not one of those cases, and that’s
just clickbait? NATARAJAN: Yeah. I think we don’t have to re-think the Big
Bang. But there are details about our models that
we don’t really understand. And as Rachel pointed— as all of us have
talked about— TYSON: But that doesn't make good clickbait
on the internet. NATARAJAN: Right. But I mean, we— TYSON: “There are some details of their
models they don’t understand.” NATARAJAN: No, no, but we are in the midst
of a revolution in terms of data. So I think it’s a new kind of revolution
that we have not seen before, where we have overabundance— no scarcity of data. So there’s a lot of data. Actually, a deluge. Which really restricts the job of theorists. We can no longer sit on a fence and say, “Well,
maybe it can be this, maybe it can be that.” TYSON: The data is constraining you. NATARAJAN: Very tightly— soon, it’s going
to start really tightly constraining the models, and hence, our theoretical understanding. TYSON: Well, that’s a good thing. That’s a good problem. NATARAJAN: Absolutely. Absolutely. Good problem to have. TYSON: It’ll give John less latitude and
he’ll have less fun at the computer, but it’ll bring him in line. NATARAJAN: Yes. No, but then remember we always also have
this additional challenge of the storyline. So we need a self-consistent unfolding of
all these elements over time. Dark matter— TYSON: That can't be overstated here. Because you can fit something then. NATARAJAN: Exactly. TYSON: You can fit something now. And if the arc does not work, go home. NATARAJAN: Yeah. Absolutely. It’s not good enough. TYSON: Okay. Rachel, why is it that— I also saw, in headlines,
the universe might be twice as old as people previously thought. Who’s saying that? What is that? Do you remember those headlines? Michael? FREEDMAN: The Big Bang was wrong too, remember. BOYLAN-KOLCHIN: Yeah. So there’s— there is somebody who wrote
a paper on this recently, and what he’s done is, he’s changed— TYSON: When you say “paper” you mean a
research paper that was peer-reviewed? BOYLAN-KOLCHIN: Two peer-reviewed research
papers. And they argue that we really do need a fundamental
revolution. Not the Big Bang itself, but in our understanding
of the matter and the energy content. So he does away with dark energy, he does
away with dark matter. But he says that light behaves differently
than what we think. And the fundamental constants of nature that
we think are constants are now not constants. So now they’re the fundamental variables
of nature, or whatever. They change with time. TYSON: Okay. So he’s doing what you’re doing, John? He’s saying, “Let’s turn the fundamental
constants into knobs.” NATARAJAN: Yes. TYSON: And let’s turn the— WISE: That brings fear into my heart. [LAUGHTER] TYSON: Yeah. Let’s turn those into knobs and adjust those
and see if you can fit things. BOYLAN-KOLCHIN: That’s right. And so that, he is claiming based on these
early galaxies from James Webb Space Telescope, that that model fits the data better. But I think that there are a lot of— there’s
a lot of other data out there. This model would not fit that as well. And one of the things that we see around us—
so, this model would predict the universe. is 26.7 billion years old, as you’ve said. TYSON: So that’s these headlines that must
have been going around. BOYLAN-KOLCHIN: That’s right. But we can measure the ages of the oldest
objects in the universe. And we’ve been doing— this is how— TYSON: It’s definitely not 27 billion. BOYLAN-KOLCHIN: They’re not 27 billion years
old. They’re very consistent with this 13, 14
billion years. TYSON: Is this a physicist who knew no astronomy,
who published this? Why did it get published? BOYLAN-KOLCHIN: Well, you know, I think it’s
a good thing, to be honest. The clickbait headlines, maybe less good. But I think that our models are best when
they’re tested the most severely, right? And so they can take it. Right? If the model’s right, it doesn't— somebody
can throw this at it, and we’ll find a hole in their model and the current model will
be right. If the current model is wrong, then we’ll
find the holes there. TYSON: Wouldn’t the— wouldn't the peer
reviewer have said, if the universe. is 27 billion years old, we would have found
something older than 13.8, 13.7 billion. FREEDMAN: Give or take. TYSON: And there’s nothing in the universe
that old. So the universe spent half its life making
nothing? BOYLAN-KOLCHIN: Well, I think that certainly
some peer reviewers would have said that. And you could say that any peer reviewer could
have caught that. But the domain expertise— you need to know
lots of different pieces here sometimes. And its just not possible for some people
to know everything. TYSON: You can't know everything. NATARAJAN: But also, we are open to speculation,
as scientists. Right? I mean, our understanding is provisional,
given what we know at the moment. So we are open to speculation. So if it resolves a problem— TYSON: I’m all with you on that. But aren’t there people, cottage industries,
that test the stability of the constants over time? NATARAJAN: Yeah. Yes. TYSON: There’s a whole industry of people
who do this. BOYLAN-KOLCHIN: As a peer reviewer, then you’d
ask, “Why do you believe this is not the case?” And we would ask the authors to put it in
their discussion, saying, “Prove this is the case.” NATARAJAN: Yeah. The caveats. BOYLAN-KOLCHIN: The caveats. TYSON: Yeah. Okay. All right. Well, I just—. I follow what people do with the physical
constants. And it’s remarkable that— let’s go back,
not to be too historical here. But after Newton’s laws of gravity were
established, and it explained our moon going around Earth, and Earth going around the sun,
it also explained Jupiter’s moons going around Jupiter. That was— no one saw that coming, unless
he was onto something, quote, “universal”. Then, maybe it only works in our own solar
system. Must it work around other stars? So when the first binary star system was discovered,
it also fit Newton’s laws of gravity. And so we’ve been systematically testing
the applicability of the laws of physics that— so we’re not just hoping that it persists
through time and across space. We have good evidence for this. BOYLAN-KOLCHIN: Well, and not only that, it
allowed us to predict the existence of Neptune. “Us” is not me. It was a long time ago. But, you know. TYSON: [LAUGHTER] Oh, you weren’t there? BOYLAN-KOLCHIN: Yeah, yeah. Almost that old. In the 1800s, you know, Neptune, or Uranus,
had a little bit of a wobble in its orbit that people couldn't explain from Newton’s
laws, unless there was another body there. TYSON: Oh, that’s right. Exactly right. Because when Uranus wasn’t following Newton’s
laws either, they found the limit of Newton’s laws in the universe, the distance beyond
which it no longer applies. That’s like your people changing the laws
of— or, hypothesize another object whose gravity you have not factored into computing
the orbit of Uranus. BOYLAN-KOLCHIN: Exactly. Exactly. WENDY [?]: Well, and to go further, you’re
going to talk about Mercury. I mean, the orbit of Mercury didn’t fit.. NATARAJAN: Exactly. FREEDMAN: And the question was, is there another
planet somewhere that’s perturbing Mercury? NATARAJAN: Right. And they thought it was Vulcan, right? FREEDMAN: Right. And it turns out—. TYSON: Yeah, invented Vulcan. They pulled that out of their ether. NATARAJAN: But then you needed— FREEDMAN: It was a reasonable hypothesis,
and it was wrong, right? And then it was—. BOYLAN-KOLCHIN: And that was a problem with
Newton’s laws. FREEDMAN: Right. And it was one of the things that— TYSON: And that was new physics. NATARAJAN: Exactly. You needed a fundamental rethinking of gravity
itself. And that’s where Einstein’s theory of
general relativity comes in. TYSON: So, has this other paper caught on
with the— BOYLAN-KOLCHIN: With the press, yes. [LAUGHTER] With scientists, I think— RACHEL [?]: But I’d never heard about it. So that tells you something. WISE: I haven’t heard about it either. WENDY [?]: Yeah, I’ve seen it.. TYSON: Okay. BOYLAN-KOLCHIN: I get a lot of e-mails saying,
“Mike, what’s going on here?” TYSON: All right. Let’s now land this plane. If I could just get some final reflections
on various topics. You mentioned the Chandra Space Telescope. This is one of the— NATARAJAN: Flagship missions of NASA. TYSON: — flagship missions of NASA, as was
Hubble. NATARAJAN: Yeah. TYSON: And there’s the Spitzer Telescope. Each one has a specialty. We just learned days ago that the Chandra
Telescope will likely have its budget zeroed— NATARAJAN: Within two years. TYSON: — within two years. And they will have no access to the x-ray
universe. NATARAJAN: We will lose our x-ray eyes into
the universe, which I think is a disaster. And the telescope is working. I think it should be funded for a little bit
longer. The idea was to phase it out as it starts
to make— ..
TYSON: And bring somethings else up! NATARAJAN: Yeah. TYSON: But we’re not bringing anything else
up. NATARAJAN: Well, there are plans. There’s been a call, and there have been
people who’ve put in proposals for other x-ray telescopes. And the Europeans are putting up an x-ray
telescope called Athena. TYSON: Athena? NATARAJAN: Athena. And— TYSON: Well, I wish you well there. I mean, that’s a tough time. I mean, the telescope is 25 years old. That’s— but if it’s still working and
we’ve got nothing else, we’ll be out of the game. NATARAJAN: Yeah. And more importantly, I think we need something
to bridge, to kind of bridge our view into the x-ray universe. Because one thing that we haven’t yet discovered,
right, which is something I want to happen before I die— well, I hope I don’t die
that fast— is the LISA Mission. The gravitational wave detection from the
collision of two supermassive black holes. We’ve detected the collision of two stellar-mass
black holes, the LIGO, the apparatus on the ground that made this discovery. The supermassive black holes also collide. And that will happen in the 2030s. We definitely need some instrument to be looking
at the universe with x-ray eyes continuously ‘til then, because the supermassive black
holes, just before they merge, and that sort of burst of gravitational waste comes out,
there’s a lot of action in the x-ray that happens beforehand. TYSON: You can predict that. NATARAJAN: Yeah. TYSON: So these two colliding supermassive
black holes would be the consequence of two galaxies colliding, and they each have their
own supermassive black hole. And they’ll probably find each other. NATARAJAN: Yeah. TYSON: Given the dynamics of this. Okay. NATARAJAN: And in that process, there’ll
be a lot of crud. All the gas and the stuff would be mixed up,
and we should be able to see it in the x-rays. TYSON: “Crud”, is that an official word? Okay. [LAUGHTER] John, you were beaming when you
were reflecting on AI and quantum computing, and supercomputers. You were like a little kid, right, in your
enthusiasm for that. How soon do you think that will be with us?.. WISE: So, AI, we’re in the midst of that
revolution right now. TYSON: Definitely. But the computing power? WISE: The computing power? I mean, I think we’re still— the hardware
is still ramping up. But it really takes people to develop those
algorithms, and to make the computer code, the simulation code, to fully use the computers
efficiently. TYSON: So we need more coders out there. WISE: Yes, yeah. TYSON: To come up in the ranks. WISE: And most students, they are good coders. But to actually use these supercomputers at
that scale requires a different level of thinking. Of how to distribute that work among a million
cores, right? I mean, a computer— imagine if you had a
million computers. How do you split up the work and make them
talk together on the order of, like, nanoseconds, and just march forward? TYSON: A billionth of a second. WISE: Yes. TYSON: Yes. WISE: A billionth of a second. TYSON: Why not a picosecond? Why not an attosecond? Why limit yourself? [LAUGHTER] That’s like, I’m old enough
to remember, if your computer had megabytes of storage, that— people lined up to look
at that. WISE: I think— because chips, right? When you look at how quickly the frequency
of the chips are, they’re in gigahertz. So you take an inverse of that, and that’s
nanohertz. Or, sorry, nanoseconds. So that’s the amount of time it takes for
a computer to, say, do one operation. So it’s not going to take— TYSON: Today. WISE: Today. But that requires a lot of power. And you have to dissipate the power. So it’s not going to come, I don't think,
anytime, any quicker than that. But we can do many more synchronous operations. TYSON: Rachel, at the CCA, what are your next
projects there? Are you done with James Webb, or is there
more data you’re waiting for or you’re going to direct it to do? SOMERVILLE: Oh, James Webb is absolutely not
done. That’s the exciting thing. So it turns out that originally, Webb was
spec’d to last for five years. But the launch went so beautifully that we
now are hopeful that Webb may last for ten years, maybe even longer. Maybe even up to 20 years. TYSON: What would— I thought it’s passively
cold, so what is it you would run out— oh, is it the stability of its orbit? SOMERVILLE: It’s keeping— exactly. It’s keeping the orbit stable. Otherwise, it will drift away, and we would
eventually lose the ability to communicate with it. So we need to keep in that nice orbit close
enough to the Earth that we can— TYSON: Let’s just— I know it’s a million
miles away, but let’s just go there and drag it back where it should— it’s supposed
to be! SOMERVILLE: Right. So, there are so many things that we would
love to do with this telescope. TYSON: Because unlike Hubble, you can't service
Webb. SOMERVILLE: Yep. Probably not. TYSON: I’m sorry. Unlike Hubble— SOMERVILLE: Not right now. Humans. TYSON: No one’s going a million miles from
Earth. SOMERVILLE: Humans cannot service Webb. It’s possible we might be able to send a
robotic mission to service Webb, eventually. TYSON: To drag it back where it’s supposed
to be. SOMERVILLE: So, there are some people who
are thinking about that. TYSON: Okay. SOMERVILLE: But we want to look at much larger
areas of the sky. We’ve only looked at very small patches
of the sky, and some of these things we’re seeing could just be flukes. We want to go much deeper than we predict
that we should see many more objects that are even further away. TYSON: With the new models that take you there. SOMERVILLE: As the models predict. And we want to get many more spectra, which
will allow us to tell how many heavy elements there are, are there hidden black holes? TYSON: You can say “metals”. We’ve been through that. SOMERVILLE: Yes. TYSON: How many metals there are. [LAUGHTER] Yeah. SOMERVILLE: We speak the lingo. We should be able to see the signatures of
the growing black holes. So there’s many, many exciting results ahead. TYSON: Beautiful. With that new understanding. Very cool. Well, keep at it. And you’re full time there now. Formerly at Rutgers, New Jersey. SOMERVILLE: Right. TYSON: So welcome to Manhattan. SOMERVILLE: Thank you. TYSON: Flatiron Institute, because it’s
in the area of the Flatiron Building, which is right there at 23rd and Broadway. SOMERVILLE: Twenty-third and Broadway is the
Flatiron building, but our building is actually at 21st. TYSON: Well, it’s the Flatiron District,
that’s why you got it— SOMERVILLE: Correct. TYSON: Okay. Well, welcome to town for that. SOMERVILLE: Thank you. TYSON: So, Michael. BOYLAN-KOLCHIN: Yes, sir. TYSON: Why do you look at me like that? Like I’m— like— [LAUGHTER]. What kind of theory is left for you to do
with pencil and paper, if most of the action is in models and simulations and the data?. BOYLAN-KOLCHIN: I think it’s a fair question. And there isn’t as much, certainly, as there
used to be. But I think there is always room for trying
to understand the very basics. And when you’re adding in extra components
of matter or energy, it really is— the laws of physics tell you that the energy content
of the universe. controls the expansion rate. And so you can do this— okay, maybe you
don’t need a million processors, you just need one processor. But you could just make a plot of this. And that’s basically pencil and paper calculation
to see how that affects the age of the universe. How that affects the relationship. between the redshift that we see something
at, and the time that we associate with that end of the universe. TYSON: So you’re not using software or hardware,
you’re using wetware, the brain. BOYLAN-KOLCHIN: That’s right. TYSON: Is wetware, I think. Is it still called that? BOYLAN-KOLCHIN: I think so, yeah. TYSON: All right, sounds good. Now, Wendy. So, you’re going to have the biggest telescope
in the land. FREEDMAN: I hope so. TYSON: And when does it come online? FREEDMAN: Well, that depends on funding. So it’s totally funding-limited now. The project has been reviewed, all the technical
milestones have been reached. The site has been leveled, the hard rock excavated. There are dormitories there for people to
work, and the mirrors have been cast. So— TYSON: You’re just waiting for money. FREEDMAN: We’re waiting for money. TYSON: How much money do you need? FREEDMAN: A lot. TYSON: How much? [LAUGHTER] BOYLAN-KOLCHIN: Who’s got a hat to pass
around? TYSON: We’ll take the collection plate here. [LAUGHTER] FREEDMAN: So the— TYSON: Wouldn’t that be— if in science,
we did that? You know? FREEDMAN: What? TYSON: Come hear a really cool project, and
we just sent around a hat. So, how— FREEDMAN: Well, no, I mean, the community
actually has been really generous. The astronomical community has benefitted
from private philanthropy. That’s been true since the time— TYSON: Since the beginning. Oh, yeah. Yeah. FREEDMAN: Yeah... TYSON: The Keck Telescope is private money. FREEDMAN: That’s right. And the Magellan telescopes were private money,
and a lot of the— TYSON: Because telescopes have very long life
expectancies, because we change out— they’re just buckets to collect light. And the detector at the business end is what
can improve over time, so you can have a telescope that you name in a naming opportunity in one
decade, and it can still be going strong six, seven decades later. FREEDMAN: And a lot of the funding for the
Giant Magellan has come from private philanthropy. TYSON: So how much more do you need? You haven’t answered my question. FREEDMAN: In the ballpark of several hundred
million dollars. It’s a lot of money.. TYSON: Not if you’re— wait, how many—
we’ve got more billionaires than ever before. That’s lunch money for them. FREEDMAN: Can I enlist you? TYSON: So Priya, I want you to take us out,
as a student of philosophy and the history of science. Where are we today in this field, and is there—
do you foresee that in five years, ten years, 20 years, a completely new understanding of
all of this will emerge? Or is this going to be tight, and maybe there’s
just something different we’ll understand, and we’ll plug this into that broader, bigger
view of what’s going on? NATARAJAN: Well, I like to think that this
is just the start of a major kind of revolution that is going to completely transform our
understanding. However, we’ve never been able to predict
the future of science itself. I don't think Copernicus ever imagined, in
1543, that we would have the capacity to have the Voyagers leave the solar system. So I’m not going to speculate exactly. But I’m going to enjoy the thrill of the
moment. I mean, these revolutions are just remarkable. And to think that we, with this little gelatinous
thing that’s in our heads, aided by the—.. TYSON: Talk about your own head. [LAUGHTER]a NATARAJAN: Small head. You know, are able to figure out so much. I mean, it’s astounding. I mean, I am in awe of the universe and the
capacity of collaboration and how science has worked, and reason. I just find it really unbelievable that there
can be science denialism, given all of this. Right? TYSON: I didn’t see it going there, but
that’s where it landed. Wow. Wow. [APPLAUSE] Wow. Yeah. So it is interesting we can make these discoveries
and people run, “I don’t trust science. I saw my YouTube, and they don’t me not
to trust scientists.” NATARAJAN: [LAUGHTER] Right. Right. TYSON: “I’m not gonna get vaccines, because
they don’t understand.” This goes on. We live in that world. NATARAJAN: We live in that crazy world. TYSON: But so do you— I’m going to end
with these two questions to you. You’re talking about our gelatinous brain. Are we smart enough genetically, as a species,
to answer the questions we have posed about the universe? Or deeper still, are we smart enough to even
know what questions to ask? NATARAJAN: Oh, I like that. That was a really beautiful second question. I think that we— there is no reason— TYSON: Or are we all just touching the elephant? NATARAJAN: Right. TYSON: And we’ll never see the elephant,
because we have no idea what we’re touching. NATARAJAN: Right. I think that regardless of whether we as individuals
have the capacity, I think this is where AI is going to be interesting. It’s going to augment our capacity to understand,
comprehend, and take in a lot of information and data, and process it in the ways that
we tell it to process. TYSON: So, I like that. So it’s AI-augmented intelligence, rather
than artificial intelligence, would be a more sensible understanding of this. NATARAJAN: Yeah. Yeah. And I think that is the way of the future,
if we— you know, but then on the other hand, something could explode, right? This is science. We don’t know. Something could fundamentally shift. And maybe there’ll be a way to cognitively
enhance ourselves genetically. I don't know. I mean, you know? That’s possible, too. Right? TYSON: Hmmm. NATARAJAN: You don’t sound— TYSON: No, no. I— you know. Okay. I just— [LAUGHTER]. NATARAJAN: Loss for words? TYSON: Yeah, yeah. I don’t— yeah. I don’t want anybody messing around inside
my head. That’s all. NATARAJAN: Oh, I see. TYSON: So. Just one final— oh, Wendy, you had a quick
comment? FREEDMAN: So, I love that we’re in this
philosophical bend, and it’s probably a good place to end. But can I inject a practical thing having
to do with data, which— TYSON: Please. FREEDMAN: And JWST data. So our group right now, in these questions
we’re discussing right now, we have a JWST program to try and measure the expansion rate
in three different ways, all in the same galaxies. And we’ve done something, we’ve blinded
ourselves, literally. We’ve taken the data and we’ve added random
numbers to the different catalogs, encrypted those random numbers— so that nobody in
our group knows what the final answer will be. And we’re doing all of the analysis in this
mode of, there’s just fake numbers that are applied to the data so that we don’t
know where this is going to end up. It hasn’t been applied to this program before. But we are this close to having an answer. And so in three different ways— so either,
you know, all three are going to agree, not agree. Two might agree. I don’t know which ones. But we will be able to do that very soon. And I’m really excited about this, because
I don't know where this is going to land, and it’s going to be fun. TYSON: So, ways of testing the integrity of
your observation, or your models. FREEDMAN: Yeah. TYSON: Yeah. Very, very cool. Well I like that, and I like the future, I
like what I see here and what you’ve all said, and the angle with which you have approached
the nearby and distant universe. I’m much more comfortable in this universe,
hearing that we have some really smart people on top of this situation. Join me in thanking our panel. [APPLAUSE]