Return to Video

How to take a picture of a black hole | Katie Bouman | TEDxBeaconStreet

  • 0:19 - 0:21
    In the movie "Interstellar,"
  • 0:21 - 0:25
    we get an up-close look
    at a supermassive black hole.
  • 0:25 - 0:27
    Set against a backdrop of bright gas,
  • 0:27 - 0:29
    the black hole's massive
    gravitational pull
  • 0:29 - 0:30
    bends light into a ring.
  • 0:30 - 0:32
    However, this isn't a real photograph,
  • 0:33 - 0:34
    but a computer graphic rendering --
  • 0:34 - 0:38
    an artistic interpretation
    of what a black hole might look like.
  • 0:38 - 0:40
    A hundred years ago,
  • 0:40 - 0:43
    Albert Einstein first published
    his theory of general relativity.
  • 0:43 - 0:45
    In the years since then,
  • 0:45 - 0:48
    scientists have provided
    a lot of evidence in support of it.
  • 0:48 - 0:51
    But one thing predicted
    from this theory, black holes,
  • 0:51 - 0:53
    still have not been directly observed.
  • 0:53 - 0:56
    Although we have some idea
    as to what a black hole might look like,
  • 0:56 - 0:59
    we've never actually taken
    a picture of one before.
  • 0:59 - 1:01
    However, you might be surprised to know
  • 1:01 - 1:06
    that we may be seeing our first picture
    of a black hole in the next couple years.
  • 1:06 - 1:09
    Getting this first picture will come down
    to an international team of scientists,
  • 1:10 - 1:11
    an Earth-sized telescope
  • 1:11 - 1:14
    and an algorithm that puts together
    the final picture.
  • 1:14 - 1:17
    Although I won't be able to show you
    a real picture of a black hole today,
  • 1:18 - 1:20
    I'd like to give you a brief glimpse
    into the effort involved
  • 1:20 - 1:22
    in getting that first picture.
  • 1:24 - 1:25
    My name is Katie Bouman,
  • 1:25 - 1:28
    and I'm a PhD student at MIT.
  • 1:28 - 1:30
    I do research in a computer science lab
  • 1:30 - 1:33
    that works on making computers
    see through images and video.
  • 1:34 - 1:36
    But although I'm not an astronomer,
  • 1:36 - 1:37
    today I'd like to show you
  • 1:37 - 1:40
    how I've been able to contribute
    to this exciting project.
  • 1:42 - 1:45
    If you go out past
    the bright city lights tonight,
  • 1:45 - 1:48
    you may just be lucky enough
    to see a stunning view
  • 1:48 - 1:49
    of the Milky Way Galaxy.
  • 1:50 - 1:52
    And if you could zoom past
    millions of stars,
  • 1:52 - 1:56
    26,000 light-years toward the heart
    of the spiraling Milky Way,
  • 1:56 - 1:59
    we'd eventually reach
    a cluster of stars right at the center.
  • 1:59 - 2:03
    Peering past all the galactic dust
    with infrared telescopes,
  • 2:03 - 2:07
    astronomers have watched these stars
    for over 16 years.
  • 2:07 - 2:10
    But it's what they don't see
    that is the most spectacular.
  • 2:10 - 2:13
    These stars seem to orbit
    an invisible object.
  • 2:16 - 2:18
    By tracking the paths of these stars,
  • 2:18 - 2:19
    astronomers have concluded
  • 2:19 - 2:22
    that the only thing small and heavy
    enough to cause this motion
  • 2:22 - 2:24
    is a supermassive black hole --
  • 2:24 - 2:29
    an object so dense that it sucks up
    anything that ventures too close --
  • 2:29 - 2:30
    even light.
  • 2:30 - 2:33
    But what happens if we were
    to zoom in even further?
  • 2:33 - 2:38
    Is it possible to see something
    that, by definition, is impossible to see?
  • 2:40 - 2:43
    Well, it turns out that if we were
    to zoom in at radio wavelengths,
  • 2:43 - 2:44
    we'd expect to see a ring of light
  • 2:44 - 2:47
    caused by the gravitational
    lensing of hot plasma
  • 2:47 - 2:49
    zipping around the black hole.
  • 2:49 - 2:50
    In other words,
  • 2:50 - 2:53
    the black hole casts a shadow
    on this backdrop of bright material,
  • 2:53 - 2:55
    carving out a sphere of darkness.
  • 2:55 - 2:59
    This bright ring reveals
    the black hole's event horizon,
  • 2:59 - 3:01
    where the gravitational pull
    becomes so great
  • 3:01 - 3:03
    that not even light can escape.
  • 3:05 - 3:08
    Einstein's equations predict
    the size and shape of this ring,
  • 3:08 - 3:11
    so taking a picture of it
    wouldn't only be really cool,
  • 3:11 - 3:14
    it would also help to verify
    that these equations hold
  • 3:14 - 3:16
    in the extreme conditions
    around the black hole.
  • 3:16 - 3:19
    However, this black hole
    is so far away from us,
  • 3:19 - 3:22
    that from Earth, this ring appears
    incredibly small --
  • 3:22 - 3:26
    the same size to us as an orange
    on the surface of the moon.
  • 3:26 - 3:29
    That makes taking a picture of it
    extremely difficult.
  • 3:30 - 3:32
    Why is that?
  • 3:32 - 3:35
    Well, it all comes down
    to a simple equation.
  • 3:35 - 3:38
    Due to a phenomenon called diffraction,
  • 3:38 - 3:39
    there are fundamental limits
  • 3:39 - 3:42
    to the smallest objects
    that we can possibly see.
  • 3:42 - 3:46
    This governing equation says
    that in order to see smaller and smaller,
  • 3:46 - 3:49
    we need to make our telescope
    bigger and bigger.
  • 3:49 - 3:52
    But even with the most powerful
    optical telescopes here on Earth,
  • 3:52 - 3:54
    we can't even get close
    to the resolution necessary
  • 3:54 - 3:56
    to image on the surface of the moon.
  • 3:56 - 4:00
    In fact, here I show one of the highest
    resolution images ever taken
  • 4:00 - 4:01
    of the moon from Earth.
  • 4:01 - 4:04
    It contains roughly 13,000 pixels,
  • 4:04 - 4:08
    and yet each pixel would contain
    over 1.5 million oranges.
  • 4:09 - 4:11
    So how big of a telescope do we need
  • 4:11 - 4:14
    in order to see an orange
    on the surface of the moon
  • 4:14 - 4:16
    and, by extension, our black hole?
  • 4:16 - 4:18
    Well, it turns out
    that by crunching the numbers,
  • 4:18 - 4:21
    you can easily calculate
    that we would need a telescope
  • 4:21 - 4:22
    the size of the entire Earth.
  • 4:22 - 4:23
    (Laughter)
  • 4:23 - 4:26
    If we could build
    this Earth-sized telescope,
  • 4:26 - 4:29
    we could just start to make out
    that distinctive ring of light
  • 4:29 - 4:31
    indicative of the black
    hole's event horizon.
  • 4:31 - 4:34
    Although this picture wouldn't contain
    all the detail we see
  • 4:34 - 4:35
    in computer graphic renderings,
  • 4:35 - 4:38
    it would allow us to safely get
    our first glimpse
  • 4:38 - 4:40
    of the immediate environment
    around a black hole.
  • 4:41 - 4:42
    However, as you can imagine,
  • 4:42 - 4:46
    building a single-dish telescope
    the size of the Earth is impossible.
  • 4:46 - 4:48
    But in the famous words of Mick Jagger,
  • 4:48 - 4:50
    "You can't always get what you want,
  • 4:50 - 4:52
    but if you try sometimes,
    you just might find
  • 4:52 - 4:53
    you get what you need."
  • 4:53 - 4:56
    And by connecting telescopes
    from around the world,
  • 4:56 - 4:59
    an international collaboration
    called the Event Horizon Telescope
  • 4:59 - 5:02
    is creating a computational telescope
    the size of the Earth,
  • 5:02 - 5:04
    capable of resolving structure
  • 5:04 - 5:06
    on the scale of a black
    hole's event horizon.
  • 5:07 - 5:10
    This network of telescopes is scheduled
    to take its very first picture
  • 5:10 - 5:12
    of a black hole next year.
  • 5:14 - 5:17
    Each telescope in the worldwide
    network works together.
  • 5:17 - 5:20
    Linked through the precise timing
    of atomic clocks,
  • 5:20 - 5:23
    teams of researchers at each
    of the sights freeze light
  • 5:23 - 5:26
    by collecting thousands
    of terabytes of data.
  • 5:26 - 5:31
    This data is then processed in a lab
    right here in Massachusetts.
  • 5:33 - 5:34
    So how does this even work?
  • 5:34 - 5:38
    Remember if we want to see the black hole
    in the center of our galaxy,
  • 5:38 - 5:41
    we need to build this impossibly large
    Earth-sized telescope?
  • 5:41 - 5:43
    For just a second,
    let's pretend we could build
  • 5:43 - 5:45
    a telescope the size of the Earth.
  • 5:45 - 5:47
    This would be a little bit
    like turning the Earth
  • 5:47 - 5:49
    into a giant spinning disco ball.
  • 5:49 - 5:51
    Each individual mirror would collect light
  • 5:51 - 5:54
    that we could then combine
    together to make a picture.
  • 5:54 - 5:57
    However, now let's say
    we remove most of those mirrors
  • 5:57 - 5:59
    so only a few remained.
  • 5:59 - 6:02
    We could still try to combine
    this information together,
  • 6:02 - 6:04
    but now there are a lot of holes.
  • 6:04 - 6:08
    These remaining mirrors represent
    the locations where we have telescopes.
  • 6:08 - 6:12
    This is an incredibly small number
    of measurements to make a picture from.
  • 6:12 - 6:16
    But although we only collect light
    at a few telescope locations,
  • 6:16 - 6:19
    as the Earth rotates, we get to see
    other new measurements.
  • 6:20 - 6:23
    In other words, as the disco ball spins,
    those mirrors change locations
  • 6:23 - 6:26
    and we get to observe
    different parts of the image.
  • 6:26 - 6:30
    The imaging algorithms we develop
    fill in the missing gaps of the disco ball
  • 6:30 - 6:33
    in order to reconstruct
    the underlying black hole image.
  • 6:33 - 6:36
    If we had telescopes located
    everywhere on the globe --
  • 6:36 - 6:38
    in other words, the entire disco ball --
  • 6:38 - 6:39
    this would be trivial.
  • 6:39 - 6:43
    However, we only see a few samples,
    and for that reason,
  • 6:43 - 6:45
    there are an infinite number
    of possible images
  • 6:45 - 6:48
    that are perfectly consistent
    with our telescope measurements.
  • 6:49 - 6:52
    However, not all images are created equal.
  • 6:52 - 6:57
    Some of those images look more like
    what we think of as images than others.
  • 6:57 - 7:00
    And so, my role in helping to take
    the first image of a black hole
  • 7:00 - 7:03
    is to design algorithms that find
    the most reasonable image
  • 7:03 - 7:05
    that also fits the telescope measurements.
  • 7:06 - 7:10
    Just as a forensic sketch artist
    uses limited descriptions
  • 7:10 - 7:14
    to piece together a picture using
    their knowledge of face structure,
  • 7:14 - 7:17
    the imaging algorithms I develop
    use our limited telescope data
  • 7:17 - 7:22
    to guide us to a picture that also
    looks like stuff in our universe.
  • 7:22 - 7:26
    Using these algorithms,
    we're able to piece together pictures
  • 7:26 - 7:28
    from this sparse, noisy data.
  • 7:28 - 7:33
    So here I show a sample reconstruction
    done using simulated data,
  • 7:33 - 7:35
    when we pretend to point our telescopes
  • 7:35 - 7:37
    to the black hole
    in the center of our galaxy.
  • 7:37 - 7:42
    Although this is just a simulation,
    reconstruction such as this give us hope
  • 7:42 - 7:45
    that we'll soon be able to reliably take
    the first image of a black hole
  • 7:45 - 7:48
    and from it, determine
    the size of its ring.
  • 7:50 - 7:53
    Although I'd love to go on
    about all the details of this algorithm,
  • 7:53 - 7:56
    luckily for you, I don't have the time.
  • 7:56 - 7:58
    But I'd still like
    to give you a brief idea
  • 7:58 - 8:00
    of how we define
    what our universe looks like,
  • 8:00 - 8:04
    and how we use this to reconstruct
    and verify our results.
  • 8:05 - 8:08
    Since there are an infinite number
    of possible images
  • 8:08 - 8:10
    that perfectly explain
    our telescope measurements,
  • 8:10 - 8:13
    we have to choose
    between them in some way.
  • 8:13 - 8:15
    We do this by ranking the images
  • 8:15 - 8:17
    based upon how likely they are
    to be the black hole image,
  • 8:17 - 8:20
    and then choosing the one
    that's most likely.
  • 8:20 - 8:22
    So what do I mean by this exactly?
  • 8:22 - 8:24
    Let's say we were trying to make a model
  • 8:24 - 8:28
    that told us how likely an image
    were to appear on Facebook.
  • 8:28 - 8:29
    We'd probably want the model to say
  • 8:29 - 8:33
    it's pretty unlikely that someone
    would post this noise image on the left,
  • 8:33 - 8:35
    and pretty likely that someone
    would post a selfie
  • 8:35 - 8:37
    like this one on the right.
  • 8:37 - 8:38
    The image in the middle is blurry,
  • 8:38 - 8:41
    so even though it's more likely
    we'd see it on Facebook
  • 8:41 - 8:42
    compared to the noise image,
  • 8:42 - 8:45
    it's probably less likely we'd see it
    compared to the selfie.
  • 8:46 - 8:48
    But when it comes to images
    from the black hole,
  • 8:48 - 8:52
    we're posed with a real conundrum:
    we've never seen a black hole before.
  • 8:52 - 8:54
    In that case, what is a likely
    black hole image,
  • 8:54 - 8:57
    and what should we assume
    about the structure of black holes?
  • 8:58 - 9:00
    We could try to use images
    from simulations we've done,
  • 9:00 - 9:03
    like the image of the black hole
    from "Interstellar,"
  • 9:03 - 9:06
    but if we did this,
    it could cause some serious problems.
  • 9:07 - 9:11
    What would happen
    if Einstein's theories didn't hold?
  • 9:11 - 9:15
    We'd still want to reconstruct
    an accurate picture of what was going on.
  • 9:15 - 9:18
    If we bake Einstein's equations
    too much into our algorithms,
  • 9:18 - 9:21
    we'll just end up seeing
    what we expect to see.
  • 9:21 - 9:23
    In other words,
    we want to leave the option open
  • 9:23 - 9:26
    for there being a giant elephant
    at the center of our galaxy.
  • 9:26 - 9:27
    (Laughter)
  • 9:28 - 9:31
    Different types of images have
    very distinct features.
  • 9:31 - 9:35
    We can easily tell the difference
    between black hole simulation images
  • 9:35 - 9:37
    and images we take
    every day here on Earth.
  • 9:37 - 9:40
    We need a way to tell our algorithms
    what images look like
  • 9:40 - 9:43
    without imposing one type
    of image's features too much.
  • 9:44 - 9:46
    One way we can try to get around this
  • 9:46 - 9:49
    is by imposing the features
    of different kinds of images
  • 9:49 - 9:53
    and seeing how the type of image we assume
    affects our reconstructions.
  • 9:55 - 9:58
    If all images' types produce
    a very similar-looking image,
  • 9:58 - 10:00
    then we can start to become more confident
  • 10:00 - 10:04
    that the image assumptions we're making
    are not biasing this picture that much.
  • 10:04 - 10:07
    This is a little bit like
    giving the same description
  • 10:07 - 10:10
    to three different sketch artists
    from all around the world.
  • 10:10 - 10:13
    If they all produce
    a very similar-looking face,
  • 10:13 - 10:15
    then we can start to become confident
  • 10:15 - 10:19
    that they're not imposing their own
    cultural biases on the drawings.
  • 10:20 - 10:23
    One way we can try to impose
    different image features
  • 10:23 - 10:26
    is by using pieces of existing images.
  • 10:26 - 10:29
    So we take a large collection of images,
  • 10:29 - 10:31
    and we break them down
    into their little image patches.
  • 10:31 - 10:36
    We then can treat each image patch
    a little bit like pieces of a puzzle.
  • 10:36 - 10:40
    And we use commonly seen puzzle pieces
    to piece together an image
  • 10:40 - 10:42
    that also fits our telescope measurements.
  • 10:47 - 10:50
    Different types of images have
    very distinctive sets of puzzle pieces.
  • 10:51 - 10:54
    So what happens when we take the same data
  • 10:54 - 10:58
    but we use different sets of puzzle pieces
    to reconstruct the image?
  • 10:58 - 11:02
    Let's first start with black hole
    image simulation puzzle pieces.
  • 11:04 - 11:06
    OK, this looks reasonable.
  • 11:06 - 11:08
    This looks like what we expect
    a black hole to look like.
  • 11:08 - 11:09
    But did we just get it
  • 11:09 - 11:13
    because we just fed it little pieces
    of black hole simulation images?
  • 11:13 - 11:15
    Let's try another set of puzzle pieces
  • 11:15 - 11:17
    from astronomical, non-black hole objects.
  • 11:18 - 11:20
    OK, we get a similar-looking image.
  • 11:20 - 11:23
    And then how about pieces
    from everyday images,
  • 11:23 - 11:25
    like the images you take
    with your own personal camera?
  • 11:27 - 11:29
    Great, we see the same image.
  • 11:29 - 11:32
    When we get the same image
    from all different sets of puzzle pieces,
  • 11:32 - 11:34
    then we can start to become more confident
  • 11:34 - 11:36
    that the image assumptions we're making
  • 11:36 - 11:39
    aren't biasing the final
    image we get too much.
  • 11:40 - 11:43
    Another thing we can do is take
    the same set of puzzle pieces,
  • 11:43 - 11:46
    such as the ones derived
    from everyday images,
  • 11:46 - 11:49
    and use them to reconstruct
    many different kinds of source images.
  • 11:49 - 11:51
    So in our simulations,
  • 11:51 - 11:55
    we pretend a black hole looks like
    astronomical non-black hole objects,
  • 11:55 - 11:58
    as well as everyday images like
    the elephant in the center of our galaxy.
  • 11:58 - 12:02
    When the results of our algorithms
    on the bottom look very similar
  • 12:02 - 12:04
    to the simulation's truth image on top,
  • 12:04 - 12:07
    then we can start to become
    more confident in our algorithms.
  • 12:07 - 12:09
    And I really want to emphasize here
  • 12:09 - 12:11
    that all of these pictures were created
  • 12:11 - 12:14
    by piecing together little pieces
    of everyday photographs,
  • 12:14 - 12:16
    like you'd take with your own
    personal camera.
  • 12:16 - 12:20
    So an image of a black hole
    we've never seen before
  • 12:20 - 12:24
    may eventually be created by piecing
    together pictures we see all the time
  • 12:25 - 12:27
    Imaging ideas like this
    will make it possible for us
  • 12:27 - 12:30
    to take our very first pictures
    of a black hole,
  • 12:30 - 12:32
    and hopefully, verify
    those famous theories
  • 12:32 - 12:35
    on which scientists rely on a daily basis.
  • 12:36 - 12:38
    But of course, getting
    imaging ideas like this working
  • 12:38 - 12:42
    would never have been possible
    without the amazing team of researchers
  • 12:42 - 12:44
    that I have the privilege to work with.
  • 12:44 - 12:45
    It still amazes me
  • 12:45 - 12:48
    that although I began this project
    with no background in astrophysics,
  • 12:48 - 12:51
    what we have achieved
    through this unique collaboration
  • 12:51 - 12:54
    could result in the very first
    images of a black hole.
  • 12:54 - 12:57
    But big projects like
    the Event Horizon Telescope
  • 12:57 - 13:00
    are successful due to all
    the interdisciplinary expertise
  • 13:00 - 13:02
    different people bring to the table.
  • 13:02 - 13:04
    We're a melting pot of astronomers,
  • 13:04 - 13:06
    physicists, mathematicians and engineers.
  • 13:06 - 13:08
    This is what will make it soon possible
  • 13:08 - 13:11
    to achieve something
    once thought impossible.
  • 13:11 - 13:13
    I'd like to encourage all of you to go out
  • 13:13 - 13:15
    and help push the boundaries of science,
  • 13:15 - 13:19
    even if it may at first seem
    as mysterious to you as a black hole.
  • 13:19 - 13:20
    Thank you.
  • 13:20 - 13:26
    (Applause)
Title:
How to take a picture of a black hole | Katie Bouman | TEDxBeaconStreet
Description:

To take a photo of a black hole, you'd need a telescope the size of a planet. That's not really feasible, but Katie Bouman and her team came up with an alternative solution involving complex algorithms and global cooperation. Check out this talk to learn about how we can see in the ultimate dark.

Katie Bouman is a Ph.D. candidate in the Computer Science and Artificial Intelligence Laboratory (CSAIL) at the Massachusetts Institute of Technology (MIT), under the supervision of William T. Freeman. She previously received a B.S.E. in Electrical Engineering from the University of Michigan, Ann Arbor, MI in 2011 and an S.M. degree in Electrical Engineering and Computer Science from MIT, Cambridge, MA in 2013. The focus of Katie’s research is on using emerging computational methods to push the boundaries of interdisciplinary imaging.

This talk was given at a TEDx event using the TED conference format but independently organized by a local community. Learn more at http://ted.com/tedx

more » « less
Video Language:
English
Team:
closed TED
Project:
TEDxTalks
Duration:
13:33

English subtitles

Revisions Compare revisions