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Hunting for Black Holes, with Janna Levin - StarTalk All-Stars

If light can’t escape from black holes, how can we observe them at all? Find out from astrophysicist Janna Levin, co-host Matt Kirshen, and Shep Doeleman, the MIT astrophysicist leading the Event Horizon Telescope project to study black hole Sgr A* at the center of our galaxy. NOTE: StarTalk All-Acc

Topics Discussed

Episode Summary

Executive Summary: The episode explains what black holes are, why scientists believe they exist, and how the Event Horizon Telescope aims to image the shadow of a supermassive black hole. It covers event horizons, Hawking radiation, black-hole size and time dilation, observational limits, and broader questions about relativity, quantum mechanics, and the Big Bang.

Main Topics: What a black hole is (Priority: 5/5): The guests define black holes as regions formed by gravitational collapse where escape velocity exceeds light speed, centered on the event horizon rather than a physical surface. Why black holes are believed to be real (Priority: 5/5): They trace the historical arc from Einstein’s skepticism to later evidence from white dwarfs, neutron stars, and the growing acceptance of black holes as physically real objects. How black holes can be observed (Priority: 5/5): Discussion focuses on seeing the shadow cast by hot infalling gas, since black holes themselves emit no light and cannot be directly viewed against a dark background. Event Horizon Telescope project (Priority: 5/5): The EHT is described as a global Earth-sized radio telescope array using synchronized dishes and atomic clocks to synthesize an image of the black-hole shadow. Quantum effects and Hawking radiation (Priority: 4/5): The show addresses evaporation, information loss, and whether quantum phenomena could alter the shadow or help reconcile gravity with quantum mechanics. Astrophysical examples and targets (Priority: 4/5): They compare the Milky Way’s central black hole Sagittarius A with Virgo A’s much larger black hole, explaining why these are prime imaging targets. Public questions and misconceptions (Priority: 4/5): Listener questions cover black-hole destruction, danger from lab-created mini black holes, whether the Big Bang could be a black hole, and how black holes affect time.

Key Arguments: Black holes are not empty voids but extreme spacetime regions where collapse creates an event horizon beyond which information cannot escape. The best way to image a black hole is indirectly, by observing the bright ring of heated gas and the shadow it casts. The Event Horizon Telescope works by combining multiple radio telescopes across Earth with precise timing to emulate a planet-sized aperture. Black holes likely exist because multiple lines of evidence show matter can reach extreme densities, from white dwarfs to neutron stars to galactic-center dynamics. Hawking radiation implies black holes can evaporate over immense timescales, but this is too slow to affect current EHT images. The EHT can test general relativity near the edge of a black hole, though deviations would be difficult to interpret and would have major theoretical implications. General relativity and quantum mechanics remain unresolved because gravity is nonlinear and may be emergent rather than fundamental.

Data Points: Year general relativity developed: 1915 - Referenced as Einstein’s formulation of general relativity Approximate time since GR's creation at recording: 101 years - Used in a discussion of GPS and Einstein’s theory Year black hole got its name: 1967 - John Wheeler reportedly popularized the term Solar mass of Milky Way’s central black hole: 4 million solar masses - Sagittarius A at the center of the Milky Way Solar mass of Virgo A black hole: 6 billion solar masses - A more massive EHT target in another galaxy Distance to Milky Way center: 25,000 light years - Distance to Sagittarius A from Earth Distance to Virgo A: 17 megaparsecs - Given as roughly 17 million years away in light-travel terms Angular size of Sagittarius A: 10 microarcseconds - Approximate apparent size on the sky Shadow size of Sagittarius A: 50 microarcseconds - Used for EHT resolution comparison Size comparison analogy: citrus fruit on the moon / quarter on the moon - Explains the tiny angular scale the telescope must resolve Asteroid-mass black hole example: 100 trillion kilograms - Illustrates that a small-mass black hole would be smaller than an atom Galactic-center cloud G2 mass: about 3 Earth masses - Mentioned as a cloud thought to be falling into Sagittarius A Black-hole formation in stars: about 1 billion stars in the Milky Way will one day become black holes - Rough population estimate stated in conversation Three initial telescopes: Hawaii, Arizona, California - First linked EHT sites Largest single radio telescope mentioned: 50 meters across - Used to illustrate telescope scale

Pivotal Quotes: "A black hole is essentially when gravity runs amok." — Shep Dolman: Definition of black holes early in the discussion "The whole Earth is a telescope." — Shep Dolman: Description of how the Event Horizon Telescope synthesizes a planet-sized aperture "You can take a black hole and you can fill it full of hello kitty dolls... and after it's done settling down, you would have no idea what went into it." — Shep Dolman: Explaining the black-hole no-hair idea in a humorous way

Implications: The episode frames black-hole imaging as a milestone test of Einstein’s theory and a probe of quantum gravity. Success would validate EHT’s global method; surprises could reshape fundamental physics and our understanding of spacetime, information, and cosmic evolution.

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