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10 videos · 5 h 53 min

  • Lecture · Nobel Prize

    2012 Nobel Lectures in Physics

    Nobel Prize · Serge Haroche & David J. Wineland · 2012

    Serge Haroche on trapping photons in a box to watch the quantum-to-classical boundary — decoherence — in action, then David Wineland on superposition and entanglement with trapped ions. The experiments that turned thought experiments into laboratory routine.

  • Course · Stanford

    Quantum Entanglements, Part 1

    Stanford · Leonard Susskind · 2006

    Nine evenings on the strangest resource in physics — spin, density matrices, entangled states and Bell's theorem — taught by Susskind to a room of non-specialists. Pairs naturally with Unit 5.

  • Course · IBM Quantum

    Understanding Quantum Information & Computation

    Qiskit · John Watrous · 2022–25

    The clearest modern course on quantum information, from IBM Quantum's John Watrous: single and multiple systems, circuits, teleportation and superdense coding, Shor's and Grover's algorithms, density matrices and error correction. Mathematically honest without being heavy.

  • Interview · World Science Festival

    Is Quantum Reality in the Eye of the Beholder? | World Science Festival

    World Science Festival · Carlo Rovelli

    Carlo Rovelli, the originator of relational quantum mechanics, explains it himself, starting at the chapter on the relational view (12:47). Rewind to 3:50 for how he sees the measurement problem and many worlds; the question critics ask in Part 6, what the world is like in itself, is the one to keep in mind.

  • Lecture · Royal Institution

    The mind-bending reality of quantum mechanics - with Jim Al Khalili

    The Royal Institution · Jim Al-Khalili · 2025

    A Friday Evening Discourse recorded at the Ri in November 2025, a century after Heisenberg's breakthrough: a hundred years of quantum theory, from the 1920s pioneers to the technologies being built now. Keep asking which claims are experiment and which are interpretation.

  • Lecture · Royal Institution

    A Brief History of Quantum Mechanics - with Sean Carroll

    The Royal Institution · Sean Carroll · 2020

    Sean Carroll tells the story from Planck and Einstein through Bohr, de Broglie and Schrödinger, then argues that the measurement problem is still open and makes his case for the many-worlds interpretation. Notice where the history ends and his interpretation begins.

  • Explainer · YouTube

    Quantum Superposition, Explained Without Woo Woo

    The Science Asylum

    Nick Lucid of The Science Asylum takes superposition back to its roots in ordinary wave physics and strips away the mystical talk that usually surrounds it. As you watch, test what you hear against this session's central claim: a superposition is one perfectly definite state written as a sum, and whether a state counts as a superposition depends on which measurement you have in mind.

  • Lecture · MIT

    Lecture 1: Introduction to Superposition

    MIT OpenCourseWare · Allan Adams · 2013

    The opening lecture of MIT's 8.04 Quantum Physics I (Spring 2013), in which Allan Adams uses thought experiments with measuring boxes to build superposition and uncertainty from scratch. Skip the first ten minutes of course logistics, then watch how a few simple box experiments force exactly the rules of this session: repeat a measurement and the answer stays put; measure an incompatible property and it is scrambled.

  • Explainer · YouTube

    The Problem with Quantum Measurement

    Sabine Hossenfelder

    A compact statement of the measurement problem from the theoretical physicist Sabine Hossenfelder, who explains why the measurement update cannot simply be derived from the Schrödinger equation. Her conclusion, that quantum mechanics therefore needs to be completed, is one position among several; chapter 22 lays out the others.

  • Lecture · MIT

    The nature of superposition. Mach-Zehnder interferometer

    MIT OpenCourseWare · Barton Zwiebach

    Zwiebach contrasts classical superposition of fields with the quantum kind using single photons in a Mach-Zehnder interferometer, then states the rule this section builds on: measure a property on αA + βB and you never get anything in between, only a or b, with odds set by |α|² and |β|², after which the state is the one you found. When he says a photon is 'in both beams at the same time', translate it into this section's language (one definite state written as a sum of two path states), and catch his point at about 7:30 that the same vector can be written as a sum in many different ways.