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10 videos · 3 h 21 min

  • Explainer · YouTube

    De Broglie wavelength | Physics | Khan Academy

    Khan Academy Physics

    A clear, unhurried blackboard introduction from Khan Academy's physics series: how Louis de Broglie gave matter a wavelength, λ = h/p, and won a Nobel Prize for the idea. Watch for where the formula comes from and how to put numbers into it; Parts 1 to 3 of the lesson take the same road with more history and more precision.

  • Explainer · YouTube

    AT&T Archives: Matter Waves, Holden and Germer on Wave Nature and the Davisson-Germer Experiment

    AT&T Tech Channel

    A classic classroom film made around 1961 by Educational Services Incorporated with two Bell Labs scientists: Alan Holden hosts and narrates, and Lester Germer himself re-creates the famous 1927 experiment he performed with Clinton Davisson. The perfect companion to Part 4: the experiment re-created by one of the first people ever to see electrons diffract.

  • Explainer · YouTube

    Why don't quantum effects occur in large objects? double slit experiment with tennis balls

    Arvin Ash

    Arvin Ash asks this section's question about a tennis ball. The lesson answers it with wavelength; he adds the second half of the answer: a big object cannot be cut off from air molecules, scattered light and its own thermal glow, any of which records its path and wipes out interference. Section 8 comes back to that idea. Keep both halves in mind: even a perfectly isolated ball would have a wavelength far too short to show fringes.

  • Demo · YouTube

    How to demonstrate electron diffraction in the classroom

    National STEM Centre

    A four-minute classroom demonstration: an electron beam passed through graphite produces diffraction rings, the same kind of ring pattern G. P. Thomson photographed in 1927. Use section 3's shortcut, λ ≈ 1.226/√V nm: a higher accelerating voltage gives a shorter wavelength, so the rings should shrink whenever the voltage goes up.

  • Explainer · YouTube

    What is Wave Particle Duality?

    Physics Explained

    A careful history of duality built around de Broglie. The jump lands on 'The Bohr Model revisited' and 'Explaining the allowed orbits', the standing-wave argument of this section, then runs on through 'Bragg Diffraction' and the Davisson–Germer results for section 4. Rewind to 'The French Prince' (18:35) for de Broglie himself.

  • Explainer · YouTube

    Can You Keep Zooming In Infinitely?

    Veritasium

    Veritasium on why seeing atoms is so hard. The jump starts at 'How does an electron microscope work?', then covers the transmission electron microscope and 'Spherical Aberration', the lens flaw that, as this section explains, long kept resolution far coarser than the electron wavelength. It ends on 'Seeing atoms'. Its sources include Ruska's 1986 Nobel lecture.

  • Explainer · YouTube

    Biggest Schrödinger’s cat

    nature video

    Nature's own short report, presented by Lizzie Gibney, on the University of Vienna experiment (Pedalino et al., Nature 2026) that put a cluster of about 7,000 sodium atoms into superposition, the record that ends this section. Watch for how it frames the open question: where does the quantum world stop?

  • 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 · MIT

    de Broglie’s proposal

    MIT OpenCourseWare

    Barton Zwiebach presents de Broglie's proposal at the blackboard in MIT's 8.04 Quantum Physics I (Spring 2016). Expect university-level reasoning about how the energy and momentum relations of the photon were extended to every particle; watch it after Parts 1 and 2.

  • Explainer · Fermilab

    How can a photon have momentum?

    Fermilab · Don Lincoln

    Fermilab's Don Lincoln takes on the exact puzzle of Psigor's callout: how can something with no mass carry momentum? He argues that the question comes from misusing equations; compare his resolution with the lesson's route through E² = (pc)² + (mc²)².