In the course

Supports 6 chapters

Keep watching

Related videos

10 videos · 5 h 17 min

  • Course · MIT

    Quantum Physics I

    MIT OpenCourseWare · Allan Adams · 2013

    Allan Adams' celebrated course starts from superposition and the experimental facts, builds the wavefunction, operators and the Schrödinger equation, then tours scattering, hydrogen, identical particles and band structure before closing on entanglement and Bell's theorem. Calculus and a little linear algebra are enough to keep up.

  • Course · Oxford

    Quantum Mechanics

    University of Oxford · James Binney · 2009–10

    James Binney's Oxford course, given over Michaelmas Term 2009 and Hilary Term 2010 and built on probability amplitudes and Dirac notation from the very first lecture. Highlights: tunnelling and radioactive decay, the EPR argument and Bell's inequality, spin and the Stern–Gerlach experiment, and a full treatment of hydrogen.

  • Lecture · MIT

    Lecture 3: The Wave Function

    MIT OpenCourseWare · Allan Adams · 2013

    Allan Adams's MIT 8.04 lecture introduces the wavefunction as the fundamental description of a quantum system, states the probability rule and normalization, shows why a wave of definite momentum is equally likely to be found anywhere, and restates superposition and uncertainty in the language of wavefunctions. A university-level companion to Parts 1 to 3; expectation values arrive in his next lecture.

  • Lecture · MIT

    Interpretation of the wavefunction

    MIT OpenCourseWare · Barton Zwiebach

    An eight-minute segment of MIT 8.04 (Spring 2016) on what the wavefunction means: Born's probability interpretation, stated on the blackboard. Compare his notation with this section's recipe, density |ψ(x)|² times a width gives a probability.

  • Lecture · MIT

    Normalizable wavefunctions and the question of time evolution

    MIT OpenCourseWare · Barton Zwiebach

    Zwiebach asks which wavefunctions can be normalized at all and whether a normalized wavefunction stays normalized as time passes: the last paragraph of this section, done properly. It looks ahead to the Schrödinger equation of chapter 10.

  • Lecture · Oxford

    001 Introduction to Quantum Mechanics, Probability Amplitudes and Quantum States

    University of Oxford · James Binney · 2009–10

    The lecture from University of Oxford Quantum Mechanics (James Binney, 2009–10) that goes with Chapter 9. The whole course is in the Lecture Hall.

  • Lecture · MIT

    Lecture 9: Operator Methods for the Harmonic Oscillator

    MIT OpenCourseWare

    Allan Adams's lecture from MIT's 8.04 Quantum Physics I (Spring 2013) solves the oscillator a second way, with raising and lowering operators instead of a differential equation. The algebra runs ahead of this course, but watch how a single commutation rule between the two operators generates the entire evenly spaced ladder, a structure Adams promises you will meet again all the way up to quantum field theory.

  • Lecture · Stanford

    The harmonic oscillator – David Miller

    David Miller Quantum Mechanics Courses · David A. B. Miller

    A segment of David Miller's Stanford quantum mechanics course that sets up the oscillator's Schrödinger equation and its solutions. At 19 minutes it is a much shorter pass at section 2 than the 81-minute MIT lecture in the Lecture Hall; check that his energy levels come out evenly spaced, starting at ½ħω.

  • Lecture · MIT

    Creation and annihilation operators acting on energy eigenstates

    MIT OpenCourseWare · Barton Zwiebach

    From MIT's 8.04 Quantum Physics I (Spring 2016): the creation (raising) and annihilation (lowering) operators applied to the state on each rung, which is section 5's first paragraph done on the board. It makes a compact companion to the briefing's 78-minute operator lecture; look for where the √(n + 1) and √n factors come from.

  • Lecture · MIT

    8. Quantum Mechanical Harmonic Oscillator

    MIT OpenCourseWare · Robert Field · 2017

    The lecture from MIT 5.61 Physical Chemistry (Robert Field, 2017) that goes with Chapter 13. The whole course is in the Lecture Hall.