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    Quantum Field Theory

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    • Introduction to Quantum Mechanics
      • 1.1Historical Background
      • 1.2Introduction to Quantum Concepts
      • 1.3Quantum States and Observables
    • Wave-Particle Duality
      • 2.1The Double Slit Experiment
      • 2.2Heisenberg's Uncertainty Principle
      • 2.3Quantum Superposition and Entanglement
    • The Schrödinger Equation
      • 3.1Time-Dependent Equation
      • 3.2Stationary States
      • 3.3Square Well Potential
    • Quantum Operators and Measurement
      • 4.1Quantum Operators
      • 4.2The Measurement Postulate
      • 4.3Complex Probability Amplitudes
    • Quantum Mechanics of Systems
      • 5.1Quantum Harmonic Oscillator
      • 5.2Quantum Angular Momentum
      • 5.3Particle in a Box
    • The Dirac Equation
      • 6.1Wave Equations
      • 6.2The Dirac Sea
      • 6.3Hole Theory
    • Introduction to Quantum Electrodynamics (QED)
      • 7.1Electromagnetic Field
      • 7.2Feynman Diagrams
      • 7.3QED Interactions
    • Path Integrals and Quantum Mechanics
      • 8.1Feynman’s Approach
      • 8.2Action Principle
      • 8.3Quantum Oscillator Problem
    • Symmetries in Quantum Field Theory
      • 9.1Gauge Symmetry
      • 9.2Poincaré Symmetry
      • 9.3Global and Local Symmetries
    • Quantum Chromodynamics
      • 10.1Color Charge
      • 10.2Quark Model
      • 10.3Confinement and Asymptotic Freedom
    • The Higgs Mechanism
      • 11.1Electroweak Symmetry Breaking
      • 11.2The Higgs Boson
      • 11.3Implication for Mass of Known Particles
    • Quantum Field Theory in Curved Space-Time
      • 12.1The Concept of Spacetime
      • 12.2Quantum Effects in Curved Spaces
      • 12.3Hawking Radiation
    • Quantum Cosmology and Conclusion
      • 13.1Big Bang Theory
      • 13.2Cosmic Inflation
      • 13.3Looking Ahead: Frontiers in Quantum Mechanics

    The Schrödinger Equation

    Understanding the Time-Dependent Schrödinger Equation

    fundamental theory in physics describing the properties of nature on an atomic scale

    Fundamental theory in physics describing the properties of nature on an atomic scale.

    The Schrödinger Equation is a cornerstone of quantum mechanics. It is a mathematical model that describes how quantum systems evolve over time. The time-dependent Schrödinger Equation is particularly important as it provides a complete description of a quantum system at any given time.

    Introduction to the Time-Dependent Schrödinger Equation

    The time-dependent Schrödinger Equation is given by:

    equation

    where H is the Hamiltonian operator (representing the total energy of the system), Ψ is the wave function of the system, i is the imaginary unit, and ħ is the reduced Planck's constant.

    The Hamiltonian operator is a sum of the kinetic and potential energy operators. The wave function Ψ is a mathematical function that provides the probabilities of the outcomes of measurements of an observable in a quantum system.

    Physical Interpretation of the Equation

    The time-dependent Schrödinger Equation is a wave equation in terms of the wavefunction which predicts analytically and exactly the probability of events or outcomes. The solutions to Schrödinger's equation, wave functions, can be used to determine the expected position, momentum, and other physical properties of a particle.

    Solving the Time-Dependent Schrödinger Equation

    Solving the time-dependent Schrödinger Equation involves finding the wave function that satisfies the equation. This is typically done by separation of variables, a common method for solving partial differential equations.

    For simple systems, such as a free particle or a particle in a one-dimensional box, the time-dependent Schrödinger Equation can be solved exactly. For more complex systems, approximate methods are often used.

    In conclusion, the time-dependent Schrödinger Equation is a fundamental equation in quantum mechanics that describes the state and evolution of quantum systems. Understanding this equation and its solutions is crucial for understanding the behavior of quantum systems.

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    Next up: Stationary States