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量子力學導論 Chap Chap Chap Chap 1 2 3 4 - The Wave Function - The Time-independent Schrödinger Equation - Formalism in Hilbert Space -表象理論 Quantum Mechanics Chap 2 - The Time-independent Schrödinger Equation ► 2.1 Stationary state Assume V is independent of t , use separation of variables Deduce from equation (2.1) , then Quantum Mechanics ...(2.2) time-independent Schrödinger equation Quantum Mechanics ■ properties of (i) Stationary state for every expectation value is constant in time (ii) Definite total energy Classical mechanics : total energy is Hamiltonian Quantum mechanics : corresponding Hamiltonian operator Quantum Mechanics thus equation (2.2) Quantum Mechanics (iii) Linear combination of separable solution ► 2.2 Infinite square well( one dimensional box) and boundary conditions: Quantum Mechanics deduce: outside the potential well finding the particle inside the well V = 0 thus , probability is zero for Quantum Mechanics normalize Quantum Mechanics ■ first three states and probability density of infinite square well Quantum Mechanics ► 2.3 Harmonic oscillator Classical treatment : solution potential energy V is related to F : Quantum treatment : Quantum Mechanics solve equation (2.3) by use ladder operator rewrite equation (2.3) by ladder operator : Quantum Mechanics compare equation(2.3) similarly discussion (i) Quantum Mechanics and (ii) and Quantum Mechanics and (iii) there must exist a min state with and from Quantum Mechanics and so the ladder of stationary states can illustrate : Quantum Mechanics and ► 2.4 Delta-function potential Energy E Consider potential then Quantum Mechanics (i) bound state : E < 0 similarly use boundary condition : find k : from Quantum Mechanics and so normalize and Quantum Mechanics (ii) scattering state : E > 0 and Quantum Mechanics for wave coming in from left ( D = 0 ) , equation (2.5),(2.6) rewrite is incident wave is reflected wave is transmitted wave R is reflection coefficient T is transmission coefficient Quantum Mechanics ► 2.5 Free particle Quantum Mechanics Fourier transform wave packet moves along at group velocity and phase velocity so wave packet