Lecture Notes: CHEM 410A - Physical Chemistry

Lecture 5.2: Physical Chemistry - CHEM 410A

Basic Information

  • Instructor: Yuezhi Mao
  • Course: CHEM 410A (Physical Chemistry)
  • Semester: Spring 2026
  • Institution: San Diego State University (SDSU)

Recap of 1-D Harmonic Oscillator and Energy Levels

  • Harmonic Potential:
    • A potential energy function typically represented in physical chemistry.
    • Configured as a parabolic curve which describes the restorative force experienced by a particle displaced from its equilibrium position.
  • Schrödinger Equation (S.E.):
    • Fundamental equation in quantum mechanics that describes how the quantum state of a physical system changes over time.
  • Results from Solving the Schrödinger Equation:
    • Derives the energy levels of a quantum system.
  • Energy Levels:
    • Defined by the vibrational quantum number (ν).
    • Levels are evenly spaced.
    • Represented mathematically as:
      E_v = igg(
      u + rac{1}{2} igg) ar{h}
      u
  • Zero-Point Energy:
    • The lowest energy state (ν = 0) of the quantum oscillator which is not zero; it includes the value given by:
      E_0 = rac{1}{2} ar{h}
      u

1-D Harmonic Oscillator Wavefunctions

Key Characteristics and Components

  • Wavefunctions:
    • Depict the probability amplitude of a particle's position.
  • Normalization Constant:
    • Ensure that the total probability across all space equals one.
    • This constant changes with the quantum number ν.
  • Hermite Polynomials:
    • A set of orthogonal polynomials crucial for the solutions of the wavefunctions of the harmonic oscillator.
    • Their highest power corresponds directly to ν, and the polynomials will either exclusively represent odd or even powers depending on ν.
  • Complete Set of Orthonormal Functions:
    • The H.O. wavefunctions can represent functions such that:
    • They are orthogonal to one another.
    • They can be normalized to 1.
  • Ground-State Wavefunction (ν = 0):
    • Expressed as a standard Gaussian function given by:
      ext{ψ}_0(x) = A e^{- rac{x^2}{2a^2}}
    • Where A is the normalization constant, and a is the characteristic length scale of the oscillator.

Features of Harmonic Oscillator Wavefunctions

  • Even/Odd Functionality:
    • The wavefunction behaves as an even function when ν is even and as an odd function when ν is odd.
  • Number of Nodes:
    • The number of nodes in the wavefunction corresponds to the vibrational quantum number ν.
  • Behavior Between Classical Turning Points:
    • The wavefunction oscillates between the classical turning points but decays to 0 beyond those limits.
  • Effect of Higher Quantum Numbers (ν):
    • As ν increases, the Hermite polynomial dimensions grow substantially before the Gaussian function rapidly decreases to zero.
    • This phenomenon leads to wavefunctions that spread out over a wider range, resulting in maxima of probability density moving towards classical turning points.
  • Classical Turning Points:
    • These points are defined where energy levels intersect with the potential energy curve, given by the equation:
      E = V, ext{ thus, } x_{tp} = igg(2ν + 1 igg) rac{ar{h}}{
      u}
    • Expresses the classical turning points of oscillator behavior, where
      x_{tp} = igg( rac{igg( 2ν + 1 igg) ar{h}}{mar{ω}} igg)^{1/2}
  • Implications of Intrinsic Properties of the Oscillator:
    • Heavier Particles: This leads to smaller energy spacings:
      ar{ω} = rac{k}{m}
    • Stiffer Spring (Higher k): Results in larger energy spacings and produces narrower wavefunctions.

Evaluating Quantities from H.O. Wavefunctions

  1. Normalization:
    • The process of ensuring the total probability of finding a particle in all space is equal to 1.
  2. Expectation Values:
    • Measured averages of physical quantities derived from wavefunctions, useful in quantum mechanics to describe particle behavior.
  3. Probability in Classically Forbidden Regions (Tunneling Probability):
    • Specifically discussed for the ground state (ν = 0) and includes cases where:
    • Probability beyond classical limits (i.e., for x > x{max} and x < -x{max} ).
    • Additionally provided a Python program to calculate tunneling probability for states where ν > 0.