Differential Equations
Schrodinger Equation
Schrodinger in 1926 wrote 4 papers in 6 weeks, each with a new solution of his equation. By year end quantum mechanics had a mathematically rigorous foundation. Two years later Dirac relativized the equation and predicted antimatter.
- Quantum chemistry: the Schrodinger equation for molecules is solved by DFT and Hartree-Fock methods
- Quantum computers: a qubit is a two-level quantum system governed by H
- Solid state physics: band structure of semiconductors from the Bloch equation
Предварительные знания
Schrodinger Equation and Hamiltonian
Schrodinger in 1926 derived his equation from the analogy with Hamiltonian mechanics: i*hbar*d_t psi = H psi, where H = -hbar^2/(2m)*Delta + V is the energy operator. For one particle psi in L^2(R^3). Normalization: integral |psi|^2 = 1. Stationary states H psi_n = E_n psi_n are energy levels. Harmonic oscillator: E_n = hbar*omega*(n+1/2).
What is the energy spectrum of the quantum harmonic oscillator?
Spectral Theory and Quantization
Self-adjointness of H guarantees real spectrum and unitary evolution U(t) = e^{-iHt/hbar} (Stone's semigroup). Discrete spectrum = bound states; continuous spectrum = scattering. Rellich-Kato theorem: if V in L^2 + L^inf, then H is self-adjoint. Quantization: x_hat = x*, p_hat = -i*hbar*d_x, [x_hat, p_hat] = i*hbar.
What does self-adjointness of the Hamiltonian H guarantee?
Key Ideas
- i*hbar*d_t psi = H psi, H = -hbar^2/(2m)*Delta + V(x)
- Stationary states: H phi_n = E_n phi_n, psi_n = e^{-iE_n t/hbar} phi_n
- Oscillator: E_n = hbar*omega*(n+1/2), zero-point E_0 = hbar*omega/2
- Uncertainty principle: Delta x * Delta p >= hbar/2
- Self-adjointness of H <-> unitary group U(t) = e^{-iHt/hbar}
Further Directions
These ideas open paths to deeper mathematics.
- de-28-wave-equation — extends
Вопросы для размышления
- Give a concrete example.
- How does this connect to other areas of mathematics?