Related simulators
Continue with similar topics in this category — or all 65 in Chemistry.
Sequential Stern–Gerlach
Two SG devices: P(up on SG₂) = cos²(θ/2) or sin²(θ/2) after |±z⟩ filter.
Crystal Field Splitting (Oct / Tet)
Δ_t = (4/9)Δ_o; HS vs LS d⁴–d⁷ from CFSE + pairing P; toy complex hue vs Δ_oct.
Orbital Shapes (Schematic)
2D |ψ|² colormap for s-, p-, and d-like angular patterns (pedagogical, not HF).
Electron Configuration
Fill orbitals visually with Aufbau principle animation.
Landau Levels in a Magnetic Field
Charged particle in a uniform B-field: equally-spaced Landau ladder E_n = ℏω_c(n+½) with cyclotron frequency ω_c = qB/m, magnetic length ℓ_B = √(ℏ/qB) and orbit radius r_n = ℓ_B√(2n+1). Animated cyclotron orbit + linear-in-B fan diagram; the n_B = qB/h degeneracy underlies the quantum Hall effect.
Hong–Ou–Mandel Two-Photon Dip
Two indistinguishable photons enter opposite ports of a 50/50 beam splitter and bunch into the same output: coincidence probability P_c(δτ) = ½(1 − V·exp(−(δτ/τ_c)²)) (Gaussian) or Lorentzian. Drag the delay δτ to walk through the dip; live Monte-Carlo converges to the analytic curve. Visibility V = indistinguishability.