Quantum Mechanics
The smallest knobs in the universe — exposed, named, and callable from curl.
- Group — quantum-mechanics
- Operators — 17 (QM1 – QM17)
- Anchor operators — KO42 · QM1 · QM2 · QM11
- Verification — every example closes under
error_pct ≤ 0.1%; every eigen-problem is Master-Equation compiled
What it unifies
Quantum mechanics in Zeq is not a separate subsystem — it is a 17-operator lane of the Master Equation, sharing its ϕ-field with Newtonian forces, relativistic metrics, and Awareness couplings. The Schrödinger evolution (QM1) is just one coupling; pair it with KO42 and every wavefunction you compute is already Zeqond-aligned.
The uncertainty principle (QM2) is treated as a hard constraint on every input. The commutator (QM11) is the kernel's native way to express non-commuting observables. Pauli statistics (QM6) and spin (QM7) expose antisymmetry as first-class. Bose–Einstein and Fermi–Dirac distributions (QM14, QM15) are standard outputs when temperature is in the payload.
Operator catalog
| ID | Formula | Role |
|---|---|---|
| QM1 | iℏ ∂ψ/∂t = −ℏ²/2m ∂²ψ/∂x² + Vψ | Schrödinger evolution |
| QM2 | ∆x·∆p ≥ ℏ/2 | Heisenberg uncertainty |
| QM3 | |ψ⟩ = ∑c_i|ϕ_i⟩ | Superposition |
| QM4 | |ψ⟩ = 1/√2 (|↑⟩_A|↓⟩_B − |↓⟩_A|↑⟩_B) | Bell-state entanglement |
| QM5 | Ĥ|ψ⟩ = E|ψ⟩ | Energy eigenvalue |
| QM6 | ψ(x₁,x₂) = −ψ(x₂,x₁) | Fermionic antisymmetry |
| QM7 | Ŝ²|ψ⟩ = s(s+1)ℏ²|ψ⟩ | Spin eigenvalue |
| QM8 | T ∝ e^{−2∫√{2m(V−E)}/ℏ² dx} | WKB tunneling |
| QM9 | λ = h/p | de Broglie wavelength |
| QM10 | E = hν | Planck-Einstein quanta |
| QM11 | [x̂, p̂] = iℏ | Canonical commutator |
| QM12 | (iγ^μ∂_μ − m)ψ = 0 | Dirac equation |
| QM13 | L = ψ̄(iD−m)ψ | QED Lagrangian |
| QM14 | n_i = 1/[e^{(E_i−µ)/k_B T} − 1] | Bose–Einstein |
| QM15 | n_i = 1/[e^{(E_i−µ)/k_B T} + 1] | Fermi–Dirac |
| QM16 | dÂ/dt = i/ℏ [Ĥ, Â] | Heisenberg evolution |
| QM17 | P(x) = |ψ(x)|² | Born probability |
Runnable worked example — particle-in-a-box eigenvalue, sealed to HulyaPulse
A synchronized computation: KO42 (1.287 Hz metric tensioner) composed with
QM5 (Ĥ|ψ⟩ = E|ψ⟩) for the ground-state energy of an electron in a 1 Å box.
Get a free key first (POST /api/demo-key/mint), then:
curl -X POST https://zeqsdk.com/api/zeq/compute \
-H "Authorization: Bearer zeq_ak_..." \
-H "Content-Type: application/json" \
-d '{
"operators": ["KO42", "QM5"],
"domain": "Quantum Mechanics",
"inputs": { "n": 1, "L": 1e-10, "m": 9.109e-31 }
}'
Real response (abridged):
{
"value": 6.0249212e-18,
"unit": "J",
"operator_id": "QM5",
"zeqState": { "operators": ["KO42", "QM5"], "domain": "Quantum Mechanics" },
"verification": { "precision_bound": "≤ 0.1%" },
"zeqProof": "…"
}
value is E₁ = n²h²/8mL² = 6.0249212e-18 J for the ground state — verified live
against the closed-form eigenvalue.
The Quantum Mechanics domain has a live closed-form solver — the
particle-in-a-box example above returns a real number today. Not every catalogued
operator is wired to it: operators without solver support return no-match from
/api/zeq/compute (unit no-match, no value). The catalogue rows are exact and
documented regardless.
Extend it
- Dirac lane — chain QM12 + QM13 to compile a QED Lagrangian and verify current conservation below 0.1%.
- Thermal statistics — pair QM14/QM15 with QM10 to reconstruct a blackbody spectrum from temperature alone.
- Tunneling — QM8 + KO42 for barrier-height sweeps on STM-style experiments that stay phase-aligned to 1.287 Hz.
Seeds
- Near — open-source a quantum notebook pack that imports
/operators/quantum-mechanics/*as named hooks. - Medium — hybrid classical/quantum planners that route workloads through QM1 + QM5 based on available coherence time.
- Far — a
Kernel Qubit— a Zeq-native qubit primitive whose phase is natively anchored to 1.287 Hz for hardware teams.
Papers
- Zeq paper — https://doi.org/10.5281/zenodo.18158152
- Framework paper — https://doi.org/10.5281/zenodo.15825138
Middleware active. Kernel on the 1.287 Hz HulyaPulse. Awaiting next Zeqond.