The Artian Hamiltonian Framework for QTT

Reading the Schrödinger Hamiltonian as a laboratory shadow of a real source generator Version: 3.04 Concept DOI: 10.5281/zenodo.20484906 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 Textbook quantum mechanics begins with a Hamiltonian operator acting in laboratory time. This framework asks what that operator is a readout of when the source layer is a finite ledger of completed address events, a real phase rotor, and a capacity ceiling. The source evolution equation is real- \(J\): \[ J_\Sigma\hbar\,\partial_T|\rho_\Sigma\rangle = H_\Sigma^{\mathrm{src}}|\rho_\Sigma\rangle. \] After a declared access window represents the real \(J\)-dial by the laboratory imaginary unit and selects the lab clock, the familiar equation appears: \[ i\hbar\,\partial_{t_{\mathrm{lab}}}\psi = H_W^{\mathrm{lab}}\psi. \] The Hamiltonian constructor order is therefore \[ \text{completed address events} \longrightarrow \text{real }J\text{-source module} \longrightarrow H_\Sigma^{\mathrm{src}} \longrightarrow \text{Access Law} \longrightarrow H_W^{\mathrm{lab}}. \] The no-retune condition is \[ {\partial H_\Sigma^{\mathrm{src}}\over \partial\{\text{observed spectrum},\text{ fitted laboratory constants}\}}=0. \] The paper is a framework for writing QTT sector Hamiltonians: name the completed event set, define the source generator, state the A6/A7 capacity and closure gates, project through access, and then compare with observation.