We determine exactly what a nil-type termination of an admissible description does and does not imply. Failure of a declared chart or continuation map does not by itself collapse nearby admissible states to a discrete set. A finite survivor set follows, for example, when a smooth constraint map between equal-dimensional real manifolds is transverse to zero and its zero set is compact. Discrete spectral values follow under a different hypothesis: a self-adjoint operator on a Hilbert space has discrete finite-multiplicity spectrum when its resolvent is compact. Neither conclusion follows from the nil label alone. These results define a useful MTT discrete survivor filter, but they do not uniquely characterize quantum mechanics. Finite classical state machines, Morse critical sets, symbolic labels, and topological winding sectors also give discrete survivors. Moreover, discreteness does not supply a noncommutative observable algebra, a complex Hilbert space, canonical commutation or anticommutation relations, dynamics, measurement instruments, or the Born rule. Exact finite-dimensional canonical commutation relations are impossible by the trace of a commutator. We therefore formulate quantum mechanics as a conditional reconstruction. Given a complex unital C-star algebra, a positive normalized state, a representation or the associated GNS construction, a dynamical law, and effects or instruments, the standard operator and probability structures are available. Program B3 establishes the discrete-filter and compact-resolvent bridges and records the remaining same-source obligations; it does not derive complex quantum mechanics from nil termination.
We develop a conditionally closed reconstruction of quantum mechanics from exactly three physical axioms: microscopic ontic definiteness and finite localization, physical reality of the spacetime--vacuum substrate, and persistent causal source--response coupling. Wave functions, Hilbert spaces, complex amplitudes, density operators, the Born rule, commutation relations, Fock spaces, path integrals, completely positive maps, and Markovian dynamics are introduced only as derived mathematical or operational structures, not as additional physical axioms. The construction distinguishes the actual finite carrier and its causal history from the quantum state used to represent preparations, transformations, and measurement probabilities. It derives unitary dynamics from self-adjoint Hamiltonians, formulates spectral observables and probability currents, and states the explicit equilibrium, additivity, noncontextuality, and calibration conditions required for the Born representation. Measurement is described through instruments, pointer dynamics, stable records, weak values, continuous monitoring, diffusive and counting trajectories, and operational error--disturbance relations. Quantum trajectories remain record-conditioned predictive representations rather than automatically ontic paths. Composite systems, identical particles, spin, entanglement entropy, purification, steering, Bell correlations, dense coding, and no-broadcasting are developed on declared tensor-product and symmetry domains. Open-system dynamics are formulated through causal Volterra equations, memory kernels, initial-slip terms, auxiliary-mode realizations, and unitary dilations. Existence, positivity, complete positivity, trace preservation, no-signalling, and energy closure are treated as logically distinct properties. Semiclassical pseudodifferential calculus, controlled path-integral convergence, Ehrenfest-time bounds, semiclassical measures, decoherence, and macroscopic-record stability define the quantum--classical interface. Topological phases, defect-bound states, relativistic wave equations, infrared dressing, and effective quantum-field-theory domains are incorporated with explicit applicability and error conditions. Numerical spectral certification, statistical model comparison, twenty-five benchmark models, theorem-status ledgers, and a complete experimental statistical protocol provide falsification and replication criteria. The resulting framework preserves standard quantum mechanics on its validated domain while isolating finite-core and historical corrections as conditional, quantitatively bounded, and experimentally testable extensions. **Keywords** Quantum foundations; topological quantum mechanics; historical memory; three-axiom reconstruction; Born rule; quantum measurement; weak measurement; quantum trajectories; entanglement; spin and statistics; open quantum systems; Volterra equations; semiclassical limit; quantum topology; numerical certification; experimental falsification.
This paper gives a measure-theoretic account of stochastic processes obtained by projecting an upper Modal Triplet Theory evolution. Given a selected probability law on upper initial data, measurable upper dynamics, and an observable map, the projected histories carry a unique path-space law and admit regular conditional kernels. Projection can make the observed process non-Markovian even when the upper process is Markovian or deterministic. The paper separates failure of the observed Markov property, absence of finite Markov order, failure of a chosen classical composition law, and quantum CP-indivisibility. Every classical path law still factorizes sequentially through history-dependent kernels and becomes Markovian on a history state space. An exact binary example has infinite observed Markov order while its memory compresses to one posterior scalar. Exponential action weights define valid kernels when their action and reference measure are supplied, but rewriting a positive kernel in Gibbs form is parameterization rather than prediction. A commutative path-space algebra does not derive quantum observables, Born probabilities, process tensors, or instruments. The remaining MTT task is to select the upper probability source and physical intervention structure from the same geometry.
Modal Triplet Theory (MTT) has established the emergence of quantum mechanics, quantum field theory, spacetime geometry, irreversibility, and cosmology from a common projection-based architecture. While these results are rigorous, their logical necessity has remained distributed across multiple constructions. This paper provides conceptual closure to the MTT corpus. We extract the minimal structural axioms already implicit in the theory, identify a single invariant admissibility margin—coherence capacity—and state a projection–admissibility obstruction theorem from which irreversibility, probability, universality, Hilbert-space structure, and geometric response follow as unavoidable consequences. No new dynamics, degrees of freedom, or assumptions are introduced. The analysis shows that once noninjective projection and finite admissibility are admitted, the qualitative form of observed physics cannot be otherwise. The paper clarifies what MTT does and does not claim, delineates universality classes and breakdown modes, and makes explicit the inevitability that was enforced by the theory’s own internal consistency.
We reconstruct nonrelativistic quantum mechanics from exactly three physical axioms: microscopic ontic definiteness and finite localization, physical reality of the spacetime-vacuum substrate, and persistent causal source–response coupling. The single-run physical state is a finite topological core, its actual causal history, the substrate state, its sector, and the associated historical disturbance. A wave function is not identified with that ontic tuple. It is a ray in a Hilbert representation of admissible preparations and response amplitudes; a density operator is a statistical or reduced representation; and a record is a stable macroscopic event. The logical construction is acyclic. Finite-energy sector spaces and their continuous symmetry representations lead, under explicit representation conditions, to a complex Hilbert direct sum. A closed semibounded quadratic form defines the Hamiltonian and its self-adjoint realization. The standard Schrödinger action, unitary propagation, probability current, spectral observables, uncertainty relations, composite-system tensor products, spin representations, exchange sectors, instruments, and completely positive open dynamics then follow on their declared domains. Gleason-type reasoning fixes the Born form only after additivity, noncontextuality, continuity, and preparation–detector calibration are stated. Those operational conditions are not hidden physical axioms. The distribution of unresolved ontic initial data that realizes quantum equilibrium remains a realization certificate, not a theorem of topology alone. The Heisenberg representation is derived as a controlled transport of observables after Hilbert space and the self-adjoint generator have been constructed. Strongly continuous time translation, two-parameter nonautonomous propagation, common-domain Heisenberg equations, spectral matrix mechanics, regular Weyl relations, open-system adjoints, and instrument effects are connected by one certificate. Schrödinger and Heisenberg predictions are proved equivalent for one-time and finite instrument records, while finite-core, historical, truncation, domain, and detector errors remain separately bounded. Three frozen matrix benchmarks verify low-energy oscillator truncation and its state-weighted CCR defect, second-order unitary convergence for a driven doublet, Schrödinger–Heisenberg equality for a sequential instrument, finite auxiliary-history truncation, and quadratic leakage scaling for a conditional Dirac–Pauli interface. Independent reproduction, including the extended-precision audit, is closed for the frozen packet; physical coefficient calibration remains open. The next interface connects an owner-resolved Dirac–Pauli Hamiltonian to spin records through a Ward-compatible vertex, a causal passive history kernel, an independently audited doublet projection, SPAM-aware forward probabilities, nuisance-profiled identifiability, and a noncompensatory coefficient-to-record error theorem. The DPHC identifiability coordinate is executed on a frozen synthetic response family. A single-scale design is rank deficient, whereas an eighteen-setting frequency–gradient–order–time design has full profiled rank, controlled conditioning, near-nominal finite-sample coverage, and a calibrated held-out statistic. A robust twenty-setting design raises the worst registered information eigenvalue by
20.12%. A ten-parameter nonlinear audit exhibits an exact radiative–detector equivalence curve. An independent dark record breaks that symmetry and restores full local rank. Continuous-set robustness, validated global exclusion, and independent implementation are executed, while physical response identification and empirical calibration remain open. Measurement is treated as a dynamics of system, apparatus, environment, and actual history. Unitary premeasurement and decoherence select robust record sectors but do not by themselves select one record. The three-axiom ontology supplies one actual branch history, while a measurable response map from the complete initial state and instrument to the final record supplies the missing dynamical content. Bell correlations require contextual and nonfactorizable ontic response while parameter independence and operational no-signalling are retained; no controllable superluminal channel is introduced. Historical response produces causal non-Markov Hamiltonians and memory-kernel master equations. Their normalization, positivity, complete positivity, and energy ledger are derived from a unitary enlarged realization whenever such a dilation exists. Finite-core form factors and causal memory yield explicit departures from point-core Markov quantum mechanics. Standard quantum mechanics is recovered as the unresolved-core, sector-fixed, quantum-equilibrium, short-memory limit. Quantum field theory is retained as a successful local, spectral, and asymptotic calculus, but field operators, Fock vectors, and vacuum functionals remain effective representations until a noncircular map from finite carriers and their complete causal histories has been certified. The manuscript proves a sequence of previously open analytic, mathematical, measurement, topological, statistical, and computational obligations on explicitly declared domains. These include non-Markov diffusion, graph-norm stability, distorted-wave and pole variation, finite passive-memory realization, Fisher-information identifiability, detector pushforwards, unique-record basins, Born-representation bounds, measurement independence, topology–Dirac charge conjugation, Stern–Gerlach records, action-scale matching, rank-two spin projection, Finkelstein–Rubinstein topology, Clifford reconstruction, and parent-to-record realization maps. Eighteen groups of numerical obligations are executed on frozen reference models. They cover spectral and scattering calculations, oscillator and two-level dynamics, Schrödinger–Heisenberg equivalence, finite-history truncation, Dirac–Pauli and Foldy–Wouthuysen reduction, gauge covariance, interference, Bell and GHZ correlations, open-system memory, Stern–Gerlach records, identifiability, global searches, topological invariants, path products, semiclassical limits, partial-wave optical closure, the relativistic/QFT interface, and conservative-parent two-level dynamics. Every environment explicitly typed as a computational obligation now has an executed frozen-model certificate; empirical identification and separately typed experimental inputs remain open. The present manuscript differs so substantially from the earlier version in scope, logical architecture, proofs, and executable certificates that it is issued as a new upload rather than as a minor revision. Because the subject is both foundational and technically consequential, readers professionally engaged in quantum foundations, mathematical physics, quantum measurement, or related fields are encouraged to consult both versions: the earlier version preserves the developmental route, whereas the present version gives the substantially expanded and reorganized reconstruction. ## Keywords Axiomatic quantum mechanics; finite particle histories; retarded Green functions; Schrödinger equation; Dirac equation; Born rule; topological spin; quantum measurement; non-Markovian dynamics; classical limit.
Temporal Bell inequalities, such as the Leggett–Garg inequalities, test whether a singlesystem can be described by a time-local realist model. Quantum mechanics violates theseinequalities while preserving operational causality. In this work we give a proof-forwardaccount of temporal Bell inequalities within Modal Triplet Theory (MTT). We show that any temporally factorized realist model satisfies the Leggett–Garg bound.We then demonstrate that MTT generically violates temporal factorization because physicallyadmissible histories are selected by global coherence and fixed-point constraints, ratherthan by independent time-local hidden variables. Despite this failure of temporalfactorization, MTT preserves no-retro-signaling: later measurement choices do not alterearlier observable marginals. As a result, MTT reproduces standard quantum Leggett–Garg violations without invokingretrocausal dynamics or abandoning realism of the underlying modal configuration.Temporal Bell violations and spatial Bell nonlocality are identified as two projections ofthe same global-consistency mechanism. The framework is fully compatible with currentexperiments and standard quantum predictions.