EXPLORE SMONAD
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66 results · Showing 41–60 · 1560 in the collection
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Space from entanglement and the ER=EPR conjecture
Entanglement can encode geometric connectivity in particular gravitational theories, but a correlated pair is not automatically a traversable wormhole. This comparison calculates how different pairings change accessible entanglement, explains the scope of ER=EPR, and identifies the source-to-geometry dictionary required by SMM/DTT.
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Temporal structure and algebraic quantum field theory
A field theory can be organized by the observable algebras available in spacetime regions. This comparison works through local commuting algebras with a globally entangled state, explains the extra requirements for a continuum field theory, and asks how DTT can generate both the regions and their causal measurement structure.
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Physical clocks and operational time: SMM/DTT and McTaggart’s A-series and B-series
McTaggart’s earlier/later ordering does not assign numerical durations. A clock adds a metric relation among changes, together with a physical procedure for reading it. The comparison develops this distinction through a worked example and explains its implications for SMM/DTT’s nested generation, completed records and account of the observable world.
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Physical clocks and operational time: SMM/DTT and Presentism and the growing-block universe
A privileged present does not tell a clock how fast to run. Presentism and growing-block theories therefore need ordinary physical clock laws unless they add a mechanism of their own. The comparison develops this distinction through a worked example and explains its implications for SMM/DTT’s nested generation, completed records and account of the observable world.
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Physical clocks and operational time: SMM/DTT and Eternalism and the block universe
Relativistic clocks can be represented along worldlines in a block, where proper time depends on the path and metric. DTT’s source-generated clock must recover those relations if its outer world is to agree with relativistic physics. The comparison develops this distinction through a worked example and explains its implications for SMM/DTT’s nested generation, completed records and account of the observable world.
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Physical clocks and operational time: SMM/DTT and The thermal-time hypothesis
Thermal time supplies a candidate flow from a state, but a physical clock must still be coupled and calibrated to that flow. The comparison develops this distinction through a worked example and explains its implications for SMM/DTT’s nested generation, completed records and account of the observable world.
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Physical clocks and operational time: SMM/DTT and The two-state vector formalism
Preselection and postselection are specified relative to physical procedures and times. The two-state formalism does not derive the clocks that locate those procedures. The comparison develops this distinction through a worked example and explains its implications for SMM/DTT’s nested generation, completed records and account of the observable world.
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Physical clocks and operational time: SMM/DTT and Whitehead’s process philosophy
Whitehead’s process philosophy explains temporal order through relations among occasions, but it does not by itself fix the calibrated rate of a laboratory clock. The comparison develops this distinction through a worked example and explains its implications for SMM/DTT’s nested generation, completed records and account of the observable world.
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Dark matter and effective geometry: SMM/DTT and semiclassical gravity
A hidden source contribution must explain more than missing mass in one orbit. Comparing DTT with semiclassical gravity, this article calculates an illustrative enclosed dynamical mass, separates clustered matter from a smooth vacuum component, and identifies the joint lensing and cosmological requirements for a source-based account of effective geometry.
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The auxiliary cycle: exact spectra and their limits
Construct covariant differences on a discrete auxiliary circle, derive the holonomy-twisted spectrum, and understand the constant modes that compactification does not remove.
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Charged thresholds, neutral modes and auxiliary invisibility
Distinguish auxiliary translation charge from gauge charge, show why a charged threshold leaves neutral dynamics open, and state the stronger conditions needed to remove the auxiliary sector.
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Completed records, selector forgetting, and retained references
Analyze the exact standard-form completion channel, its fixed algebra, its erasure obstruction, and the joint reference data that local forgetting must preserve.
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Completion channels: exact erasure, preserved algebras and residual memory
Calculate the spectrum, Kraus form and dilation of the selector channel, distinguish linear invertibility from physical reversal, and test what its fixed algebra preserves.
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When compressed observables form an algebra
Use explicit two- and three-state calculations to distinguish compression, operator systems, corner algebras and closed effective dynamics.
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Connect gauge structure to the rest of SMONAD
A question-led map from gauge records, geometry and dynamics to hydrogen, matter, quantum theory, time, derivations, experiments and philosophy.
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Falsifying a finite model: controls, calibration and predictions kept separate
Design tests that distinguish the exact singlet and channel models from their approximations, calibrate parameters on reserved data, and state precisely what a failed or successful prediction establishes.
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Choose a path through gauge structure
Guided routes from local frames to gauge transport, completed records, exact models, spectral geometry and the constructive lattice programme.
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Gauge research projects for collaboration
Six concrete projects with prerequisites, reproducible starting calculations, expected outputs and explicit criteria for assessing a contribution.
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Gauge research: assumptions, results and open problems
A claim-by-claim ledger for gauge transport, retained symmetry, exact singlet loops, protected geometry, anomalies, vacuum coercivity and continuum identification.
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The vacuum and outer-time reconstruction
Follow the positive transfer operator to its unique vacuum, reversible Markov representation and reflection-positive reconstruction, while keeping finite periodic trace states distinct.
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