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SMONADSINGLE MONAD · DUALITY OF TIME
عربي
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SIX WAYS INTO THE COLLECTION

Follow a reading path.

Choose a question, then move through a small sequence of connected articles. Every route returns to the full index.

01

Begin with the framework

From the central question to histories, records, and the postulate.

  1. A001The Single Monad Model of the Cosmos
  2. A054The Principle of Ever-renewed Creation
  3. A081One action, two temporal roles
  4. A082When two histories count as the same observation
  5. A085From available records to a temporal arrow
  6. A220The DoT postulate: a compact reading route
02

The historical vocabulary

Read the philosophical background before comparing it with physical models.

  1. A006Time in Greek Philosophy
  2. A007Time in Earlier Islamic Philosophy
  3. A010Introducing Ibn al-Arabi's View of Time
  4. A012Physical Time and Spiritual Time
  5. A033Eternity
  6. A218Reading Ibn ‘Arabi — Time and Cosmology
03

Phase, readout, and the number 137

Follow the algebraic construction, then inspect the physical coupling bridge.

  1. A093Why quaternions appear in the reconstruction
  2. A094The center-blind route to three dimensions
  3. A095Hopf geometry from a spinor doublet
  4. A096Why the symmetric receiver has ten modes
  5. A097Alternating branches and the ranks one, three, seven
  6. A098Two phase actions and determinant closure
  7. A088Why a record count is not yet a coupling
  8. A090The conditional ideal value one over 137
04

How a geometry becomes observable

Move from prepared locality to clocks, cones, and observer transformations.

  1. A123Why local geometry can be statistically rare
  2. A126Six inner stages and one publication interface
  3. A128What spatial readout forgets
  4. A165Why a bare source does not imply spacetime
  5. A166One clock direction plus three readout directions
  6. A167Symmetric cones and causal order
  7. A169When geometric symmetries become physical boosts
05

Constants and independent tests

Separate parameter fitting, prediction, and physical matching.

  1. A099A dependency map for physical constants
  2. A104A common dimensional dictionary
  3. A100Identifiability: can observations determine the model?
  4. A101Prediction after calibration
  5. A102What a failed mass-ratio ansatz teaches
  6. A103Why normalized response misses absolute vacuum offsets
06

From binding to spectroscopy

Start with an atom that binds, then ask what the model can predict.

  1. A171A neutral pair is not yet an atom
  2. A172Eliminating a mediator to obtain attraction
  3. A173Why the Coulomb law requires a continuum input
  4. A174A normalizable hydrogen-like ground state
  5. A176Why binding does not fix the coupling
  6. A182What would count as a DTT spectroscopic residual?
  7. A188Designing an overconstrained atomic test