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FOUNDATIONS · EXPANDED GUIDE

SMM/DTT glossary: 60 connected definitions

A working reference for the concepts used throughout the foundation guides and article atlas, with links from each definition to a fuller explanation.

Expanded About 14 minutes to read

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The central idea

Use the glossary to keep assumptions, mathematical objects, and physical interpretations distinct. It is organized by topic, and existing term links remain valid.

How to use this glossary

Each entry gives a working definition for this edition and links to a detailed article. Terms such as dimension, phase, completion, and time can refer to different mathematical objects; use the definition attached to the particular construction you are reading.

Definitions describe the role of a concept in the programme. Follow the linked article for its assumptions, worked examples, and the physical questions that remain open.

Framework and temporal roles

Single Monad Model
The proposal that observable multiplicity arises from a common generative source. Its formal development requires source states, operations, retained information, and observation rules. “Single” concerns the proposed origin; it does not imply that all generated records are identical.
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Duality of Time Theory
A framework distinguishing the activity that forms a configuration from its completed observable availability. Different DTT formulations implement that distinction differently, so their state spaces and temporal parameters must be compared before their results are combined.
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Common-source premise
The starting claim that several observable sectors depend on one generative origin. A shared label or controller does not by itself derive agreement between independently chosen laws. The research task is to identify source properties that constrain their agreement.
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Inner generation
The ordered operations through which a proposed configuration is formed. A concrete model represents them through a state update, flow, or allowed compositions, including any memory and controller required. Their iteration labels are not automatically physical clock readings.
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Outer completion
The rule or interface by which a result becomes available as a retained record. A model should state the completion criterion and how it is physically registered. A returning phase is a useful marker only when it is linked to that criterion.
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Six nested inner roles
A hierarchy of functional dependencies, often illustrated by a paired readout with ranks 1,1,2,2,3,3. Higher-level work depends on lower-level activity. These are not six independent laboratory time axes; their necessity depends on the specified architecture.
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Generation order
The order of operations in the source description. It may contain many updates between completed observations. A private scan through an address space need not describe a particle trajectory in the resulting record geometry.
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Record order
An ordering of completed observations or available retained distinctions. To turn it into a physical duration, specify a clock observable and calibration. A record order can also be partial, leaving some events incomparable within the admitted access relation.
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Renewed creation
The historical idea that apparent continuity is sustained through continual renewal. It motivates asking how successive configurations retain recognizable relations. A mathematical account must specify the renewal operation and explain persistence; the philosophical idea alone does not determine a physical update law.
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Physical duration
A comparison made using a specified clock and its calibration. Counting source updates or completed records gives an ordering or a dimensionless count; connecting that count to measured duration requires a reproducible physical clock response and a unit convention.
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Records, dynamics, and observation

History
A permitted sequence or composition of operations. Histories may be distinguished by order, internal state, or accumulated phase even when their present displays agree. Which distinctions matter depends on the completion rule and the admitted future tests.
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Record
Information retained and accessible through a specified observation interface. A record is not necessarily a complete microscopic state. If hidden distinctions affect later accessible outcomes, a predictive description must retain them or represent their effects through memory.
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Observable quotient
The identification of histories or records that the admitted contextual tests cannot distinguish. It supports an autonomous observable update only when that update preserves equivalence. Equality of one immediate measurement is generally a weaker condition.
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Test language
The declared family of preparations, controls, follow-up operations, and measurements used to compare records. Enlarging the family can reveal previously hidden distinctions and refine the observable quotient. It is therefore part of the operational model.
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Congruence
An equivalence relation preserved when equivalent operations are placed in the same allowed compositional context. This condition makes operations on equivalence classes well defined. Without it, the result can depend on an allegedly irrelevant representative history.
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Autonomous dynamics
Evolution generated by the model’s own specified state and law. Any controller, clock, memory, or reset mechanism required to run a schedule must be included in its physical resources. Autonomy does not by itself explain why the programmed rules are selected.
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Retained memory
The part of the state that carries information between operations or completed observations. Its capacity and retention time affect what can be predicted. An unbounded mathematical archive is an idealization that must be identified when discussing finite implementations.
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Completion instrument
A measurement or registration rule with its outcome-dependent state updates. In a quantum model, accepted, rejected, and incomplete outcomes belong to one complete instrument. Conditional successful statistics must be considered together with acceptance probabilities and state disturbance.
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Completion certificate
A specified condition indicating that the intended record has been formed. It may be a consistency check or return to an appropriate state section. Its relation to a phase marker or clock reading must be established by the model.
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Clock observable
A physically specified readout used to compare durations. It may respond to some source operations while ignoring others. A derivation relating time to geometry must define the clock independently and explain why the chosen clock class is physically selected.
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Phase and algebraic structures

Phase
An angular relation carried by an amplitude, representation, or recurrent process. A common phase may be unobservable in one comparison but a relative phase observable in another. The relevant state, transformations, and measurement interface determine its physical role.
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Complex structure
A real-linear operator J satisfying J² = −I. For an orthogonal complex structure, J is also skew-adjoint. It permits a real space to be described using complex scalars, but compatibility with a representation, dynamics, and composition must be checked.
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Split-complex numbers
Numbers u+jv with j² = +1. Their product with the conjugate is u²−v², and hyperbolic transformations preserve this form. They differ from ordinary complex numbers, whose squared imaginary unit is −1; the two roles need an explicit bridge.
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Quaternionic readout
A specified observation or quotient of a quaternionic carrier. The imaginary quaternion subspace has three real dimensions, providing a candidate readout sector. Selecting the carrier and interpreting that sector as physical space require further assumptions and dynamics.
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Real commutant
The algebra of real-linear operators commuting with the given representation. It organizes which phase structures and other transformations are compatible with that representation. The commutant depends on the actual representation and its multiplicities, not only its name.
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Polar phase selection
For an appropriate skew-adjoint generator A, the dynamic sector can admit A = J|A| with J² = −I. In an invertible finite-dimensional example, J = A(−A²)⁻¹ᐟ². Zero modes and infinite-dimensional domains require separate attention.
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Kernel or zero-mode sector
The vectors annihilated by an operator. For a dynamical generator, these are stationary under that generator and may retain phase choices not selected by its motion. Having no exact zero mode is different from a uniform spectral gap away from zero.
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Holonomy
The transformation accumulated by transport around a closed path under a specified connection. Its observable effect depends on the state and readout. A nontrivial internal holonomy can be invisible at an interface that does not retain the relevant distinction.
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Hopf fibre
In the standard normalized complex-spinor construction, a common phase traces a circle above each point of the associated two-sphere. The full bundle has total space S³. A drawing of circles over a sphere is a schematic, not a literal embedding of S³ in three-space.
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Phase balancing
The relation that identifies acting by the selected complex scalar on one factor of a composite with acting by it on the other. Selecting a complex structure on each real factor alone does not automatically supply the standard complex tensor product.
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Geometry and propagation

Adjacency
A declaration that two records are directly connected by a permitted operation or comparison. It can define a graph without assigning coordinates in advance. Which operations count as local neighbours remains part of the source-to-geometry problem.
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Locality
A restriction on which records can directly interact or influence one another, relative to a specified geometry and dynamics. Constructing a local graph shows possibility. A physical account must explain its selection, stability, and relation to signal propagation.
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Readout rank
The number of independent directions in the image or affine span of a specified readout. It is an algebraic property of that map. It need not equal a spectral dimension, a scaling dimension, or the dimension measured by every physical probe.
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Record-scaling dimension
A dimension obtained from how distinguishable records and their measured scales change under refinement. In a regular model with B children and scale ratio q, the exponent is log B/log q under the declared metric assumptions.
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Spectral dimension
A scale-dependent dimensional diagnostic extracted from a return probability or related spectral quantity. For example, a logarithmic slope can measure diffusion behaviour. It does not by itself provide a unique metric or establish physical spacetime dimensionality.
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Spectral distance
A distance reconstructed through a specified algebra, representation, and operator. Its normalization and operator weights matter: changing them can change distances while leaving the underlying labels unchanged. A physical interpretation must identify the relevant measuring procedure.
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Lorentz cone
The cone of pairs satisfying t ≥ ‖x‖ in a normalized Euclidean readout. Positive two-by-two Hermitian matrices give a standard algebraic realization. Connecting its coordinates and symmetries to physical clocks and observers requires additional input.
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Causal cone
The allowed relation between delay and influence or displacement in a model. A finite propagation bound constrains causal access, but its coefficient need not equal a band group velocity or a universal signal speed without a connecting argument.
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Refinement
A controlled change in resolution or record organization. A useful refinement law states how counts, lengths, clock readings, and dynamics transform. Comparing settings with separately refitted parameters cannot establish a common scaling prediction.
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Continuum limit
A limiting procedure in which discretization or resolution scales change while specified observables converge. The topology, normalization, uniform bounds, and retained physical scales must be stated. A fine lattice picture alone is not a controlled continuum derivation.
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Constants, matter, and matching

Structural 137
The exact integer obtained from a selected grammar such as Qd = 10Qd₋₁ + (2ᵈ−1) at d = 3. Its reciprocal becomes a coupling only after a response law and physical normalization are selected. The counting identity and the matching claim are distinct.
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Receiver
The specified space or map that retains a chosen set of source distinctions. A symmetric second-power receiver on a four-real-dimensional carrier has ten modes. The word describes an operational role; it does not itself select that particular representation.
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Response capacity
For a positive invertible operator K and source f, the quadratic response C = ⟨f,K⁻¹f⟩. It depends on both K and f. Rescaling K changes the response without changing the number of carrier modes, so dimension alone does not fix it.
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Physical matching
The identification of model variables, operators, and scales with measured quantities. It should specify units and the comparison procedure. The research is strengthened when a relation previously supplied by matching follows from the selected source dynamics.
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Calibration
The use of specified observations to fix units, parameters, or a response dictionary. Predictions should then use the same fixed choices for observables not used in that calibration. Calibration is a legitimate modelling step when its role is stated.
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Action scale
The factor converting a dimensionless phase or generator convention into physical action units. A phase-selection theorem need not determine its numerical SI value. A proposed derivation of ℏ must identify the independent dimensional standards and avoid reusing the target.
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Reduced mass
For two particles of masses m₁ and m₂, μ = m₁m₂/(m₁+m₂) is the inertial coefficient of their relative coordinate in the standard two-body reduction. Relative velocity and the velocity of one constituent are therefore generally different.
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Bound state
A normalizable state localized by the specified dynamics, with an appropriate spectral position relative to scattering states. Neutrality alone does not establish binding. A proposed atom needs both the interaction and kinetic structure that support its states.
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Mass gap
A strictly positive separation above the vacuum in the relevant physical spectrum. A finite-system gap, an effective screening scale, and a uniform continuum quantum-field-theory gap are different claims and require different hypotheses and limiting arguments.
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Gauge invariance
Invariance of physical quantities under changes of redundant description. It constrains admissible operators and comparisons. Choosing a particular Hamiltonian, coupling, or representation may still require additional dynamical input beyond invariance alone.
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Reasoning and research methods

Conditional result
A conclusion established under specified hypotheses. The proof can be exact even when the physical selection of its assumptions remains open. A later advance may derive one of those hypotheses from a smaller or more unified source specification.
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Independent prediction
An observable consequence obtained after relevant inputs are fixed elsewhere, without adjustment to the target outcome. A useful comparison also includes uncertainties and alternative explanations. Reproducing the quantity used to fit a parameter is not an independent prediction.
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Memory kernel
A function or operator weighting the influence of past visible states on present reduced evolution. Eliminating hidden variables can generate it from a larger local system. The existence of memory does not by itself establish dissipation or another readable clock.
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Identifiability
Whether different allowed model parameters or structures can be distinguished by the specified observations. If many choices produce the same outcomes, those observations cannot select one of them without additional constraints or measurements.
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Countermodel
An explicit model satisfying stated premises while failing the proposed conclusion. It identifies a missing assumption or shows that a necessity claim is too strong. It can also reveal which physical freedom a more informative theorem should remove.
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Necessity or selection theorem
A result showing that the stated assumptions require a structure or exclude specified alternatives. It is stronger than giving one example with the desired property. The admitted model class and the equivalences used to compare solutions are part of the statement.
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Realization
An explicit model implementing a proposed architecture or set of relations. It demonstrates compatibility and can support exact calculations. It does not alone show that the chosen architecture is unique, natural, or physically selected.
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Stability
Persistence of a stated property under a defined class of perturbations or over a specified evolution interval. Stable memory, a stable local graph, and a stable bound state concern different objects. The perturbation norm and the controlled quantities must be identified.
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Coarse graining
A map retaining selected distinctions while omitting others. The reduced description may require memory if the omitted information affects later visible outcomes. Its entropy and irreversibility properties depend on the state, dynamics, and observation rules.
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Resource budget
The declared limits on memory, energy, precision, preparation, control, and reset operations. It makes the physical cost of a construction visible. An unlimited archive or externally prescribed schedule should not be hidden inside an apparently autonomous finite source.
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A compact notation guide

Symbols are defined locally
SymbolMeaning in these foundation guides
UAn update or evolution operator; its state space must be stated.
ΠThe map from complete histories to accessible records.
JA real-linear complex structure with J² = −I.
jThe split-complex scalar unit with j² = +1.
B, qChild count and scale ratio in the regular refinement example.
DA specified dimension or scaling exponent; identify which one.
T, τClock readings or timing variables as defined in the relevant model.
K, fA response operator and source vector in C = ⟨f,K⁻¹f⟩.
μReduced mass in the hydrogen discussion; elsewhere a mass-ratio symbol may use the same letter.
α₀The ideal-model coupling label, not an automatic renormalization-scale assignment.

A symbol can have a different meaning in another paper. Translate its definition, dimensions, and measurement role before combining equations from separate constructions.

Further reading

Continue with the individual articles and their source references.

  • One action, two temporal roles

    Inner generation and outer record order can be roles of one process. A completed return becomes an observable advance only when its action respects the retained records and their tests.

  • When two histories count as the same observation

    Completion identifies histories that leave the same record, while observation identifies records that available tests cannot distinguish. Their combined quotient is consistent only with the declared operations and contexts.

  • The center-blind route to three dimensions

    Removing the scalar center of a quaternionic carrier leaves a three-dimensional readout space. Accessible rotations or a suitable finite acquisition protocol are needed to ensure that detectors actually recover all three directions.

  • From record refinement to a joint clock–band relation

    Independent count, scale, phase, clock, and band measurements can satisfy a joint refinement relation under the supplied interfaces. The ungated-clock alternative identifies why the protected-clock premise remains essential.

  • Six inner stages and one publication interface

    A six-digit nested counter with paired signed readout realizes ranks 1, 1, 2, 2, 3, 3 before one completion interface. Its exact counts reveal sampling bias and the restricted assumptions behind the six-channel bound.

  • Why a bare source does not imply spacetime

    A structureless source cannot select a nonzero metric, an oriented vector or a proper causal cone while preserving every change of representation. Recurrence, composition and observable readout supply the additional structure needed for an SMM/DTT reconstruction.

  • Real-commutant phase selection: a paper guide

    An oriented real orthogonal flow can select an ordinary complex structure on its dynamic sector. Planar examples explain residual zero-mode freedom, time-reversal antilinearity and the extra balancing rule needed for composite systems.

  • Temporal asymmetry: reading the published model

    The temporal-asymmetry model connects projected dynamics with memory and path dependence. A solvable hidden-mode example distinguishes those effects from dissipative stability and from evidence for a second observable clock.

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