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Bell nonlocality and causal structure: SMM/DTT and relational quantum mechanics

Bell correlations challenge a particular local causal factorization while preserving ordinary no signalling. Comparing DTT with relational quantum mechanics, this article calculates the ideal singlet violation and its unchanged local marginals, then asks what a single generative source must explain to reproduce both features through one physical mechanism.

In this article
  1. The question behind this comparison
  2. The SMM/DTT starting point
  3. How the comparator works
  4. The decisive comparison
  5. Worked benchmark
  6. What follows for the source programme
Key ideas · Continue on SMONAD

01The question behind this comparison

Bell inequalities test restrictions on correlations, not the speed of an observed signal. In the usual local causal model, outcomes at two separated laboratories become independent once the relevant common cause and local settings are specified. Measurement-setting independence is another premise. Quantum states can violate the resulting bounds while preserving the inability to transmit a controllable message by changing a distant measurement choice alone.

A Single Monad is naturally a common origin for records, but a common origin by itself does not evade Bell’s argument: the hidden variable in a Bell model already represents an arbitrarily rich common cause. The decisive issue is the form of the conditional probabilities. A DTT account must specify whether its source violates factorization, changes a setting-independence assumption, or uses a different causal structure. An inaccessible inner ordering is not an automatic explanation of the observed correlation law. [3] [4] [5]

02The SMM/DTT starting point

The Single Monad Model begins with one nonspatial generative source. The Duality of Time Theory distinguishes the source’s inner production from the outer order in which completed records become accessible. Its six inner levels are nested functional roles of one process: a higher role organizes lower-level work. The seventh is the completion or observation interface. They are neither six independent clocks nor six additional time coordinates.

This distinction supplies a useful research question: which features of an observed world can follow from the way a source produces, retains and releases information? A concrete answer needs a state space, an autonomous update, retained memory and a rule connecting completion to an accessible measurement. In the constructions discussed here, those mathematical ingredients are stated explicitly. A successful finite example establishes what its specified mechanism can do; further arguments connect it to physical particles, spacetime or universal laws. [1]

From a source process to a complete record instrument
From a source process to a complete record instrument. Outcome probabilities, retained conditional states, and the outcome-averaged channel belong to the same instrument. Keeping every outcome prevents postselection from being mistaken for a signal. View full size ↗

03How the comparator works

Relational quantum mechanics treats physical quantities and state assignments as relative to interactions between systems. An observer is any relevant physical system, not necessarily a conscious mind. What is definite relative to one system need not be represented by the same state relative to an external system that has not yet interacted with it. Communication and subsequent interactions are part of the physical account of how records are compared.

DTT’s separation of generation from accessible records can be formulated in this language when completion is indexed to a receiving system. A universal outer archive, by contrast, would add an observer-independent structure beyond Rovelli’s original proposal. Neither choice is settled merely by saying that observations occur. The useful comparison concerns exactly which system retains a record, which interactions make it accessible, and which consistency conditions connect descriptions. Relational quantum mechanics does not derive the six inner levels, while their presence alone does not decide whether completion should be universal or relational. [2]

04The decisive comparison

Relational quantum mechanics interprets Bell outcomes as facts relative to local interactions, with their joint correlation established when records are compared. This does not erase Bell’s statistical constraint: the comparison must still reproduce the nonclassical joint distribution. DTT agrees that the observer-facing world is constituted by accessible records, but it can add a common source history behind those relations.

Whether that source has an absolute simultaneous completion is a separate question. A universal release time is not licensed by the fact that observers eventually agree about correlations, and a local readout must not acquire remote setting information before communication. The worked singlet example separates those issues: the joint distribution violates the local bound, while each accessible marginal remains uniform. A DTT model with relational completion could derive both from a shared process without a preferred public simultaneity. One with an absolute hidden order must show how that order remains absent from accessible signalling. The useful comparison is therefore about the compatibility of records and causal access, rather than an appeal to observers that bypasses the Bell assumptions. [2] [3] [4] [5]

05Worked benchmark

For a spin singlet, the correlation of ±1 outcomes along unit vectors a and b is E(a,b)=−a·b. Choose a=z, a′=x, b=(z+x)/√2 and b′=(z−x)/√2. In the CHSH combination E(a,b)+E(a,b′)+E(a′,b)−E(a′,b′), the four terms add to −2√2, whose absolute value exceeds the local bound 2.

Each local outcome remains equally likely. Indeed the reduced state at either wing is I/2. A distant trace-preserving operation leaves the local reduced state unchanged when its outcome is not conditioned upon. Correlation beyond the Bell bound and no signalling therefore coexist in the same calculation. This is the benchmark for temporal source proposals: a mechanism must reproduce both facts. Explaining only the strong correlation while allowing the remote setting to change a local marginal would describe a different, experimentally constrained theory. [3] [4] [5]

|S|=2√2 for the ideal singlet; p(a|x,y)=p(a|x)=1/2

CHSH outcomes are ±1. The local bound presupposes local factorization and suitable independence of measurement choices from the common cause.

06What follows for the source programme

The strongest use of DTT here is to make the hidden production architecture precise enough that its causal assumptions can be inspected. A source update that coordinates records may be nonlocal at the underlying level while yielding a relativistically admissible observable interface. That is a substantive possibility, but a claim of compatibility requires the interface calculation. Existing Bell violations support the quantum correlation structure, not a unique ontology of its origin. [3] [4] [5]

THE SAME QUESTION, DIFFERENT STARTING POINTS

The comparison at a glance

QuestionSMM/DTTrelational quantum mechanics
Starting structureOne nonspatial source, retained memory and six nested inner functions with an outer completion interface.Interactions among physical systems and relative state assignments.
Observable connectionThe source update and readout must generate the measured records and their calibrated relations.A record is a fact relative to its interacting receiver.
Bell nonlocality and causal structureWhether that source has an absolute simultaneous completion is a separate question.Relational quantum mechanics interprets Bell outcomes as facts relative to local interactions, with their joint correlation established when records are compared.
Status of the claimA constructive research programme; a specified finite model establishes only its stated conditional results.Relational interpretation does not require a privileged conscious observer.

KEEP THE CONNECTION

Key ideas

  • The strongest use of DTT here is to make the hidden production architecture precise enough that its causal assumptions can be inspected.
  • Six inner levels are nested functions of one source; the seventh is its accessible completion interface.
  • A new physical prediction requires a constrained mechanism and a measured observable beyond a change in interpretation.

Continue on SMONAD

Sources and further reading

References support the comparator and the specific mathematical or interpretive claims indicated. SMM/DTT connections are developed in the analysis above.

  1. Mohamed Haj Yousef, Six inner stages and one publication interface (SMONAD, 2026) ↗Author’s explicit nested-level counter example and limitations of its six-channel lower bound.
  2. Carlo Rovelli, Relational Quantum Mechanics (1996) ↗Original interpretation: states and facts relative to interacting physical systems.
  3. B. Hensen et al., Experimental loophole-free violation of a Bell inequality using entangled electron spins separated by 1.3 km (2015) ↗Primary Bell experiment, including assumptions, data analysis and finite-sample statistics.
  4. Fabio Costa and Sally Shrapnel, Quantum causal modelling (2016) ↗Original quantum causal-model framework; operational interventions and causal structure.
  5. E. B. Davies and J. T. Lewis, An operational approach to quantum probability (1970) ↗Original quantum-instrument framework; measurement probabilities and conditional operations.

How these comparisons distinguish premises, results and physical claims

SMONAD

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