TFPT scientific source excerpt Original repository path: experiments/theory-contracts/foundational-process-classification-20261016/OBSERVABILITY.txt Original file SHA-256: 5253c7df5f3347129e2eb5d8e6bb161d09d9fa19ae64a456ca967eebc7439468 Inclusive original lines: 93-212 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000093 | 4. Countermodel R: deterministic relational readout traces 000094 | 000095 | Primitive description: two preparation events r0,r1 and a repeatable read 000096 | event q. Allowed finite traces after rb are exactly q:b repeated n times, 000097 | for every n>=0. Composition concatenates compatible traces. There is no 000098 | primitive random choice or probabilistic mixture. This is a complete 000099 | deterministic prediction for every experiment in its declared vocabulary, 000100 | not an unweighted envelope with unspecified branching probabilities. 000101 | 000102 | Its two residual classes can be represented by B={0,1}; this is a minimal 000103 | realization of the trace rule. A read relates b to continued b and report b. 000104 | The selective branches M_a are partial identities on {a}. They satisfy 000105 | M_a M_a=M_a and M_0 M_1=M_1 M_0=empty. Identity and these branches exhaust 000106 | the continued-system maps generated here. In particular they commute. 000107 | 000108 | Preparations occur at the beginning. Erasing/discarding the continuing 000109 | system, re-preparing it mid-protocol, arbitrary functions, flips, external 000110 | coins and parallel subsystem operations are NOT part of this minimal model. 000111 | The common benchmark did not require them. They can be added as explicit 000112 | extensions, but that changes the countermodel. R realizes repeatable 000113 | distinctions with no nontrivial probability/convex structure or noncommuting 000114 | continued-system action. Delta-probability notation can describe it; this 000115 | does not make a full probabilistic mixture space necessary. 000116 | 000117 | Discriminator: a controlled rb followed by the opposite report falsifies R 000118 | as specified. Reproducible nontrivial statistical mixtures would require an 000119 | extension of its preparation menu. Nominal variability alone cannot exclude 000120 | every larger deterministic model with hidden preparation contexts. 000121 | 000122 | 5. Countermodel I: quantitative classical information with joint access 000123 | 000124 | Primitive quantitative preparation data are distributions p_ab on four 000125 | joint report assignments (a,b), a,b in {-1,+1}. All convex mixtures are 000126 | allowed. The full joint readout is available. The minimal operational state 000127 | is exactly p because joint outcomes distinguish all its entries. Normalized 000128 | states form a simplex with four vertices, affine dimension3, unique pure 000129 | mixture coefficients. Real probabilities and randomization are explicit 000130 | model assumptions, not derived from observation. 000131 | 000132 | X_a(p)_cd=indicator(c=a) p_cd; Z_b similarly filters d=b. Total X and total Z 000133 | are identity channels; selective X/Z branches commute. They repeat their own 000134 | results, preserve the other value, and permit joint readout/parity Y=ab. 000135 | Allow stochastic transformations and resets as an explicit extension beyond 000136 | readout. Erasure and observation then coexist, so observation does not require 000137 | global information conservation under every allowed transformation. 000138 | 000139 | Define even preparation=(delta_+++delta_--)/2 and odd preparation= 000140 | (delta_+-+delta_-+)/2. Their individual X and Z marginal distributions agree, 000141 | but parity is always+1 in the first and-1 in the second. The serial protocol 000142 | X,Z,X preserves the first X report with probability1. 000143 | 000144 | Discriminator: a genuine loss of the earlier X record caused by intermediate 000145 | Z falsifies these specified nondisturbing I instruments. It does not falsify 000146 | all classical dynamics; an ordinary classical disturbing instrument is an 000147 | alternative explanation. 000148 | 000149 | 6. Countermodel D: operation-generated square with repeatable disturbance 000150 | 000151 | Specify report probabilities and continued responses rather than importing 000152 | a particle or quantum algebra. The complete normalized single-system 000153 | response profile is (x,z) in [-1,1]^2, with 000154 | P(a|X)=(1+a x)/2, P(b|Z)=(1+b z)/2. 000155 | All square-corner preparations, convex mixtures, square symmetries and the 000156 | following instruments are admitted, closed under finite serial/adaptive 000157 | composition and probabilistic coarse-graining. These choices define a 000158 | counterworld; they are not claimed logically necessary. 000159 | 000160 | Use unnormalized v=(t,x,z), t>=0, |x|<=t, |z|<=t. The mass functional is t. 000161 | X_a(v)=((t+a x)/2,(a t+x)/2,0), 000162 | Z_b(v)=((t+b z)/2,0,(b t+z)/2). 000163 | Each branch is positive: s=(t+a x)/2>=0 and the output is (s,a s,0), a cone 000164 | element. The branch masses sum to t. Subsequent same-test outcomes repeat 000165 | with certainty, including X_a squared=X_a and X_-a X_a=0 here. Those stronger 000166 | idempotences are choices in this example, not the general lemma of section3. 000167 | 000168 | Total channels are X(v)=(t,x,0) and Z(v)=(t,0,z). Each destroys the other 000169 | coordinate. The total channels commute (both orders give (t,0,0)); selected 000170 | branches generally do NOT. Do not report all measurement orderings as 000171 | noncommuting. For example X_+ Z_+(1,0,0)=(1/4,1/4,0), whereas 000172 | Z_+ X_+(1,0,0)=(1/4,0,1/4), distinguishable by a subsequent readout. 000173 | 000174 | After X gives a, the normalized profile is (a,0); after Z gives b it is 000175 | (0,b); the last X is uniform. Thus X,Z,X preserves the first X result with 000176 | probability1/2, including on every corner preparation. This distinguishes D 000177 | from the specified I model through an actual common serial protocol. 000178 | 000179 | D has four extreme profiles but affine dimension2. Its diagonal mixtures 000180 | are equal: (++ + --)/2=(+- + -+)/2=(0,0). Every allowed continuation acts 000181 | linearly on unnormalized profiles, so those mixtures give identical answers 000182 | for ALL allowed protocols, not just a sampled list of words. Their images 000183 | in I have different parity. An affine parity effect on D is impossible: 000184 | every affine g satisfies g(++)+g(--)=g(+-)+g(-+), contrary to the desired 000185 | parity indicator values1,1,0,0. Similarly no sharp joint X/Z readout exists: 000186 | its ++ branch would take corner values1,0,0,0, violating the same identity. 000187 | 000188 | The simplex I and square D cannot be isomorphic preserving mixtures and 000189 | all operational answers: their affine dimensions and decomposition fibers 000190 | differ. R has only two predictive classes and no mixture operation, so is 000191 | inequivalent to either enriched theory. Embedding R as a restricted fragment 000192 | of I does not make the complete declared theories equivalent. The models 000193 | are deliberately different operational predictions, not three incompatible 000194 | claims about the hidden ontology of Nature. 000195 | 000196 | D uses the familiar single-system square response geometry of generalized 000197 | probabilistic frameworks, not a derived quantum system. Only the generated 000198 | operations above are admitted: positivity on this cone does not establish 000199 | validity of every positive map on arbitrary multipartite composites. No 000200 | bipartite, spacetime, Bell, locality or thermodynamic completion is claimed. 000201 | 000202 | Indeed D has a classical hidden implementation for these generators: keep 000203 | two hidden bits; an X read reports the first and independently reseeds the 000204 | second uniformly, with the roles exchanged for Z. Readout marginals and 000205 | their future answers reproduce D. Different corner-mixture procedures can 000206 | then have different inaccessible hidden parity although D identifies their 000207 | operational states. No preparation-noncontextuality condition was imposed. 000208 | This is why disturbance or a non-simplex operational quotient alone does 000209 | not exclude all classical implementations or establish fundamental quantum 000210 | structure. I and D remain distinguishable operational theories because I 000211 | admits nondisturbing joint/parity access and D does not. 000212 |