The predicate ledger of the corpus: the master ledger 00 and the ledger of every public paper, one predicate per row. A row is cited by its ledger and label, as 00:A1 or 35:P11, and each label opens the row in its own ledger. The accession key pNNNNN stays fixed while labels may move, and register.html#pNNNNN opens its row. The Filters choose a paper, a block and a status, and the search runs within the choice. Across all papers, a prediction or an explanation stated in more than one paper is listed once, at its first appearance, with its restatements linked.
Filters
| # | Predicate | Status | Sources |
|---|---|---|---|
| A. Foundation: from existence to the finite carrier | 8 7 1 | ||
| A1p00001 | The Universe exists: the sole indubitable given (“I think, therefore the Universe is”). Neither axiom nor assumption. | G | |
| A2p00004 | Finitude: the Universe is the totality of its registered manifestations (A8). For any totality and any reading of capacity $R$, the registered Universe embeds in the shell of $R$ members, and among any $R+1$ members two share a residue (5:C2, 29:C1, 29:C2): the Universe is finite, its structural cardinality $\Om$ (A7). | T | |
| A3p00003 | Completeness of the totality: whatever exists is registered within — the registration of any totality is onto its registered Universe (A8) — so no outside (A8), no host (A1). Unique: two totalities each registered whole within the other have one count (5:C2 both ways), one count one Carrier (A6). No proper closed substructure (A10). Observers are parts within (A4). | T | |
| A4p00197 | Incompleteness of observation: every observation is a registration by an embedded part (C4, A13) of cardinality $\p<\sqrt\Om$ (A6, B8): every reading identifies two members (25:D1, 5:C2) — an incomplete projection, complete only at the whole count. No frame sees more: one translation carries each member to each, one affine map each frame to each (A6, 1:C2). Horizon: Z1, Z9. | T | |
| A5p00188 | Counting closes by return: the successor $C_q:x\mapsto x{+}1\ (\mathrm{mod}\ q)$ on $q\ge2$ points is one $q$-cycle with no fixed point, so iteration is bounded and cyclic; its interpretation is A2’s. | T | |
| A6p00008 | The Carrier C: A timeless torsor of $\Om$ elements, its cardinality is its only absolute characteristic; reframings $x\mapsto ax+b$ are automorphisms, so $0,1,-1$ are frame data; a Subject’s frame charts it as the prime field $\F_\Om$ — the frame’s chart, never the Carrier (C1). Arena and numbers: B1. | D | |
| A7p00009 | Scale, the sole quantitative import: the de Sitter entropy of the observable universe fixes the cardinality exactly, $\Om=4\dS+1$. Its chart numeral is $\dS=\pi(r_H/\ell_P)^2=3.3\times10^{122}$ [chart] at $r_H=c/H_\Lambda$ (14-entr), so $\Om=1.3\times10^{123}$ [chart]. The Carrier congruences are certified by the realisations (B5, C8), not imported. Metrology: L2. | I | |
| A8p00010 | Realisation, not correspondence: a sufficiently expressive, predictive, registration-complete structure is its subject, not an abstraction of it. By the incompleteness of observation (A4) no registration reaches an unregistered reality, so a distinction with no registered residue is no distinction. Identification rows (R) are therefore constitutive: defended by the totality of registered consequences, killed by explicit falsifiers. | D | |
| A9p00161 | The trusted base: the kernel’s type theory, with the prelude’s natural numbers read as the index of shells; no core statement asserts unboundedness, and no step of a certificate computes a count above $\Om$ at any admissible instance. | D | |
| A10p00162 | Completeness is primality: the residues of a count $q\ge2$ have no proper nonzero ideal iff $q$ is prime, so the arithmetic of a counting cycle is complete exactly on prime cycles — the formal shadow of A3, since a proper closed substructure of the totality would be a second totality within it. | T | |
| A11p00163 | The quarter-turn exists iff $\p\equiv1\pmod4$: for an odd prime $\p$, $-1$ is a square in $\F_\p$ iff $\p\equiv1\pmod4$ (the formal shadow of B3). | T | |
| A12p00164 | Every prime carries a frame: every prime field $\F_\p$ of the totality has a primitive root, so a drive $\gen$ with $\langle\gen\rangle=\F_\p^{\times}$ exists (the formal shadow of C1). | T | |
| A13p00196 | Labels and support: a reading’s labels $\mathcal L_i$ count distinctions only through their support $\rho_i{:}\mathcal L_i\to\Om$; labels with one support are one distinction, so the distinctions realised are the quotient $\mathcal L_i/{\sim_i}$, and labels may outnumber them without adding one (A4). | D | |
| B. The Carrier: the substrate structure | 5 5 | ||
| B1p00011 | All numbers are unframed Carrier residues, framed rationals ($\fQ$) in a Subject frame, in which every structure the sciences use is built exactly. The continuum is a labelled idealisation read against $\mathbb R$ [chart], never an object. The accessible smalls are the counts below the observer’s horizon, the wrap-free window of primality, parity and order (B8, B9). | D | |
| B2p00012 | Phase cycle $\Phi=\F_\Om^{\times}\cong C_{\Om-1}$, the split torus of order $\Om-1=4\dS$; the cycle’s order and divisor lattice are frame-invariant (the arithmetic of $\dS$ is the spectrum of admissible dynamics), its marked elements frame data. | D | |
| B3p00013 | Quarter-turn torsion: $4\mid\Om-1$ by construction ($\Om=4\dS+1$, A7), so the split torus carries a unique order-four subgroup — the Carrier’s $Q_4$ core $\{1,\hbar,-1,h\}$ ($\hbar^2\equiv-1$, $h:=-\hbar$ the root-pair partner of $\hbar$, B7), the symmetry-complete condition. The Subject’s labels $\{1,\im,-1,-\im\}$ are frame data (C1), the two quarter-turns distinct objects (D7). | D | |
| B4p00014 | Triality centre: $3\mid\Om+1$, so $x^2+x+1$ has no root in $\F_\Om$, and its roots $\omega,\omega^2$ with $1$ form the unique order-three group of norm-one residue pairs, the triality centre; its labels $\{1,\omega,\omega^2\}$ are Subject frame data (C1); jointly with B3 it forces the substrate residue (B5). | D | |
| B5p00015 | The substrate residue: the quarter-turn ($4\mid\Om-1$, B3) and the triality centre ($3\mid\Om+1$, B4) jointly hold iff $\Om\equiv5\pmod{12}$. Both are relations certified by realisations, never properties of an integer: $Q_4$ by the quantum realisation (D4), the triality centre by the strong realisation (D6). The inference runs structure $\to$ congruence (A3); a laboratory pattern instantiates the residue or does not (10:E9). | T | |
| B6p00016 | Four generative levels (succession $\to$ addition $\to$ multiplication $\to$ fixed-base exponentiation) generate the carrier’s two cyclic structures ($C_\Om$, $C_{\Om-1}$) and the exponential bridge lemma; the fifth level (tetration) folds back since exponents are $(\Om{-}1)$-cardinality residues, so the hierarchy, unbounded under the classical reading, closes at four over $\F_\Om$ (structural, not a cost claim). | D | |
| B7p00165 | Physical constants are definite Carrier residues: the register $\{\dS,\Om,c,\hbar,G,k_B\}$ is generator-free in $\dS$ alone — $G=2\dS=-c^2$, $c^2=2^{-1}$ (C8, D7), $\hbar^2=-1$, $k_B^2=-2$, $|k_B|=\hbar/c$; the defining congruences are the observer’s complete certificates, $G$ exact, the rest up to sign (B10); $h:=-\hbar$ is the root-pair partner of $\hbar$ (B3, D7). No Subject counterpart of $G$ or $\hbar$; no fifth constant (C1). | T | |
| B8p00166 | The window ladder: a nested Subject, $\p^2<\Om$, has its own horizon below the Carrier’s quarter-root, $\sqrt\p<\Om^{1/4}$, and its shell below the coherence horizon, $\p<\Om^{1/2}$; the saturating Subject ($\p^2\to\Om$) locks the ladder $\mathrm{small}<\Om^{1/4}<\p\text{-hard}<\Om^{1/2}<\Om\text{-hard}<\Om$, one square-root horizon per embedding (the bands: B12). Lab-verified ($\Om=2{,}408{,}561$). | T | |
| B9p00019 | Certification is the orthogonal axis to the B8 bands: a certified entity carries a bounded-height defining relation holding across shells; a framed transcendental is a hard role with none. Registers: at the Carrier the four constants (B7); at the Subject the half-period and quarter-turn, $2\pi\equiv-1$, $\im^2\equiv-1$ (C1) — the same congruence shapes (self-similarity). Physical constants $\Om$-hard, mathematical constants $\p $-hard. | D | |
| B10p00168 | One gauge bit closes the sign sector: no C14-type marker exists — $-1$ is a square on admissible $\Om$, so square class is pair-blind, and integer parity is frame data (A6). Registered faces are pair-invariant: $c^2$, the one-way member synchronisation gauge (C8); $|k_B|$ (C12); $\{\hbar,h\}$ the two named unit faces (B7). | T | |
| B12p00167 | The two-level horizon law: hardness is one mechanism at every scale — a role is $\Om$-hard when it lives at the Carrier’s scale, $\p$-hard when it lies beyond the Subject’s own horizon $\sqrt\p$ inside its own shell; hardness attaches to roles, never to bare residues. The ladder: B8; certification: B9. | D | |
| B13p00169 | The sign of the Boltzmann residue: $k_B:=-\hbar/c$, the sign fixed by the Hawking scaling $k_Bc=h$ read in the chart [chart]; the registered face is $|k_B|$ (B10). | D | |
| B14p00170 | The octant sector: $C_8\subset C_{4\dS}$ exists exactly when $\dS$ is even (14:C6). | T | |
| C. The Subject: the frame and its registration | 13 13 | ||
| C1p00021 | The frame, Subject-only: $(\chron;0,1,\gen)$, origin, unit and the drive $x\mapsto gx$ (A6). Shell data, capacity-first: $\kap $ primitive, $\p =4\kap +1$, $\im=-\gen^\kap $ (C7), $\pi=2\kap $, $e=\gen^{\,\im}$; $\gen$ the one nonsquare frame datum (C3, C8). Exponents of $\gen$ are taken in $\Zp$, a residue in an exponent standing for its lift $\iota:\F_\p\to\{0,\dots,\p-1\}$. The web closes on every shell: $2\pi\equiv-1$, $\gen^{\,\pi}\equiv-1$, $-\pi=2^{-1}$ (N2). | T | |
| C2p00022 | Scale-shift duality: dilation $x\mapsto gx$ is phase evolution of the frame, advancing $t$; over the cycle it is the fractional Fourier transform, whose quarter-turn $Q_4$ is the discrete Fourier transform. | T | |
| C3p00150 | Euclidean--Lorentzian dichotomyThe drive fixes a Lorentzian time axis, causal order is algebraic, the split and non-split tori the two signatures. The signature is the square class of the temporal coefficient $\nu=\gen$ (C1); in $\F_\p$, $\nu=2^{-1}\cdot(2\gen)$, both classes fixed by the parity of $\kap$ (8:B3). In the Carrier $c^2=2^{-1}$ is a square (C8, D7), and $\eta_{00}=-c^2$ is a chart artifact. | T | |
| C4p00024 | Observer $=$ embedded shell (frame); observation $=$ shared-core comparison of two phase cycles. | D | |
| C5p00025 | Oriented frame $=$ unimodular basis; two oriented frames differ by exactly one matrix of determinant one. | D | |
| C6p00171 | One frame group, three sectorsGravity’s $(3{+}1)$ tensor, the Riemann observer geometry and the quantum spinor structure are three readings of a shell’s frame group $\mathrm{SL}_2$ (C22), element by element, its three tori the scale-time, translation and boost freedoms; continuum shadow the declared $S^3$ (C23), spinor double cover the Clifford layer (D4). Falsifier: a registered space-time, observer or spinor freedom outside the three tori. | R | |
| C7p00189 | Orientation is derived, not conventional: the $c$-square congruence ($\dS$ even, C8) annihilates orientation transport on every Carrier carrying it ($\im^{\dS}\in\{\pm1\}$); the oriented quarter-turn $\im=-\gen^\kap $ is a selection, read by pullback covariance and count positivity; the joint flip $(\gen,\im,s)\mapsto(\gen^{-1},-\im,-s)$ permutes the registration channels. The constants’ derivation consumes no selection (B7). Parity marker: C14. The selection by matter content: D16. | T | |
| C8p00028 | The square class is chronon parityFor a primitive drive the squares are $\langle \gen^2\rangle$: a residue’s quadratic class is its drive-step parity. Registered transport is even, the one-way multiplier $\gen$ odd, so the one-way speed is gauge and the two-way constant invariant. $[c^2]$ is even iff $\dS$ is even, a relation certified by the unit realisation (D7). The Tsirelson $\sqrt2=\zeta_8+\zeta_8^{-1}$ is its two-way symmetrisation. | T | |
| C9p00029 | The Object frame is $(\dt;\,q,k,v)$: every entry a Subject residue — offset $\dt$ (synchronisation datum), position $q$, winding $k$ (D2), rate $v$; one relative datum per frame datum. The momentum reading is one quarter-turn from the winding, $p=\im\,k$; the canonical commutator $[\hat q,\hat p]=\im\hbar$ composes the Subject’s chart quarter-turn with the Carrier’s action quantum (D7, B7). | D | |
| C10p00030 | Two strata of probabilityA registered probability is a framed rational; a structural weight is an element of the parity-even cyclotomic subring. The strata coincide exactly on the stationary core-valued $Q_4$ sector, joined by two proved reductions and the stratum-sampling clause (D10). On a single Object the weights are uniform over the fibres (22-qm Rem. borndomain); non-uniform statistics arrive through the engineered-core readout. | T | |
| C11p22028 | Pair-tally uniqueness (22-qm Prop. gleason, the uniqueness of the pair tally on the stationary $Q_4$ sector): on the stationary core-valued $Q_4$ sector, tally-valued, fibre-additive, drive-invariant, parity-even registration functionals form the character cone fixed by the pure windings; adding channel-selectivity (assumed, not derived; the sampling clause D10) picks the Born ray. The minimal degree is forced; proof shape: 22-qm. | T | |
| C12p00032 | Temperature and the classical arity, derived: the temperature domain is acceleration, $[\Theta]=[E][k_B]^{-1}=[L][T]^{-2}$, flag-free, $\Theta_P=E_P/|k_B|$, Unruh closing as a domain identity; neither mass nor temperature is primitive — $M$-$L$-$T$-plus-thermal is the torsion-free shadow of the two-generators-plus-flag system (the mass primitive standing in for the flag, the thermal for $k_B$), classical dimensional analysis recovered in exponents and arity. | T | |
| C14p00034 | The quarter-turn is the odd member of the $\pm\sqrt{-1}$ pair: the two representatives have opposite integer parity (distinct from chronon parity, C8), and $e^{\,\im\pi}:=\gen^{\,2\kap\,\iota(\im)^{2}}\equiv(-1)^{\iota(\im)}$ (the lift $\iota$ of C1), so $e^{\,\im\pi}\equiv-1$ holds exactly on the odd member. The conjugate chart toggles it: the parity names the matter–antimatter gauge (C7), and the selection is generator-independent within the chirality. | T | |
| C16p00151 | The spinor dichotomy: $\kap$ odd $\Leftrightarrow$ $C_{\p-1}\cong C_4\times C_\kap$ $\Leftrightarrow$ $v_2(\p-1)=2$ $\Leftrightarrow$ $3\kap r+4s\equiv1\ (\mathrm{mod}\ 4\kap)$ is solvable: the spinor class. Shell and Carrier share the $2$-part $C_{2^m}$, $m=\min(v_2(\p-1),v_2(\Om-1))$, and the shell closes on a cover of degree $2^{v_2(\Om-1)-m}$; the shared order times the cover degree is the Carrier’s $2$-part, $8$ exactly when $\dS\equiv2\ (\mathrm{mod}\ 4)$. The midpoint event of a $\kap$-odd shell: 38:C14. | T | |
| C19p00190 | The Hopf section: on the frames by elements (no group counted, Q20) the boost torus $C_{\p +1}$ is fixed-point-free on $\mathbb{P}^1$ and meets the Borel trivially, so every frame factors uniquely as (cone-chart event)$\times$(boost): the cone chart is a global section of the non-split fibration (C22), $\p (\p -1)$ fibres of $\p +1$; $\mathrm{SL}_2$ obstructs at $-1$. | T | |
| C20p00040 | The mass–energy channel: the winding sector $C_{\p -1}$ meets the boost base $C_{\p +1}$ in the sign alone and the spinor cover $C_{2(\p +1)}$ in exactly $Q_4$, every $\p =4\kap +1$; the quarter is spinorial, $N(\im)=\im^{2}=-1$: the mass transport crosses the sheet; mass phase $=$ winding rate, one $Q_4$ datum (D2); Carrier instance $78^{58}=89=h$ on $\Om =233$ (38:A4). | T | |
| C21p00041 | The dilation rigidity theorem: static clock comparison is a register character $\gen^{-\Delta n}$; characters are rigid, so the strong-field dilation law is the unique exponential reading, zero coefficient freedom; the PPN temporal form admits no register character (transitivity defect exactly $4ab$); the cover halves the angle at every tick (C20). | T | |
| C22p00152 | The frame variety and its two fibrations$\mathrm{PGL}_2(\F_\p)\cong\mathrm{SO}_3(\F_\p)$; the norm-one sphere is $\mathrm{SL}_2$, the spin cover of $\mathrm{PSL}_2$, whose elements are frame moves, not registrations. For every $\p=4\kap+1$ of the totality each element is one direction in $\mathbb{P}^1$, one shell cell and one drive phase. Two fibrations partition the variety: non-split $C_{\p +1}$ over $\p (\p -1)$, with the cone-chart section (C19), split $C_{\p -1}$ over $\p (\p +1)$ without. | T | |
| C23p00182 | The spatial chart is the 3-sphere (declared)$SU(2)=S^3$ is declared the continuum chart of the frame group (C27) [chart]. The group has the three element types of $\mathrm{SL}_2(\mathbb{R})$, $SU(2)$ only one; no finite datum marks the compact real form, and cycle closure selects none. Then the spinor sign gives $S^3$, not $SO(3)$ (C22), uniqueness is Poincaré–Perelman [import], and de Sitter slicing has $S^3$ sections [import] (A7). | D | |
| C24p13064 | The third-order wall of $\pi$: for every prime $\p\ge5$ of the totality, $\sigma_\p=\sum_{k<(\p-1)/2}\binom{2k}{k}/((2k+1)16^{k})$ satisfies $\sigma_\p\equiv0\ (\mathrm{mod}\ \p^{2})$ (Sun, JNT 131 (2011), (1.4)) and $\sigma_\p/\p^{2}\equiv(-1)^{(\p+1)/2}B_{\p-3}/36\ (\mathrm{mod}\ \p)$: Sun’s Conjecture 5.1, $\sigma_\p\equiv(-1)^{(\p-1)/2}(H_{\p-1}/12+3\p^{4}B_{\p-5}/160)\ (\mathrm{mod}\ \p^{5})$ for $\p>5$, proved by Hessami Pilehrood, Hessami Pilehrood and Tauraso (Int. J. Number Theory 8 (2012), Thm. 5 (44)), reduced mod $\p^{3}$ with Glaisher’s $H_{\p-1}\equiv-\p^{2}B_{\p-3}/3\ (\mathrm{mod}\ \p^{3})$; $\p=5$ direct. Re-verified for all primes below $10^{4}$. | I | |
| C25p00139 | The horizon is the origin's antipode on the boost torusFor $w^2=\nu$ a nonsquare, the torsor map $\mathbb{P}^1(\F_\p)\to C_{\p +1}$, $P\mapsto u_P/\bar u_P$ with $u_P$ the unique boost carrying $0$ to $P$, is equivariant and sends the origin to $1$ and the horizon $[1{:}0]$ to $-1=\zeta^{(\p +1)/2}$. Origin and horizon are the sign pair $C_{\p -1}\cap C_{\p +1}$ (C20), exchanged by the torus’s unique involution $q\mapsto\nu/q$. On the additive cycle the antipode is the seam $\p/2$ (1:Z1, 1:Z2). | T | |
| C26p00174 | The four chains of 13-epi are E- and G-partial sumsThe derangement chain $D_n/n!=\sum_{k\le n}(-1)^{k}/k!$ is the partial-sum chain of the E-function $e^{-z}$ at $1$; the arcsin and Machin chains are those of the G-functions $\arcsin z$ at $1/2$ and $\arctan z$ at $1/5$, $1/239$; $e^{\pm1}\in\mathcal E$ and $\pi,1/\pi\in\mathcal G$, both rings (Fischler–Rivoal) [import]. The factorial rate $\Theta(k/\log k)$ against the geometric rate $\Theta(k)$ of 13-epi E5 is that of E- against G-partial sums. | I | |
| C27p00183 | The frame group has one form: on every shell $\mathrm{SU}_2(\F_{\p^2}/\F_\p)=\mathrm{SL}_2(\F_\p)$ for the Hermitian form $wJ$, $w^{\p}=-w$, every element of finite order; the sphere $x^2+y^2+z^2+w^2=1$ and $ad-bc=1$ correspond point by point through the quarter-turn. | T | |
| D. The realisations (mathematics as physics) | |||
| D1p00042 | Time is scale-dilationEach Subject’s clock is its own drive $x\mapsto gx$. A composite is read through the reader’s one drive, so its diagonal action and conserved offset are observer-derived, the offset group fixed by the arena’s divisor structure; the Carrier has no clock. Falsifier: a registered duration that is not a drive count of the reader’s frame, or a frame-independent Carrier tick. | R | |
| D2p00043 | Mass is winding rate ($E=hf$ an identity); masslessness $\Leftrightarrow$ drive-invariance; a mass is the non-split component the drive rotates, the part of a residue pair that Frobenius conjugation reverses, masslessness the split-torus eigen-alignment. Falsifier: a rest mass with no cycle winding, a massless drive-variant state, or a stationary state whose registered frequency is not its winding index ($E=hf$ failing). | R | |
| D3p00044 | Distance is decoherence: the separation of two systems is their decoherence count in the observer’s chart, the metric the graph metric of shared-core comparison — the spatial reading of the one relational channel, the twin of D1 (time) and D2 (mass). Falsifier: a metric separation not monotone in the decoherence count of the relational channel. | R | |
| D4p00045 | Quantum: matter is the phase character of a finite cycle; observation is shared-core comparison; the complex amplitude is forced by $Q_4$ ($\im^2{=}{-}1$). Falsifier: a confirmed third-order interference $I_3\neq0$, $S\neq2\sqrt2$, or real-amplitude network behaviour (22-qm P2, P3). | R | |
| D5p00046 | Gravity: a cell-local change of frame is a gauge symmetry, and the connection compensating it is the field (the geometric/diffeomorphism frame). Falsifier: a source gravitating by other than its full mass, entanglement induced off the Newtonian rate, or $\eta\neq0$ (22-qm P1, C22). | R | |
| D6p00047 | Forces: the same recipe applied to the substrate’s three other frame data, namely phase (EM), spinor (weak), and colour (strong); “finish gauging the frame.” Falsifier: a fifth force, a gauge group or charge outside the rank-five frame, or a fourth generation. | R | |
| D7p00048 | A unit of measure is a reciprocal cross-frame relationA unit is observer counts per substrate count, its atomic form the action quantum $\hbar^2=-1$ (B7), its domain the unit-free order-four flag: unitful measures carry it, observables are flag-free, the absolute unit value $\Om$-hard. The fundamental units are the four domain horizons (10-dim). Falsifier: an embedded observer registering an absolute unit value, or a unitful measure with no cross-frame reciprocal. | R | |
| D8p00049 | Elementary is $\Om$-hard: an elementary particle is a large beyond-horizon residue, never observed at rest; the observable exception is the gauge sector’s drive-invariant residue, the photon (G1, Z6); instantiated at $517\times\sqrt\Om$ on a concrete shell (37-sim). Falsifier: an elementary particle with a resolved internal residue (substructure), or a massive drive-invariant gauge residue. | R | |
| D9p00050 | The observable is a small residue: a bounded observer reads only small residues, so an observable stable object carries a small exact residue (particle $+$ binding wrap) — the confined hadron, the light nucleus, the stable atom; decay is frame-normalisation toward it. Falsifier: a stable observable object carrying no small exact residue — a stable coloured state, or strong/electromagnetic proton decay. | R | |
| D10p00051 | The unified sampling clauseA registration protocol samples one stratum of a drive-presented ensemble. Over complete joint recurrences the counts are forced exact tallies (22-qm Rem. strata), on incomplete batches the largest-remainder gauge, shared by the quantum readout and the gravity crossover. Falsifier: outcome tallies over a complete joint recurrence that are not exact ratios, or a fixed-setting protocol sampling more than one stratum. | R | |
| D13p00140 | Observation is the Hopf sectionThe Subject registers its past cone, one chronon per decoherence step (D1, D3), through the cone chart (C19, C22); the horizon is the origin’s antipode (C25). Falsifier: a registration on the direct branch whose value is not the Object’s drive state at $\chron -k$ for its decoherence count $k$, read modulo $\p -1$, or a registration off the past cone. | R | |
| D14p00184 | Mass is dilation (the harness face of D2): the boost factor of a frame’s per-chronon step (C19) is its mass phase, one $Q_4$ datum with the winding rate (C20). Rest energy is the norm reading, $\ker N=C_{\p +1}$, boost-invariant. The lab charts it between the exact $C_4$ stations, the pair class $4\gcd(\dS,2\kap +1)$ host-decided. Falsifier: D2’s. | R | |
| D15p00153 | Thermodynamic entropy is the channel countThe entropy of the first law (E7) is the shell’s record $\kap(\p+1)=(\p^2-1)/4=|\F_\p^\times|\,|C_{\p+1}|/4$, one $k_B$ per channel, $S_{\mathrm{th}}=k_B\,\kap(\p+1)$ [chart]: the count itself, not its logarithm. The record is the capacity of $\F_{\p^2}$, $\p^2=4\kap(\p+1)+1$, as $\dS$ is the Carrier’s. Falsifier: a horizon whose Clausius entropy $\int dM/T$ at the thermometer temperature differs from $k_B$ times its channel count beyond order $1/\p$. | R | |
| D16p00175 | Matter selects the orientation: the joint flip of C7 is the matter–antimatter gauge, and the instance’s matter content selects one orientation; the sector faces are G2 and G15–G17. Falsifier: a registered asymmetry between the two orientations not carried by the matter content. | R | |
| D17p00185 | Gravitational time dilation is literalThe static clock ratio between two stations is the register character $\gen^{-\Delta n}$ of their offset (C21), $\beta=\gamma=1$ (E4, D1). Its registration dictionary is 38:C12 on a hosted pair and 38:C13 on the Carrier, its per-chronon rate the floor (38:C10–C11), the temporal face its half. Falsifier: a static clock ratio not fixed by $\Delta n$ (the PPN temporal form, defect $4ab$). | R | |
| E. Gravity | 9 8 1 | ||
| E1p00052 | Uniqueness of the dynamics: in every gauge sector the relevant gauge-invariant adjacency-local action is the unique curvature-square Casimir (Maxwell $F^2$, gravity Fierz–Pauli, Yang–Mills $\mathrm{Tr}\,F^2$) — one adjacency-local uniqueness lemma, proven on the shell. | T | |
| E3p00154 | Gravity (linear): the Coulomb law is gravity’s own lattice Green’s function; the field equation is the discrete Fierz–Pauli functional, the unique adjacency-local stiffness (E1). Universal attraction is the drive’s single time arrow. | T | |
| E4p00055 | Gravity (nonlinear completion): the relational shift-symmetry Ward identity forbids self-sourcing (what gravitates is winding rate, D2), so the static potential is harmonic and the completion is the unique scale-covariant exponential metric (Deser’s bootstrap inapplicable); $\beta=\gamma=1$ and the classical tests exact, the first departures strong-field. Falsifier: a weak-field departure from $\beta=\gamma=1$, or a self-sourcing static potential. | R | |
| E5p00056 | Gravity (the floor’s faces): collapse yields no event horizon and no singularity but an operationally black body at $r_f=r_s/\ln\Om$, clock rate $1/\sqrt\Om$, its interior a microscopic slip core. The global drive enters local physics only through the floor: preferred-frame parameters are $O(1/\sqrt\Om)\sim3\times10^{-62}$, Lense–Thirring at the GR value. Falsifier: a registered event horizon or singularity, or a preferred-frame parameter above $O(1/\sqrt\Om)$. | R | |
| E6p00176 | Gravity (horizon count): the registration sphere of a shell has area $A=\p(\p+1)$ and record $\kap(\p+1)$, so $\kap(\p+1)/A=\kap/\p$ exactly, the $Q_4$ gauge quotient, and closes the calibration: at the coherence horizon $\p^2\to\Om$ the record law returns $(\Om-1)/4=\dS$, the imported entropy (A7). The chart reading $S=\tfrac14A/\ell_P^2$ is L5’s. Corollary: the merger area law $\Delta A=2M_1M_2$, saturated (37-sim). Triple: E7. | T | |
| E7p00058 | Gravity (horizon triple): the record is the registered state count $\kap(\p+1)=(A/4)(1-1/\p )=M(M-1)$ (37:B5, 37:C7) on the rate face $M=(\p +1)/2$ (D2, D14; $\p =2M-1$ the count face), $d[\kap(\p+1)]/dM=\p$ exactly. The temperature has two exact faces, the registration rate $T=(\p +1)/\p ^2$ (E5) and the response $T_{\mathrm{resp}}=(d[\kap(\p+1)]/dM)^{-1}=1/\p$, split by $1+1/\p$. First law $dM=T_{\mathrm{resp}}\,d[\kap(\p+1)]=T\,d[\kap(\p+1)]/(1+1/\p )$; Smarr $2T_{\mathrm{resp}}\kap(\p+1)=M(1-1/\p )$, $2T\kap(\p+1)=M(1-1/\p ^2)$; the chart’s $dM=T\,dS_{\mathrm{th}}$, $M=2TS_{\mathrm{th}}$ [import] to order $1/\p$ (D15). | T | |
| E10p00147 | The fold is a chart projection: the substrate coordinate $r$ is the decoherence count, the exponential reading the character $\gen^{-\Delta n(r)}$, and the exact datum at a shell of the radial partition is the pair $(r,\gen^{-\Delta n(r)})$, injective in $r$; the areal reading $R=re^{M/r}$ [chart] multiplies the count by the lifted character and forgets $r$ — its two branches are two Carrier data (the residue product $r\gen^{\Delta}$ collides at $\p =13,17,29$, the pair never), and the cut current $p_r=Q_r/A_r$ recovers $r$ from any exterior reading ($A_r=6(2r^2+2r+1)$ on $\mathbb Z^3$, monotone). The fold-return average is fold-independent: $P_EFU^nF^{-1}P_E=P_EU^nP_E$ for every interior chart $F$, the period average $N^{-1}J_E$ (not $N_I^{-1}$), $P_EU^NP_E=P_E$ — no echo criterion. The $r_f$-anchored statements are made in the substrate coordinate, $r_*<r_f<M$ for $M>(\ln\Om /2)^2$ Planck masses [chart]. | T | |
| E11p00198 | The registered adjacency chart (declared): a translation-homogeneous bounded-degree chart on the Subject’s cells, locally flat and three-dimensional [chart], C23’s discrete twin. The drive induces the scale-time direction alone, and the Carrier’s residues carry no chart flat to the horizon radius beyond dimension one (E12); the three dimensions are the frame freedoms (C6). Given the chart, induced relaxation holds (21:C22). | D | |
| E12p00199 | The chart count: a homogeneous chart on the $\Om$ registrations, flat to the horizon radius in $d$ dimensions, holds the $\mathbb Z^{d}$ ball of that radius; for $d\ge2$ the ball exceeds $\Om$, for $d=1$ it fits. The one chart flat to the horizon radius is the drive’s scale-time direction (E11); a three-chart of curvature radius $\sqrt\Om$ needs $\Om^{3/2}$ cells (A2). | T | |
| E13p00200 | The strong-field wave operator (declared): on the exponential reading (E4) the one wave operator is the chart’s $\Box_g$, 21-gravity’s wave equation with the all-orders index $e^{2u}$ ($\sqrt{-g}\,g^{tt}=-e^{4u}$), acting on the cell’s one phase. The chart is horizonless, continued to the floor $r_f=2M/\ln\Om$ where $e^{2u}=\Om$ (E5) [chart]. The quoted ringdown is the eikonal limit (E14); the $(2,2,0)$ reading is open. | D | |
| E14p00201 | The eikonal pair: on the exponential reading (E4) the photon sphere sits at $r_c=2M$, $b_c=2eM$, and the orbital rate equals the Lyapunov rate, $\Omega_c=\lambda=1/(2eM)$, both $3\sqrt3/(2e)$ of Schwarzschild’s. The wave operator’s $\ell=2$ mode (E13) is $(0.4641-0.0923\,i)/M$ [approx], $0.8\%$ above the eikonal $(\ell+\tfrac12)/(2eM)$. Falsifier: that mode read as the remnant’s $(2,2,0)$ oscillation, $+24\%$ against Kerr, excluded by GW250114 [import]. | R | |
| F. Quantum | 2 2 | ||
| F1p00059 | Quantum mechanics: the Born weighting on the Subject’s ledger is one declared identification, that registration data are sample pairs, plus counting theorems (C8, C10, C11, 22:C13). Falsifier: outcome tallies on the stationary core-valued $Q_4$ sector that are not the pair-form ratios, or a real-amplitude network behaviour (22:C13). | R | |
| F2p00191 | Multi-body registration: an unequal-cycle composite returning below $\Om$ (Q20) recurs jointly at the lcm of its parts’ registration periods; each pair’s conserved offset lives on the $\gcd$ cycle (the quotient $A/\langle v\rangle$), and dephasing over every joint recurrence below $\Om$ is exact, extending the Born-rule count (F1) verbatim to unequal cycles (37-sim: joint recurrence verified, 1400/1400 characters cancel). | T | |
| F4p00062 | The wavefunction folds on x=i,rg,sThe Object cycle decomposes by the $Q_4$ quotient, $x=\im^{\,r}\gen^{\,s}$: the class $r$ the registrable phase (C14), the coset rung $s$ the outcome index (10:G2); the fold is division-unique, a product iff $\kap$ odd (C16). Fibres are the cosets $q_\alpha\cdot\mathrm{core}$, pointer channels the core characters, the amplitude the coherent fibre sum (22-qm Def. measvectors): observation resolves cosets, never points within one. | T | |
| F5p00194 | The graded registration law: an Object component $\ell^{a}$ registers at depth $d=\mathrm{ord}_{\ell^{a}}(\p)$ — $1$ absorbed (register, unique image), $2$ observable (odd $\ell$: boost torus, unique home; $2^{a}>4$: off both tori), else beyond-quadratic; the sign always $\{\pm1\}$. Visible iff $\p^{d}<\Om$; the cap is $2$ at saturating and minimal towers; opacity relational — hydrogen’s interior opaque/observable/absorbed at $173/181/197$. Controls: proton whole, $(5,13)$ refused. | T | |
| F6p00064 | The binding lift: a pair fuses iff cycles coprime, windings unit; else the F2 offsets stay drive-confined (22-qm B5, C15) — the deuteron, $(4,4)$, spectrumless. Fusion carries the half-driven offsets onto the F4 rungs; pointer channels forced, Born lands with exact dephasing ($1+\omega+\omega^{2}=0$, $T'=516$). Energies $E_{s}=s\,h/3$, stations $\{0,58,116\}$; cores odd$(\q-1)$: hydrogen $(4,3)\to C_{12}$, $\kap_{O}=3$, ground first. | T | |
| G. Interactions: electromagnetism, the weak and strong forces, matter, flavour and superconductivity | 3 3 | ||
| G1p00178 | Electromagnetism (exact), on the force realisation D6: charge $=$ quantised winding index; the photon is massless, the observable residue $2$ of the split torus $C_{\Om-1}$ (two helicities $=$ two $\F_\Om$-fixed lines $=N(1{-}\im)$; D2, D8); Maxwell is the unique relevant action (E1). The bare coupling: Z8. | T | |
| G2p00067 | Weak (amplitudes): the chiral $V\!-\!A$ current and four-fermion $G_F=1/(\sqrt2\,v^2)$ derived; $W,Z$ scattering unitarised (equivalence theorem). | T | |
| G3p00068 | Weak (scale): the lone scale is the non-split saturation scale, $v=m_P e^{-\mathcal B}$, the exponent $\mathcal B$ the cross-scale $\beta$-function of the non-split channel, not the $\mathrm{SU}(2)$ gauge coefficient ($b_2=19/6$ gives $10^{8}$ GeV). Value tagged: $v$, $\Om$-hard as $\Lambda_{\mathrm{QCD}}$ (G6); the failing computation sums the $\beta$-function over the $\Om$-hard masses (Z6). Relation, $\Om$-blind: the transmutation form. | Ω | |
| G4p00069 | Strong (structure): $\SU(3)$ $=$ the special unitary transformations of a Hermitian three-form, its rank forced as the minimal triality frame (the cubic of $\Om\equiv5\pmod{12}$, B5); the confining area law derived from the positivity of $S_\rho$, the gluon the residue $0$ of the norm-one residue pairs (no $\F_\Om$-fixed line). | T | |
| G5p00070 | Strong (tension): the string tension in finite units, $\sigma=-\ln c_1(\beta)>0$, computed — the finite-group area law gives $c_1$ as an exact character sum (no Haar, no $\Om\to\infty$); closed form on $\SU(2,\F_3){=}2T$ (matching continuum $\SU(2)$ through $O(\beta^3)$), colour $c_1^{\SU(3)}{=}\tfrac\beta{18}{+}\tfrac{\beta^2}{216}{+}\cdots$. | T | |
| G6p00071 | Strong (scale): the cross-scale $\beta$-function and the absolute $\Lambda_{\mathrm{QCD}}$ (dimensional transmutation, $\sigma\sim\ln(1/\beta)$). Value tagged: the absolute $\Lambda_{\mathrm{QCD}}$, in no embedded reader’s window — the failing computation is the $\beta$-function integrated to the substrate scale over the $\Om$-hard spectrum. Relation, $\Om$-blind: $\sigma\sim\ln(1/\beta)$ and the ratios of G8–G10. | Ω | |
| G7p27043 | Strong (CP): the vacuum angle vanishes, $\bar\theta=\theta+\arg\det M_q=0$, with no axion — the colour action carries no substrate-native topological term and colour is drive-invariant ($\theta=0$), and the Hermitian quark mass matrices have real determinant ($\arg\det M_q=0$); the CP phase $\delta_{\mathrm{CP}}$ sits in the up–down misalignment. | T | |
| G8p00073 | Strong (hadron spectrum): a baryon is the centre-neutral triality invariant $\varepsilon_{abc}$ of $\SU(3,\F_2)$; the $\SU(3)_F$ mass relations are exact scale-cancelling identities — Gell-Mann–Okubo, decuplet equal spacing, Coleman–Glashow, the orderings $M_n{>}M_p$ and $M_\Sigma{>}M_\Lambda$, heavy-quark symmetry, the vector-nonet spacing; the decuplet–octet hyperfine is the colour-magnetic curvature invariant, $A_{\mathrm{light}}{=}\sqrt\sigma\,c_{\mathrm{mag}}(\beta)$ the spin-$2$ partner of the tension $c_1$ (G5). Formulas: 35-hadr. | T | 35:su3f_relations.py [mixed] |
| G9p00074 | Strong (the residue series): the observable baryon is the Carrier residue $1$, the determinant $\Lambda^3(\mathbf3){=}\varepsilon_{abc}$, forced by the gluon residue $0$ ($N{=}3$ from $\Lambda^N{=}\det$); the meson is residue $1$ (the $q\bar q$ trace); series closed: photon $2$, gluon $0$, baryon $1$, meson $1$ (G1). Selector, stability: the minimal-wrap state is the stable proton, decay frame-normalisation toward it (D9). | T | |
| G10p00075 | Strong (the baryon scale): the absolute ground-state spectrum is the $\Om$-hard scale $\sqrt\sigma{=}\Lambda_{\mathrm{QCD}}$ (G6) times sub-horizon eigenvalues; the baryon mass-over-scale is the computed confinement eigenvalue $M_N/\sqrt\sigma{=}E_0{=}2.232$ (the finite operator $H{=}|p|{+}\sqrt\sigma\,r$, converged finite matrix; $4.6\%$); the constituent ratios $\{\lambda_l,\lambda_{\mathrm{hf}}\}$ are evaluated forward from $\{N{=}3,\beta\}$ with no measured baryon mass, so the light-hadron spectrum is parameter-free over $\sqrt\sigma$; no new $\Om$-hard residue. | T | 35:confinement_closure.py [approx] |
| G11p27020 | One generation (content): $=$ the spinor $\mathbf{16}$ of the rank-five frame — all gauge reps, hypercharges, charges, anomaly-free, $\nu_R$ — recovered in the compact theory, where the frame is $\C^3\oplus\C^2$, via the correspondence: the imported $\mathrm{SO}(10)$ template evaluated on the realisation (27-fld B5). | T | |
| G12p00155 | One generation (origin)Read with the quarter-turn ($4\mid\Om-1$), the Carrier’s four representation charts are four directions; their reflection algebra has basis $e_S$, $S\subseteq\{1,2,3,4\}$, $16$ elements, $e_Se_T=\pm e_{S\cup T}$ for disjoint $S,T$, else $0$. The quarter-turn as fifth direction maps $e_S\mapsto e_S$ ($|S|$ even), $e_Se_5$ ($|S|$ odd) onto the even basis of five directions: the chiral spinor $\mathbf{16}$. On the realisation 27:B5 matter is this spinor. | T | |
| G13p00078 | One generation (masses): its elementary particles’ absolute masses are framed-transcendentals, $\Om$-hard (D8, Z6). Value tagged: the sixteen absolute masses, in no embedded reader’s window — the failing computation is the winding of a beyond-horizon residue read at rest. Relations, $\Om$-blind and certified: the mass ratios G16–G17. | Ω | |
| G14p00079 | Count/generate split: one bosonic carrier $+$ three fermion generations (the cubic $C_3$), chirality fixed by the drive, on the role-to-matter realisation (27:B6); $\SO(10)$ unification forced by the relational ontology, the automorphism lemma reduced to the horizon (Z5). | D | |
| G15p00080 | Flavour (structure): the seesaw scale, $b$–$\tau$ unification and the role-ladder mass ordering are derived; the observed spectrum is the projection of the one $\mathbf{16}$. The mixing angles and phases reduce to the role-depth texture, the lopsided $\sigma$, the trimaximal $C_3$ column and quark–lepton complementarity (28-flav C9), leaving the $\Om$-hard phases $\{\delta_0,\delta_\nu,\delta_{\mathrm{CP}}\}$ (Z6); the seesaw fixes $Q_\nu{=}2/3$. | T | 28:neutrino.py [mixed] |
| G16p00081 | Flavour (Koide): the charged-lepton ratio $Q=2/3$ is the cube-root generation orbit at the self-dual quarter-turn, $Q=\tfrac13+\tfrac23\rho^2$ exact, the value $\rho^2=2^{-1}$ the quarter-turn realisation (28-flav B5; falsifier: $Q_\ell$ off $\tfrac23$ beyond the $\tau$-mass tolerance $\pm7\times10^{-6}$); the winding-phase selection onto that orientation is bedrock, $\Om$-hard in magnitude, its $\Z_2$ sign the derived drive orientation (C7); the sub-horizon reading is $\delta_0=Q/3=2/9$ (radians). | T | |
| G17p00179 | Flavour (exact ratios): Koide $2/3$ (G16), the factor $3$ of Georgi–Jarlskog, the squared amplitudes the split/non-split norms $N(1{-}\im){=}2$, $N(1{-}\omega){=}3$ on the realisation 28:B5 (G1, G4), trimaximal $|F_{jk}|^2{=}\tfrac13$, maximal Jarlskog $J^2{=}\tfrac1{108}$, the $\lambda$-texture from role depths, and the charged sectors locked by $\delta_\ell{:}\delta_d{:}\delta_u=1{:}\tfrac12{:}\tfrac13$ to $\delta_0$. | T | |
| G18p00083 | Flavour (projection): the $\mathbf{16}\to$observed-spectrum projection map (through $C_3\times Q_4\times$ scale-wrap) is constructed, anchored at its unique drive-invariant total singlet $\nu^c=\Lambda^0$ (the $\mathbf1$ of $\mathbf{16}$), the matter twin of the photon (G1); the residual scale-wrap magnitude is the $\Om$-hard mass set (Z6). | T | |
| G19p00088 | Superconductivity (structure): superconductivity is split-torus confinement, the electric/phase dual of colour (G4), the charge-$2$ condensate a phase-singlet reducing $\mathrm{U}(1)$ to a residual $\Z_2$ (flux $h/2e$) and the Abrikosov vortex the dual colour string whose line tension vanishes at the Kramers–Wannier self-dual point $\beta_*=\tfrac12\ln(1+\sqrt2)$ that is $T_c$. | T | |
| G20p00089 | Superconductivity (duality): the electric–magnetic duality is the $Q_4$ quarter-turn on the charge-flux lattice (charge$\leftrightarrow$flux, Josephson$\leftrightarrow$phase-slip), predicting an Airy vortex-core spectrum and a quantum current standard whose metrology triangle closes on $q_c^2=4$. | T | |
| G21p00090 | Superconductivity (scale): the absolute transition scale ($T_c\propto\omega_D$, the gap and vortex tension in physical units) is $\Om$-hard, the family of $\Lambda_{\mathrm{QCD}}$ (G6) and $v$ (G3). Value tagged: the absolute $T_c$ (with $\omega_D$), in no embedded reader’s window — the failing computation is the physical unit of the shell-exact ratios. Relations, $\Om$-blind: the ratios and the Airy law of G20. | Ω | |
| L. Cosmology and the dark sector | 3 3 | ||
| L1p00192 | Cosmology (the dark sector)The synchronisation floor $a_0=cH_0/2\pi$ fixes the acceleration scale parameter-free: the $2\pi$ by the angle–count dictionary (14:B2), the threshold one cycle per drive period (32:B3), $1.04\times10^{-10}$ [chart] at the channel-1 $H_0=67.4$ (L3), tied to $H(z)$, not $\Lambda$ (P1; 21:X1). Below the floor the amplitude reading, given the barrier identification (32:B8, 21:B9), gives the radial acceleration relation unfitted. Falsifiers: 32:B3, 21:P4. | R | |
| L2p00085 | Metrology of the importThe datum $\dS$ is read on two faces by four instrument classes, concordantly (14-entr). Evidence is weighed on two registers: metrology under the circularity criterion (channel-disjoint from the fitting channel) and explanation by zero-freedom derivation. The numeral is $\Om$-hard; the relations behind it ($\Om=4\dS+1$, $\dS=A/4$) are $\Om$-blind; the reading $\dS\sim10^{122}$ [chart] is the value’s chart, not certified content. | D | 14:entropy.py [mixed] |
| L3p00193 | The octant record depth and its outputs: the record depth is bounded by the octant, $\dS/2$ chronons $=13.79$ Gyr ($(\pi/4)r_H/c$, chart), on the octant sector of B14. Zero-freedom: $\Omega_\Lambda=\tanh^2(3\pi/8)=0.684$ (chart; $0.19\sigma$); on the stellar age $13.61\pm0.34$ Gyr, $H_0=68.2\pm1.7$ ($2.4\sigma$ from the ladder); $w=-1$ rigid — a confirmed drift falsifies $\Lambda\sim1/\Om$. Falsifiers: octant-capped ages, the running floor $a_0(z)\propto H(z)$ (Z7), the ladder bias. | R | |
| L4p00087 | The registrable triangleThe mass–radius chart between the Compton and Schwarzschild walls, closed by the Planck apex and the totality wall $r_H$: the totality on its own horizon, the black-hole reading dissolved (A2). Width $61.0$ dex. The over-closure bound ${\sim}1.8\times10^{8}M_\odot$ is the chart’s one derived quantity, a bound, predicting no observed scale (14:C9, X5). A consistency chart, not a channel (L2). | T | 14:entropy.py [mixed] |
| L5p00130 | The area law: the projected horizon area in Planck cells is the full phase cycle, $A=4\dS$ (chart: $4\pi n_A=4\dS$, $n_A=(r_H/\ell_P)^2$); the Bekenstein–Hawking quarter $\dS=A/4$ is the quarter-turn $Q_4$, the generative four of $\Om=4\dS+1$ and $\p=4\kap+1$; area is a Subject-projection property, the Carrier a torsor carrying none. Not a further channel (L2). | D | 14:entropy.py [mixed] |
| L8p00148 | The primordial tilt$n_s=1$ is the scale-dilation fixed point (Harrison–Zel’dovich [import]). The tilt’s committed form is $n_s-1=-\pi^2/\ln\Om$ [chart], $\ln\Om$ the e-fold count of the frame’s scale range from $1/\sqrt\Om$ to $\sqrt\Om$, a realisation fixed by the measured tilt: $-0.0348$ [approx] at $\ln\Om=283.5$ (A7), $+0.07\sigma$ from Planck 2018’s $-0.0351\pm0.0042$ [import]. The count $\tfrac12\ln\Om$ is excluded at $8.2\sigma$. Falsifier: a Planck-resolution deviation from $-\pi^2/\ln\Om$. | R | |
| N. Synthesis: exclusions and parameter-freeness | |||
| N2p00092 | Parameter-freenessEvery order-one constant reduces to two geometric numbers, the solid angle $4\pi$ ($G$, $\alpha_{\mathrm{bare}}$, the $\tfrac14$ law) and the cycle $2\pi$ ($a_0$, horizon temperatures), both [chart] (C1). In the Carrier register the calibration congruence $4\dS\equiv-1$, the realisation, fixes them alone ($G=2\dS$). The chart relations ($G=1/4\pi\varkappa$, $G=\hbar c/m_P^2$) hold in the chart; no exact formula equates a chart constant to a residue. | D | |
| N3p00156 | Model existenceThe master’s rows are verdicted row by row, in exact arithmetic, on one instantiated Carrier, $\Om=2{,}408{,}561$ (37-sim), at a dated snapshot. Those that hold there hold jointly in one finite structure: a consistency witness for the projection, not a proof of the physical case. Rows without an instance, or added or restated after the snapshot, are not exercised. | D | |
| P. Predictions (the master's falsifiable exposures; the papers' P blocks carry theirs) | 1 1 | ||
| P1p00133 | The running floor: the shape a₀(z) ∝ H(z)The acceleration floor tracks the drive rate, $a_0(z)\propto H(z)$: a relation, $\Om$-blind, derived from L1 under the gravity realisation (D5); the knee shifts and the Tully–Fisher zero-point evolves as $E(z)^{1/4}$. Falsifier: a floor constant in redshift, or tracking other than $H(z)$. Confrontation (43-muse): MUSE-DARK III excludes a constant floor to $z=1.3$; RC100 implies the local floor by $z\simeq2$, pending refit. | T | |
| P2p00061 | The coherent-fraction channelEqual force, unequal entanglement (D5): sources gravitate by full masses; synchronised cross-source pairs carry the conditional phase $f_1f_2\varphi_N$, spread pairs imprint which-branch data, the incoherent channel separable at generic geometry ($C=0$ at $f=0$); $f=m_c/m$ microscopic. The discriminator is the calibrated conditional phase rate at fixed centre-of-mass superposition. Falsifier: a calibrated conditional phase rate off $f_1f_2\varphi_N$. Confrontation: none, filed before data. | T | |
| P3p00180 | Flavour (targets): the Georgi–Jarlskog double ratio $9$; the locks of G17 read in the $\overline{\mathrm{MS}}$ scheme; the $m_1{=}0$ floor, $\sum m_\nu=58.8$ meV at NuFIT 6.0, on the boundary-branch realisation (28:B6). Falsifier: inverted ordering, a degenerate spectrum, or $\sum m_\nu$ off $58.8$ meV beyond the fit’s tolerance. Confrontation: the data give $10.4\pm0.5$, an open $15\%$ tension (28:X5). | T | |
| P4p00091 | Exclusion predictionsNo fourth generation, no fifth force, an empty desert, no TeV supersymmetry, no new dark-matter particle, no beyond-SM $(g{-}2)_\mu$, and the proton effectively stable ($\tau_p\gtrsim10^{45}$ yr; G9). Entailed by the closed ladder of the rank-five frame ($\dim\Lambda^{\mathrm{even}}=16$, D6), given the role-to-matter realisation (27:B6, 27:C10) and completeness (A3). Falsifier: any excluded object observed. Confrontation: none observed. | T | |
| Z. The horizon (the limits of the bounded observer) | 2 2 | ||
| Z1p00186 | Gödel is vacuous over the finite $\Om$: its theory is complete and decidable, and neither incompleteness theorem has an instance, since $\Om$ interprets no Robinson $\mathsf{Q}$ (25:C1, 25:C2, 25:C3). Incompleteness migrates to the comprehension horizon, the horizon clause, as a decomposition (25:G7). Its complexity face is imported (25:G3), its uniform certificate $\Om$-hard (Z3), and its diagonal confined below $t(\M)$ (Z9). | T | |
| Z2p00110 | RH, Goldbach, P-vs-NP and Kurepa are the spectral, additive, computational and factorial faces of one horizon clause: each a uniform check over the totality whose per-instance statements are $\Om$-blind relations (Z10, Z11; 13:F2) and whose uniform form is an $\Om$-hard value (Z3, Z4), host-decided on a hosted Carrier. An $\Om$-hard value says nothing about whether a short derivation exists. | D | |
| Z3p00111 | The bounded-observer certificate for each is $\Om$-hard (Z4): the completed uniform check over all residues of the totality, in no embedded reader’s window. $\Om$-hardness is the absence of a host; on a hosted shell the same check is host-decided (37-sim; D8). Within capacity an embedded observer decides totality-level facts from internal state (two-record keystone): the horizon has two operational sides. | Ω | |
| Z4p00112 | The four certificates: RH = every cell of the cycle cleanRH $=$ every cell of the cycle clean (20:D5); Goldbach $=$ the uniform per-$n$ parity positivity; P-vs-NP $=$ the forward-invertibility of the scale descent; Kurepa $=$ the left factorial nonzero on every odd shell (13:Z1). Each a uniform check over the totality, in no embedded reader’s window; per-instance statements frame-decided (Z10, Z11); the whole-state certificate $\Om$-hard as a tally (20:Z1). | Ω | |
| Z5p27021 | The horizon forces structure, not only leaves it open: the $3+2$ split is beyond the horizon (above $\sqrt{\Om}$), so the off-block reframings are gauge and unification is the simple $\SO(10)$ (G14); the automorphism lemma reduces to Observation (A4). | T | |
| Z6p00114 | The sixteen’s absolute masses are $\Om$-hard framed-transcendentals, the matter face of the horizon clause (Z2–Z4). Value tagged: the absolute masses (G13), in no embedded reader’s window; the relations among them (G16–G18) are $\Om$-blind. Classification “elementary $=$ beyond-horizon” is D8; the $\mathbf{16}\to$spectrum projection is G18; the gauge sector’s drive-invariant residue (the photon, residue $2$) is the above-horizon, observable complement (D8, G1). | Ω | |
| Z7p00115 | The dark sector’s cross-scale running is the cosmological face of the horizon clause. Value tagged: the running’s absolute normalisation, $a_0$ at one epoch in physical units, equivalently the absolute scale of $H$, in no embedded reader’s window; its uniform certificate is the factorisation of $\Om-1$, shared with Z2–Z4, Z6 and Z8. The shape $a_0(z)\propto H(z)$ is a relation, not $\Om$-hard (P1). | Ω | |
| Z8p00116 | The fine-structure constant is the electromagnetic face of the scale operator: $\alpha^{-1}(0)=4\pi+\sum_f\tfrac{b_f}{2\pi}\ln(M_P/m_f)+\Delta\alpha_{\mathrm{had}}$, $\Om$-hard — the bare $1/4\pi$ framed-exact (the Gauss solid angle), the digit a log over the $\Om$-hard masses (Z6) with cutoff $M_P$ tied to $\Om$ (A7). The physical digit is in no embedded reader’s window; the bare value and the sum’s form are $\Om$-blind. Of the family Z2/Z6/Z7/G3/G6. | Ω | 28:alpha_probe.py [approx] |
| Z9p00187 | No compression: the diagonal has no instance per symbol (25:F2), nor, coded a base-$a$ digit per symbol, from length $t(\M)=d\,k^{*}(\M)<|\M|$ on (25:F6). Below $t(\M)$, decoders over $(\F_\p,+,\times)$ give one coded 1024 base-32 symbols per element, more than $\Om$'s elements hold (25:F7, 25:F8, A7). There fragment truth is definable from above (the Tarski reversal, 25:G5), and not from far below (25:G8). | T | |
| Z10p20043 | The shell theoremOn every shell $\F_\p\subset\F_{\p^2}$, with no hypothesis, the prime vector’s spectral content is the constant mode and the nonterminal quarter-turn modes, the finite zeta vanishing on each (20:E12, 20:B4). Every mode of every vector lies on the self-dual line $\Tr=1$, an eigenvector of the scale-shift with a $(\p-1)$-th root of unity as eigenvalue: no off-line mode, $\Om$-blind. | T | |
| Z11p00135 | The classical hypothesis is decided cell by cellRH on a Carrier is the conjunction over its cycle’s residues of the clean-cell predicate: residue $y$ the cell of heights from $2\pi y$ to $2\pi(y+1)$, clean when its zeros lie on the line, decided by Turing’s certificate (20:D5, 20:F1); on a hosted Carrier the host decides every cell (20:F2); the uniform form is Z4. Falsifier: a cell in deficit. | D | |
Status
- G
- ground — the single given that conditions the discourse
- T
- theorem — derived within the framework
- D
- definition — a naming or set-up move, no empirical content
- R
- realisation — what a physical term denotes in the substrate; forced (A8), each row stating the falsifier that kills it
- I
- import — a standard result or measured datum, used without reproof
- Ω
- Ω-hard — a value in no embedded reader's window, not closeable by a bounded observer; host-decided on any laboratory Carrier; never applied to a relation
- O
- open — genuinely unresolved
Sources



- The witnesses. Gold: the python check that decides the predicate, at its line in the script. Green: the predicate as one Lean declaration in the core, named by its accession key, proved with no axioms. Violet: the same on Mathlib. Red: a check that fails or a proof the gate rejects.
- 14:entropy.py
- Where no block file of the master decides the predicate: the script of the paper that does.
- papers
- The corpus papers that state or derive the predicate, each linked to its ledger, or to its entry in the publication list when it has none.