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Shadow Theory

Appendix A

Notation and Conventions

From A Source-to-Readout Architecture for a Theory of Everything, Version 1.0 (July 2026) · doi:10.5281/zenodo.21366204

This appendix collects only notation used across more than one chapter. Sector-specific symbols are defined where they first occur.

SymbolMeaning
S0\mathsf S_0, Sadm\mathsf S_{\rm adm}raw and admitted source categories
W0\mathcal W_0, Lsrc\mathbb L_{\rm src}witness class and source-closure operator
XX, YRealPrepΩ[X]Y\in\operatorname{RealPrep}_{\Omega}[X]an admitted source and a supported realization
Ω\Omegafixed target-neutral, source-local realization convention containing no Tier-1 target or physical-success predicate
CompT1\mathsf{Comp}_{T1}compatible Tier-1 readout object
QQ, A\mathcal A, MM, GG, CC, AA, OOquantum, QFT, matter, gravity, cosmology, arrow and observer sectors
ρ\rho, EYE_Y, IY\mathcal I_Yquantum state, POVM and instrument
Rpre,Rcand,Rsel,Ract,RobjR^{\rm pre},R^{\rm cand},R^{\rm sel},R^{\rm act},R^{\rm obj}record stages
DiobjD_i^{\rm obj}, AYobj\mathcal A_Y^{\rm obj}an objective record and the objective archive of realization YY
κinf\kappa^{\rm inf}, dreld_{\rm rel}intervention-derived influence and relational distance
dstrCd_{\rm str}^{C}, dCcmpd_C^{\rm cmp}, drefd_{\rm ref}strong metric on a Lorentzian comparison region, induced cell Hausdorff distance, and refinement path pseudometric
Recmet\operatorname{Rec}_{\rm met}set-valued metric reconstruction relation
NormY\operatorname{Norm}_Y, sYs_Ymetric-scale normalization functional and normalized section
GRG_R, Λbr\Lambda_{\rm br}, Qμνgrav\mathcal Q_{\mu\nu}^{\rm grav}renormalized Newton coupling, branch cosmological constant and pure-metric higher-curvature correction
SMdynS_M^{\rm dyn}, ΓQFT,dynren\Gamma_{\rm QFT,dyn}^{\rm ren}disjoint matter action and normalized state-dependent QFT influence functional
mR\mathfrak m_REFT matching datum fixed before the gravitational solution
ΓR,CTP\Gamma_{R,\rm CTP}, TμνR,totT_{\mu\nu}^{R,\rm tot}matched record-exclusive influence and total record contribution TμνR+χMRTμνMRT_{\mu\nu}^{R}+\chi_{MR}T_{\mu\nu}^{MR}
q=6Yq=6Y, gq=gY/6g_q=g_Y/6integer hypercharge and its compact-group coupling, with gqq=gYYg_q q=g_Y Y
gYg_Y, g2g_2, g3g_3hypercharge, weak and strong gauge couplings
KFLRW\mathcal K_{\rm FLRW}, kcomk_{\rm com}physical FLRW curvature scale and comoving perturbation wavenumber
χ\chi, ϱ=fK(χ)\varrho=f_{\mathcal K}(\chi)radial geodesic distance and areal comoving curvature radius
Φ,Ψ,Vi,hij\Phi,\Psi,V_i,h_{ij}scalar Bardeen potentials, vector shear and tensor perturbation
D\prec_D, (TY,t)(\mathcal T_Y,\preceq_t), ΘA\Theta_Astrict event-dependency order, temporal carrier and order embedding
HY,o\mathcal H_{Y,o}, OY,o(t)\mathfrak O_{Y,o}(t)common objective/arrow history and structural observer-readout family
d1Pd_{\rm 1P}, dH1Pd_H^{\rm 1P}metric on individual observer structures and its Hausdorff metric on closed output sets

Unless stated otherwise, the spacetime signature is (+++)(-+++ ), units satisfy c==1c=\hbar=1, Greek indices are spacetime indices and Latin indices are spatial or internal indices according to context. Curvature conventions are fixed by

[μ,ν]Vρ=RρσμνVσ,Rμν=Rρμρν,Gμν=Rμν12Rgμν.[\nabla_\mu,\nabla_\nu]V^\rho =R^\rho{}_{\sigma\mu\nu}V^\sigma, \qquad R_{\mu\nu}=R^\rho{}_{\mu\rho\nu}, \qquad G_{\mu\nu}=R_{\mu\nu}-\frac12Rg_{\mu\nu}.

The relation arrow \rightsquigarrow denotes a possibly partial or set-valued relation. A quotient by redescription identifies presentations of the same candidate; physical coarse-graining is a separate operation performed afterward.