Artian Small-x Proton Beam Access Framework: A Higgs and Dijet Blind-Audit Execution of the QTT Universal Gluon-Luminosity Rail

A blind small-x gluon rail for Higgs and dijet rows Concept DOI: 10.5281/zenodo.20938370 Author: Ali Attar Website: quantumtraction.org Main book anchor: Quantum Traction Theory: Main Book v10.01 This paper turns the small-\(x\) proton-beam rail into a blind-audit framework for Higgs and dijet gluon-luminosity rows. The source rail is frozen before empirical PDF tables, measured Higgs rates, dijet rates, or \(K\)-factors can enter. The proton-gluon source rail is \[ g_p^{\mathrm{QTT}}(x,\mu_A) =\frac{16/31}{B(2-\lambda_A,7)}x^{-\lambda_A}(1-x)^6, \] with the running exponent \[ \lambda_A =1-\frac2\rho\frac{C_A}{24\pi} \int_{\ln k_B^t}^{\ln\mu_X}\alpha_s^{\mathrm{QTT}}(\mu')\,d\ln\mu', \qquad \rho=2\pi\cos(\pi/8),\quad C_A=3. \] The finite-binomial luminosity row is \[ \mathcal L_{gg}^{\mathrm{QTT}}(\tau,\lambda_A) =A_g^2\tau^{1-\lambda_A} \sum_{i=0}^{6}\sum_{j=0}^{6}(-1)^{i+j}{6\choose i}{6\choose j}\tau^jI_{ij}(\tau). \] Core labels: Σ-SMALL-X-PROTON-BEAM-ACCESS, Σ-GLUON-LUMINOSITY-RAIL, Σ-HIGGS-DIJET-BLIND-AUDIT.