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We construct a QCD coupling $$ \mathcal{A} $$ A (Q2) in the Effective Charge (ECH) scheme of the canonical part d(Q2) of the (inelastic) polarised Bjorken Sum Rule (BSR) $$ {\overline{\Gamma}}_1^{\textrm{p}-\textrm{n}} $$ Γ ¯ 1 p − n (Q2). In the perturbative domain, the coupling $$ \mathcal{A} $$ A (Q2) practically coincides with the perturbative coupling a(Q2) [≡ αs(Q2)/π] in the four-loop ECH renormalisation scheme. In the deep infrared (IR) regime, $$ \mathcal{A} $$ A (Q2) behaves as suggested by the Holographic Light-Front QCD up to the second derivative. Furthermore, in contrast to its perturbative counterpart a(Q2), the coupling $$ \mathcal{A} $$ A (Q2) is holomorphic in the entire complex Q2-plane with the exception of the negative semiaxis, reflecting the holomorphic properties of the BSR observable d(Q2) [or: $$ {\overline{\Gamma}}_1^{\textrm{p}-\textrm{n}} $$ Γ ¯ 1 p − n (Q2)] as dictated by the general principles of the Quantum Field Theory. It turns out that the obtained coupling, used as ECH, reproduces quite well the experimental data for $$ {\overline{\Gamma}}_1^{\textrm{p}-\textrm{n}} $$ Γ ¯ 1 p − n (Q2) in the entire Nf = 3 regime 0 < Q2 ≲ 5 GeV2.
We construct a QCD coupling $$ \mathcal{A} $$ A (Q2) in the Effective Charge (ECH) scheme of the canonical part d(Q2) of the (inelastic) polarised Bjorken Sum Rule (BSR) $$ {\overline{\Gamma}}_1^{\textrm{p}-\textrm{n}} $$ Γ ¯ 1 p − n (Q2). In the perturbative domain, the coupling $$ \mathcal{A} $$ A (Q2) practically coincides with the perturbative coupling a(Q2) [≡ αs(Q2)/π] in the four-loop ECH renormalisation scheme. In the deep infrared (IR) regime, $$ \mathcal{A} $$ A (Q2) behaves as suggested by the Holographic Light-Front QCD up to the second derivative. Furthermore, in contrast to its perturbative counterpart a(Q2), the coupling $$ \mathcal{A} $$ A (Q2) is holomorphic in the entire complex Q2-plane with the exception of the negative semiaxis, reflecting the holomorphic properties of the BSR observable d(Q2) [or: $$ {\overline{\Gamma}}_1^{\textrm{p}-\textrm{n}} $$ Γ ¯ 1 p − n (Q2)] as dictated by the general principles of the Quantum Field Theory. It turns out that the obtained coupling, used as ECH, reproduces quite well the experimental data for $$ {\overline{\Gamma}}_1^{\textrm{p}-\textrm{n}} $$ Γ ¯ 1 p − n (Q2) in the entire Nf = 3 regime 0 < Q2 ≲ 5 GeV2.
No abstract
We consider heavy quark contributions to the polarized Bjorken sum rule. We found good agreement between the experimental data and the predictions of analytic QCD. To satisfy the limit of photoproduction, we use new representation of the perturbative part of the polarized Bjorken sum rule, recently proposed.
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