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The part of the proton spin carried by quarks is calculated in the framework of the QCD sum rules in the external fields. The operators up to dimension 9 are accounted. An important contribution comes from the operator of dimension 3, which in the limit of massless quarks is equal to the derivative of QCD topological susceptibility . The comparison with the experimental data on gives $\chi^{\prime}(0)= (2.3 \pm 0.6) \times 10^{-3} ~ GeV^2\Sigma\chi^{\prime}(0)\Sigma \ga 0.05,~~ \chi^{\prime} (0) \ga 1.6 \times 10^{-3} ~ GeV^2g_A = 1.37 \pm 0.10g^8_A = 0.65 \pm 0.15$ are also determined.

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