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What does the CCFR measurement of the Gross--Llewelyn Smith sum rule tell us?

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arxiv hep-ph/9410292 v2 pith:3N5O3G6L submitted 1994-10-14 hep-ph

What does the CCFR measurement of the Gross--Llewelyn Smith sum rule tell us?

classification hep-ph
keywords ruleccfrmeasurementsmithanalyzedbarebbarecollaboration
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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abstract

Recently the CCFR Collaboration reported the measurement of the Gross--Llewellyn Smith sum rule %at $Q^2=3\; \mr{GeV}^2$: $\int^{1}_{0}\mr{d}F_{3}^{\nu p+\bare{\nu}p}(x,Q^2=3\;\mr{GeV}^2)= 2.50\pm 0.018(\mr{stat})$. Subsequently Kataev and Sidorov analyzed the $Q^2$--dependence of this sum rule and pointed out a discrepancy between the results obtained via integration of the NLO fits to $xF_{3}(x,Q^2)$ and the purely perturbative prediction. We suggest an explanation of this disagreement and show that the result of the CCFR measurement of the GLS sum rule integral can be determined from the knowledge of the value of $\Lambda_{\bbare{MS}}$ only.

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