Determination of the high-twist contribution to the structure function \(xF^{\nu N}_3\)

• Published in: arXiv.org
• Main Authors: Alekhin, S I, Anykeyev, V B, Batusov, Y A, Borisov, A A, Bozhko, N I, Bunyatov, S A, Chernichenko, S K, Denisov, O Y, Fachrutdinov, R M, Goryachev, V N, Goryachev, S V, Kazarinov, M Y, Kirsanov, M M, Klimov, O L, Kononov, A I, Kozhin, A S, Krasnoperov, A V, Lipajev, V V, Mukhin, A I, Nefedov, Y A, Popov, B A, Prakhov, S N, Salomatin, Y I, Snyatkov, V I, Sviridov, Y M, Tereshchenko, V V, Tumakov, V L, Vovenko, A S
• Format: Paper
• Language: English
• Published: Ithaca Cornell University Library, arXiv.org 09.04.2001
• Subjects: Infrared analysis; Mathematical models; Neutrino beams; Neutrinos; Parameters
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.0104013

We extract the high-twist contribution to the neutrino-nucleon structure function \(xF_3^{(\nu+\bar{\nu})N}\) from the analysis of the data collected by the IHEP-JINR Neutrino Detector in the runs with the focused neutrino beams at the IHEP 70 GeV proton synchrotron. The analysis is performed within the infrared renormalon (IRR) model of high twists in order to extract the normalization parameter of the model. From the NLO QCD fit to our data we obtained the value of the IRR model normalization parameter \(\Lambda^2_{3}=0.69\pm0.37~({\rm exp})\pm0.16~({\rm theor})~{\rm GeV}^2\). We also obtained \(\Lambda^2_{3}=0.36\pm0.22~({\rm exp})\pm0.12~({\rm theor})~{\rm GeV}^2\) from a similar fit to the CCFR data. The average of both results is \(\Lambda^2_{3}=0.44\pm0.19~({\rm exp})~{\rm GeV}^2\).