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Teoreticheskaya i Matematicheskaya Fizika, 2009, Volume 160, Number 3, Pages 471–486
DOI: https://doi.org/10.4213/tmf6410
(Mi tmf6410)
 

This article is cited in 2 scientific papers (total in 2 papers)

The Jost–Lehmann–Dyson representation and target mass effects

O. P. Solovtsovaab, V. I. Lashkevichb

a Joint Institute for Nuclear Research, Dubna, Moscow Oblast, Russia
b International Center for Advanced Research, Pavel Sukhoi Gomel State Technical University, Gomel, Belarus
Full-text PDF (516 kB) Citations (2)
References:
Abstract: We develop a method for taking target mass effects into account for the structure functions of inelastic lepton–hadron scattering using analytic moments in the variable $s$ instead of the well-known Nachtmann variable $\xi$ and Bjorken variable $x$. We find new expressions for the structure functions $F_1$, $F_2$, and $F_3$ that depend on the target mass and agree with the spectral property.
Keywords: Jost–Lehmann–Dyson representation, structure function, inelastic lepton–hadron scattering, target mass correction.
Received: 08.12.2008
English version:
Theoretical and Mathematical Physics, 2009, Volume 160, Issue 3, Pages 1260–1273
DOI: https://doi.org/10.1007/s11232-009-0114-3
Bibliographic databases:
Language: Russian
Citation: O. P. Solovtsova, V. I. Lashkevich, “The Jost–Lehmann–Dyson representation and target mass effects”, TMF, 160:3 (2009), 471–486; Theoret. and Math. Phys., 160:3 (2009), 1260–1273
Citation in format AMSBIB
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\paper The~Jost--Lehmann--Dyson representation and target mass effects
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  • https://www.mathnet.ru/eng/tmf6410
  • https://doi.org/10.4213/tmf6410
  • https://www.mathnet.ru/eng/tmf/v160/i3/p471
  • This publication is cited in the following 2 articles:
    Citing articles in Google Scholar: Russian citations, English citations
    Related articles in Google Scholar: Russian articles, English articles
    Теоретическая и математическая физика Theoretical and Mathematical Physics
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    Abstract page:516
    Full-text PDF :185
    References:120
    First page:6
     
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