Home > Publications database > Hadronic energy distributions in deep-inelastic electron-proton scattering > print

001     389967
005     20250804165417.0
024 7 _ |a 10.1007/BF01566687
|2 doi
024 7 _ |a 1434-6044
|2 ISSN
024 7 _ |a 1434-6052
|2 ISSN
024 7 _ |2 WOS
|a WOS:00
024 7 _ |a inspire:355326
|2 inspire
024 7 _ |a openalex:W2157042157
|2 openalex
037 _ _ |a PUBDB-2017-09180
041 _ _ |a English
082 _ _ |a 530
100 1 _ |a Derrick, M.
|b 0
245 _ _ |a Hadronic energy distributions in deep-inelastic electron-proton scattering
260 _ _ |a Berlin
|c 1993
|b Springer
336 7 _ |a article
|2 DRIVER
336 7 _ |a Output Types/Journal article
|2 DataCite
336 7 _ |a Journal Article
|b journal
|m journal
|0 PUB:(DE-HGF)16
|s 1503642455_29893
|2 PUB:(DE-HGF)
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a Journal Article
|0 0
|2 EndNote
500 _ _ |a ZEUS
520 _ _ |a This paper presents energy distributions of the hadronic system produced in neutral-current electron-proton deep-inelastic scattering at a centre of mass energy of 296 GeV. Comparison of the results with QCD Monte Carlo models shows that QCD radiation has a strong influence on the characteristics of the final state. The data are reasonably reproduced by the Lund model based on a matrix element calculation in first order ofαs, followed by appropriate parton showers, as well as by the colour dipole model. The HERWIG parton shower model also gives a reasonable representation of the data. Neither the first order matrix elements alone nor the Lund parton shower model, without the matrix element calculation, reproduce the data.
536 _ _ |a 899 - ohne Topic (POF3-899)
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588 _ _ |a Dataset connected to CrossRef
693 _ _ |0 EXP:(DE-MLZ)NOSPEC-20140101
|5 EXP:(DE-MLZ)NOSPEC-20140101
|e No specific instrument
|x 0
700 1 _ |a Krakauer, D.
|b 1
700 1 _ |a Magill, S.
|b 2
700 1 _ |a Musgrave, B.
|b 3
700 1 _ |a Repond, J.
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700 1 _ |a Repond, S.
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700 1 _ |a Stanek, R.
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700 1 _ |a Lane, J. B.
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700 1 _ |a Adamus, M.
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