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001     276034
005     20250731122646.0
024 7 _ |a 10.1016/j.nuclphysbps.2009.03.133
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024 7 _ |a 0920-5632
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024 7 _ |a 1873-3832
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024 7 _ |a arXiv:0901.3037
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088 1 _ |a MAN-HEP-2009-3; CERN-TH-2009-012; arXiv:0901.3037
088 _ _ |a MAN-HEP-2009-3
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088 _ _ |a CERN-TH-2009-012
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088 _ _ |a arXiv:0901.3037
|2 arXiv
100 1 _ |a Forshaw, J. R.
|b 0
111 2 _ |a Ringberg Workshop on New Trends in HERA Physics 2008
|c Ringberg Castle
|d 2008-10-05 - 2008-10-10
|w Germany
245 _ _ |a Soft gluons and superleading logarithms in QCD
260 _ _ |a Amsterdam
|c 2009
|b Elsevier
336 7 _ |a Journal Article
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336 7 _ |a article
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336 7 _ |a Journal Article
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336 7 _ |a ARTICLE
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336 7 _ |a Internal Report
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520 _ _ |a After a brief introduction to the physics of soft gluons in QCD we present a surprising prediction. Dijet production in hadron-hadron collisions provides the paradigm, i.e. h_1 +h_2 \to jj+X. In particular, we look at the case where there is a restriction placed on the emission of any further jets in the region in between the primary (highest p_T) dijets. Logarithms in the ratio of the jet scale to the veto scale can be summed to all orders in the strong coupling. Surprisingly, factorization of collinear emissions fails at scales above the veto scale and triggers the appearance of double logarithms in the hard sub-process. The effect appears first at fourth order relative to the leading order prediction and is subleading in the number of colours.
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693 _ _ |a HERA
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700 1 _ |a Seymour, M. H.
|b 1
773 _ _ |a 10.1016/j.nuclphysbps.2009.03.133
|g Vol. 191, p. 257 - 267
|0 PERI:(DE-600)1466572-4
|p 257 - 267
|t Nuclear physics / B / Proceedings supplements
|v 191
|y 2009
|x 0920-5632
787 0 _ |a Grindhammer, Guenter et.al.
|d Hamburg : Deutsches Elektronen-Synchrotron, DESY, Hamburg, 2009
|i IsPartOf
|0 PUBDB-2015-04349
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|t HERA 2008, proceedings of the Ringberg Workshop New Trends in HERA Physics 2008, Ringberg Castle, Tegernsee, Germany, 5-10 October 2008
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