000169108 001__ 169108
000169108 005__ 20211110124219.0
000169108 0247_ $$2arXiv$$aarXiv:1405.4295
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000169108 037__ $$aDESY-2014-02794
000169108 041__ $$aEnglish
000169108 0881_ $$aDESY-14-069; IPPP/14/35; DCPT/14/70; CERN-PH-TH/2014-083; KCL-PH-TH/2014-22; arXiv:1405.4295
000169108 088__ $$2DESY$$aDESY-14-069
000169108 088__ $$2IPPP$$aIPPP/14/35
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000169108 088__ $$2CERN$$aCERN-PH-TH/2014-083
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000169108 088__ $$2arXiv$$aarXiv:1405.4295
000169108 1001_ $$0P:(DE-H253)PIP1014870$$aSchlaffer, Matthias$$b0$$eCorresponding Author
000169108 245__ $$aBoosted Higgs Shapes
000169108 260__ $$c2014
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000169108 3367_ $$0PUB:(DE-HGF)15$$2PUB:(DE-HGF)$$aInternal Report$$mintrep
000169108 500__ $$a17 pages, 7 figures, 6 tables
000169108 520__ $$aThe inclusive Higgs production rate through gluon fusion has been measured to be in agreement with the Standard Model (SM). We show that even if the inclusive Higgs production rate is very SM-like, a precise determination of the boosted Higgs transverse momentum shape offers the opportunity to see effects of natural new physics. These measurements are generically motivated by effective field theory arguments and specifically in extensions of the SM with a natural weak scale, like composite Higgs models and natural supersymmetry. We show in detail how a measurement at high transverse momentum of $H\rightarrow 2\ell +\mathbf {p}\!\!/_\mathrm{T}$ via $H\rightarrow \tau \tau $ and $H\rightarrow WW^*$ could be performed and demonstrate that it offers a compelling alternative to the $t\bar{t} H$ channel. We discuss the sensitivity to new physics in the most challenging scenario of an exactly SM-like inclusive Higgs cross section.
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000169108 650_7 $$2INSPIRE$$aHiggs particle: boosted particle
000169108 650_7 $$2INSPIRE$$atransverse momentum: high
000169108 650_7 $$2INSPIRE$$aHiggs model: composite
000169108 650_7 $$2INSPIRE$$agluon: fusion
000169108 650_7 $$2INSPIRE$$ascale: electroweak interaction
000169108 650_7 $$2INSPIRE$$atop: pair production
000169108 650_7 $$2INSPIRE$$anew physics
000169108 650_7 $$2INSPIRE$$aeffective field theory
000169108 650_7 $$2INSPIRE$$asupersymmetry
000169108 650_7 $$2INSPIRE$$asensitivity
000169108 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000169108 7001_ $$0P:(DE-HGF)0$$aSpannowsky, Michael$$b1
000169108 7001_ $$0P:(DE-HGF)0$$aTakeuchi, Michihisa$$b2
000169108 7001_ $$0P:(DE-H253)PIP1013656$$aWeiler, Andreas$$b3
000169108 7001_ $$0P:(DE-HGF)0$$aWymant, Chris$$b4
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000169108 9141_ $$y2014
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