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@ARTICLE{CarvalhoDorsch:300804,
author = {Carvalho Dorsch, Gláuber and Huber, S. J. and Mimasu, K.
and No, J. M.},
title = {{H}ierarchical versus degenerate 2{HDM}: {T}he {LHC} run 1
legacy at the onset of run 2},
journal = {Physical review / D},
volume = {93},
number = {11},
issn = {2470-0010},
address = {[S.l.]},
publisher = {Soc.},
reportid = {PUBDB-2016-02424, DESY-15-240. arXiv:1601.04545},
pages = {115033},
year = {2016},
abstract = {Current discussions of the allowed two-Higgs-doublet model
parameter space after LHC run 1 and theprospects for run 2
are commonly phrased in the context of a quasidegenerate
spectrum for the new scalars.Here, we discuss the generic
situation of a two-Higgs-doublet model with a nondegenerate
spectrum for thenew scalars. This is highly motivated from a
cosmological perspective since it naturally leads to a
stronglyfirst-order electroweak phase transition that could
explain the matter-antimatter asymmetry in the
Universe.While constraints from measurements of Higgs signal
strengths do not change, those from searches of newscalar
states get modified dramatically once a nondegenerate
spectrum is considered.},
cin = {T},
ddc = {530},
cid = {I:(DE-H253)T-20120731},
pnm = {611 - Fundamental Particles and Forces (POF3-611) /
EWBGANDLHC - Electroweak Baryogenesis in the Era of the LHC
(625809)},
pid = {G:(DE-HGF)POF3-611 / G:(EU-Grant)625809},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000378375300003},
eprint = {1601.04545},
howpublished = {arXiv:1601.04545},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:1601.04545;\%\%$},
doi = {10.1103/PhysRevD.93.115033},
url = {https://bib-pubdb1.desy.de/record/300804},
}