37,045 research outputs found
Right unimodal and bimodal singularities in positive characteristic
The problem of classification of real and complex singularities was initiated
by Arnol'd in the sixties who classified simple, unimodal and bimodal w.r.t.
right equivalence. The classification of right simple singularities in positive
characteristic was achieved by Greuel and the author in 2014. In the present
paper we classify right unimodal and bimodal singularities in positive
characteristic by giving explicit normal forms. Moreover we completely
determine all possible adjacencies of simple, unimodal and bimodal
singularities. As an application we prove that, for singularities of right
modality at most 2, the -constant stratum is smooth and its dimension is
equal to the right modality. In contrast to the complex analytic case, there
are, for any positive characteristic, only finitely many 1-dimensional (resp.
2-dimensional) families of right class of unimodal (resp. bimodal)
singularities. We show that for fixed characteristic of the ground field,
the Milnor number of satisfies , if the right modality of
is at most 2.Comment: 19 page
Invariants of plane curve singularities and Pl\"ucker formulas in positive characteristic
We study classical invariants for plane curve singularities ,
an algebraically closed field of characteristic : Milnor number,
delta invariant, kappa invariant and multiplicity. It is known, in
characteristic zero, that and that
. For arbitrary characteristic,
Deligne prove that there is always the inequality by showing that
measures the wild vanishing cycles. By introducing new invariants
, we prove in this note that with equalities
if and only if the characteristic does not divide the multiplicity of any
branch of . As an application we show that if is "big" for (in fact
), then has no wild vanishing cycle. Moreover we obtain some
Pl\"ucker formulas for projective plane curves in positive characteristic.Comment: 15 pages; final version; to appear in the Annales de l'Institut
Fourie
Was the Higgs boson discovered?
The standard model has postulated the existence of a scalar boson, named the
Higgs boson. This boson plays a central role in a symmetry breaking scheme
called the Brout-Englert-Higgs mechanism (or the
Brout-Englert-Higgs-Guralnik-Hagen-Kibble mechanism, for completeness) making
the standard model realistic. However, until recently at least, the
50-year-long-sought Higgs boson had remained the only particle in the standard
model not yet discovered experimentally. It is the last but very important
missing ingredient of the standard model. Therefore, searching for the Higgs
boson is a crucial task and an important mission of particle physics. For this
purpose, many theoretical works have been done and different experiments have
been organized. It may be said in particular that to search for the Higgs boson
has been one of the ultimate goals of building and running the LHC, the world's
largest and most powerful particle accelerator, at CERN, which is a great
combination of science and technology. Recently, in the summer of 2012, ATLAS
and CMS, the two biggest and general-purpose LHC collaborations, announced the
discovery of a new boson with a mass around 125 GeV. Since then, for over two
years, ATLAS, CMS and other collaborations have carried out intensive
investigations on the newly discovered boson to confirm that this new boson is
really the Higgs boson (of the standard model). It is a triumph of science and
technology and international cooperation. Here, we will review the main results
of these investigations following a brief introduction to the Higgs boson
within the theoretical framework of the standard model and Brout-Englert-Higgs
mechanism as well as a theoretical and experimental background of its search.
This paper may attract interest of not only particle physicists but also a
broader audience.Comment: LateX, 23 pages, 01 table, 9 figures. To appear in Commun. Phys.
Version 2: Minor changes, two references adde
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