Domizia Orestano
(Universita di Roma Tre)
27/09/2010, 14:50
Alexandre Nikitenko
(Imperial College)
27/09/2010, 15:30
Phillip Gutierrez
(University of Oklahoma),
Phillip Gutierrez
(University of Oklahoma-Unknown-Unknown)
27/09/2010, 16:40
Maria Rozanska
(Institute of Nuclear Physics PAN)
27/09/2010, 17:20
Tobias Hurth
(CERN)
28/09/2010, 09:00
Radovan Dermisek
28/09/2010, 09:35
Andrew Akeroyd
28/09/2010, 10:40
Claudio Verzegnassi
(Univ. + INFN)
28/09/2010, 11:15
Oscar Stål
(DESY)
28/09/2010, 11:50
Michael Kraemer
(Particle Physics)
28/09/2010, 14:00
Marco Zaro
(Center for Particle Physics and Phenomenology)
28/09/2010, 14:25
Ilya Ginzburg
(Sobolev Inst)
28/09/2010, 14:45
Michael Gustafsson
28/09/2010, 15:05
Ilya Ginzburg
(Sobolev Inst)
28/09/2010, 15:55
Glenn Wouda
(Uppsala University)
28/09/2010, 16:15
Ayse Cagil
(Exptl. High Energy Physics Lab.-Physics Department-Middle East T)
28/09/2010, 16:35
Maria Krawczyk
(Warsaw University of Technology),
Per Osland
(Unknown)
28/09/2010, 17:00
Martin Flechl
(Universität Freiburg), Prof.
Stefano Moretti
(NExT Institute)
28/09/2010, 17:30
Ketevi Adikle Assamagan
(Department of Physics),
Sven Heinemeyer
(CERN)
28/09/2010, 17:50
Tilman Plehn
(Heidelberg University)
29/09/2010, 09:00
Oliver Brein
(Universitaet Freiburg)
29/09/2010, 09:25
Johan Christoffer Rathsman
(Department of Physics and Astronomy-University of Uppsala)
29/09/2010, 09:50
Dr
Nazila Mahmoudi
(Clermont-Ferrand)
29/09/2010, 10:10
Prof.
Christopher Kolda
(University of Notre Dame)
29/09/2010, 11:05
Rui Santos
(University of Southampton and NExT Institute)
29/09/2010, 11:25
Jaime Hernández
(Benemerita Universidad Autónoma de Puebla)
29/09/2010, 11:45
Martin Jung
(IFIC)
29/09/2010, 12:05
Sven Heinemeyer
(CERN)
29/09/2010, 12:25
Yann Coadou
(CPPM Marseille)
29/09/2010, 14:00
Dr
Jyothsna Rani KOMARAGIRI
(Karlsruher Institut für Technologie (KIT))
29/09/2010, 14:25
Mr
Matti Kortelainen
(Helsinki Institute of Physics (HIP))
29/09/2010, 14:50
Camille Belanger-Champagne
(Dept. of Nuclear and Particle Phys.-University of Uppsala)
29/09/2010, 15:15
Arnaud Ferrari
(University of Uppsala)
29/09/2010, 16:05
Michele Gallinaro
(LIP Lisbon)
29/09/2010, 16:30
Alexandros Attikis
(University of Cyprus-Unknown-Unknown)
29/09/2010, 16:55
Dr
Fabien Tarrade
(Brookhaven National Laboratory)
29/09/2010, 17:20
Martin Flechl
(Universität Freiburg)
29/09/2010, 17:45
Simonetta Gentile
(Universita di Roma I "La Sapienza")
30/09/2010, 09:30
Lauri Andreas Wendland
(Helsinki Institute of Physics (HIP) - Univ. of Helsinki, Fac. of)
30/09/2010, 09:55
Miika Klemetti
(McGill University)
30/09/2010, 10:20
Dr
Un-ki Yang
(University of Manchester)
30/09/2010, 11:15
Marco Battaglia
(UCSC and CERN)
30/09/2010, 11:40
Karl Jakobs
(Fakultaet fuer Physik)
30/09/2010, 13:30
Prof.
Stefano Moretti
(NExT Institute)
30/09/2010, 14:15
Rui Santos
(University of Southampton and NExT Institute)
The LHC has started colliding protons. Several extensions of the Standard Model predict a charged scalar particle which according to the LEP bound
could be as light as 100 GeV. In this work we compare the four flavour conserving Yukawa versions of a CP-conserving two-Higgs doublet model (2HDM) regarding charged Higgs production and decay. We define a set of benchmarks where an early detection...
Prof.
Ilya Ginzburg
(Sobolev Inst. of Mathematics SB RAS)
We propose method for using of production od charged Higgs pair in
$e^+e^-$ collisions (at LC) for discovery of Dark Matter (DM) particles and measuring of their mass if they appear as scalar of Inert doublet model. In many cases this approach is also useful for another mechanisms of DM.
Marco Zaro
(Center for Particle Physics and Phenomenology)
We present the total cross sections at next-to-next-to-leading order (NNLO) in the strong coupling for single and double charged Higgs production via weak boson fusion. Results are obtained via the structure function approach, which builds upon the approximate, though very accurate, factorization of the QCD corrections between the two quark lines. We also provide ans estimate for the...
Dr
Jyothsna Rani KOMARAGIRI
(Karlsruher Institut für Technologie (KIT))
The identification of jets containing the weak decay of a B-hadron is an essential tool for a wide range of analyses in the context of the Standard Model and beyond. A variety of algorithms exploit the long lifetime and the presence of soft leptons to discriminate these jets from those associated to light quarks. The distributions of the corresponding observables - track impact parameters,...
Dr
Ayse Cagil
(Exptl. High Energy Physics Lab.-Physics Department-Middle East T)
Little higgs models, as a result of extended symmetry group of S.M contain heavy scalars in their content of particles. In the littlest Higgs model of little Higgs models there exists a new heavy scalar triplet.The physical states of this trilet contains a double charged scalar, a single charged scalar, as well as a neutral scalar and a neutral pseudoscalar. In little higgs models a majorana...
Prof.
Ilya Ginzburg
(Sobolev Inst)
We discuss thermal evolution of Universe after inflation in the frame of Inert doublet model in the case when modern state of Universe with dark matter is described by inert doublet model.
Dr
Jaime Hernández-Sánchez
(Benemerita Universidad Autónoma de Puebla)
We discuss the implications of assuming a four-zero Yukawa texture for the properties of the charged Higgs boson within the context of the general 2-Higgs Doublet Model of Type III. We begin by presenting a detailed analysis of the charged Higgs boson couplings with heavy quarks and the resulting pattern for its decays, including the decay $H^+ \to W^+ \gamma$ at 1-loop level. The parameters...
Mr
Matti Kortelainen
(Helsinki Institute of Physics)
The reconstruction of the missing transverse energy and jets, the trigger
plans and the reconstruction efficiencies in the CMS detector are discussed.
The performance with the 7 TeV proton-proton collision data is presented.
Domizia Orestano
(Universita di Roma Tre and INFN)
The ATLAS Experiment at the CERN Large Hadron Collider
was operated with colliding proton beams at 7 TeV center of mass energy
since March 2010. It will study a broad range of particle physics at the
highest available laboratory energies, from measurements of the standard
model to searches for new physics beyond the standard model.
At the time of writing ATLAS, with high data taking...
Dr
Yann Coadou
(CPPM Marseille)
Analysis tools and backgrounds
Tau leptons will play an important role in the physics program at the
LHC. In particular, they provide a useful signature in searches for
new phenomena like charged Higgs bosons or Supersymmetry. In addition,
they are being used for standard model electroweak measurements and
for detector related studies such as the determination of the missing
transverse energy scale.
Due to the huge...
