XXXI International workshop on high energy physics "Critical points in the modern particle physics"

Session

Morning session

1

5 Jul 2017, 09:00

NRC "Kurchatov Institute", SRC RF IHEP, Protvino

2. Opening address

Vladimir Petrov (IHEP)

05/07/2017, 09:00

Talk

3. Searches for Supersymmetry in ATLAS

Alberto Cervelli (INFN, Bologna, Italy)

05/07/2017, 09:10

Talk

32. Searches in ATLAS

Oleg Zenin (IHEP, Protvino)

05/07/2017, 09:50

Talk

Recent results of searches for TeV-scale BSM phenomena in proton-proton collisions at $\sqrt{s} = 13$~TeV with ATLAS detector are presented.
The report covers searches for objects and signatures originating from a variety of SM extensions:extended Higgs sector, extra gauge bosons, heavy and excited quarks leptoquarks, extra dimensions, contact interactions.

29. Overview of ALICE results

Dmitri Peresunko (NRC Kurchatov Institute)

05/07/2017, 10:40

Talk

The ALICE experiment at the LHC performs comprehensive studies of the QCD matter with pp, p-Pb and Pb-Pb collisions. A complete set of observables measured by ALICE allows one to study particle production in QCD vacuum in pp collisions, investigate initial-state and possible collective effects in p-Pb collisions and explore properties of the deconfined quark-gluon matter at high temperature...

5. Lattice QCD, Heavy Ion Collisions, and QCD Phase Structure

Atsushi Nakamura (FEFU, Vladivostok)

05/07/2017, 11:15

Talk

One of the important missions of high energy heavy ion collisions is to reveal the QCD phase structure at finite temperature and baryon density. Lattice QCD simulations are expected to provide valuable information as a first principle calculation of QCD. However, lattice simulations at finite baryon density have suffered from the `sign problem' and no calculations were successful except at...

6. Decay properties of the B and Bs mesons

Ajaykumar Rai (SVNIT, Surat, India)

Talk

For study of masses of the ground, orbitally and radially excited states of heavy-light $B$ and $B_S$ meson using Cornell potential with $\mathcal{O}(1/m)$ correction to the potential energy term. We have also incorporated the relativistic correction to the kinetic energy term of the Hamiltonian. The spin-hyperfine, the spin-orbit and the tensor interactions as well as the effect of mixing are...