Conveners
High energy physics: Section 1
- Alexey Aparin (Joint Institute for Nuclear Research)
- Oleg Samoylov (JINR)
High energy physics: Theory
- Oleg Samoylov (JINR)
- Alexey Aparin (Joint Institute for Nuclear Research)
High energy physics: Section 2 Part 1
- Alexey Aparin (Joint Institute for Nuclear Research)
- Vadim Babkin (Joint Institute for Nuclear Research)
High energy physics: Section 2 Part 2
- Alexey Aparin (Joint Institute for Nuclear Research)
- Vadim Babkin (Joint Institute for Nuclear Research)
Ms
Diana Seitova
(LHEP JINR)
17/04/2019, 14:00
High Energy Physics
Oral
The work is devoted to the study of microscopic black hole production with the CMS experiment at LHC. One of the predictions of theoretical models with extra spatial dimensions and low-scale quantum gravity is the possibility of production of microscopic black holes in particle collisions, in particular, at colliders. Based on the simulation with the BlackMax and the Charybdis2 event...
Vladislav Shalaev
(JINR, Dubna State University)
17/04/2019, 14:15
High Energy Physics
Oral
The main subject of my reserach is the Drell-Yan process, in particular measurement of the polarization angular coefficients of Z boson which sesnsetive to (V –A) structure of weak interactions and can be indicators of effects from higher orders and QCD twists, as well as the nontrivial QCD vacuum structure. Also measurment of this coefficients is important for subsequent precision measurement...
Ms
Anastasia Kalitkina
(JINR, DLNP, University Centre, MSU)
17/04/2019, 14:30
High Energy Physics
Oral
Neutrino physics is a major part of modern science. Now in Dzhelepov Laboratory of Nuclear Problems of JINR, we are developing a global neutrino analysis software (GNA). The main goal of this program is to create some universal way to analyze any kind of neutrino experiments. At first, this problem has been being solved only for reactor neutrino experiments such as Day Bay, JUNO.
This talk...
Oksana Koval
(JINR)
17/04/2019, 14:45
High Energy Physics
Oral
А direct search for the production of a Higgs boson in association with single top quark is performed. The analysis considers single top quark production via t channel and uses Higgs boson decays to a bottom quark-antiquark pair and semileptonic top quark decays. Such process is strongly suppressed in the Standard Model. An observation of this production mode would be an unambiguous indication...
Ms
Aigul Baeva
(JINR,LHEP)
17/04/2019, 15:00
High Energy Physics
Oral
The main goal of the NA62 experiment at CERN is a study of the ultrarare decay К+ → pi nu nu. The collected statistics allows to analyse other rare decays, in particular, К+→ mu nu mu mu. Rare decays make it possible to experimentally investigate one of the aspects of the Standard Model, the chiral perturbative theory (ChPT). ChPT predicts decay probability of К→ mu nu mu mu: 1.35 х 10^(-8)....
Mr
Peter Parfenov
(MEPhI, Moscow)
17/04/2019, 15:15
High Energy Physics
Oral
The Multi-Purpose Detector (MPD) at NICA collider has a substantial discovery potential concerning the exploration of the QCD phase diagram in the region of high net-baryon densities and moderate temperatures. The anisotropic transverse flow is one of the key observables to study the properties of dense matter created in heavy-ion collisions. The MPD performance for anisotropic flow...
Mr
Faig Ahmadov
(JINR)
17/04/2019, 15:30
High Energy Physics
Oral
Analyzed the experimental data of ATLAS obtained in proton-proton collisions in Run-2 LHC at a centre-of-mass energy of 13 TeV for the period 2015-2017, corresponding to an integrated luminosity of 79.8fb^-1. The Run 2 VH, H → bb result is further combined with the results of other Run 2 searches for the Higgs boson produced in the VH production mode, but decaying into either two photons or...
Igor Denisenko
(JINR)
17/04/2019, 15:45
High Energy Physics
Oral
The inner part of the BESIII drift chamber is expected to be replaced with a cylindrical GEM (CGEM) tracker in summer 2019. Despite providing generally similar performance to the currently installed inner drift chamber, in may improve tracking of the low-momentum charged particles, which is strongly affected by the beam-induced background. Moreover, it can be seen as testing ground for...
Ms
Liudmila Kolupaeva
(JINR)
17/04/2019, 16:30
High Energy Physics
Oral
Neural networks become a wide-spread way to identify particles in the high energy experiments and neutrino physics follows this tendency. Primarily goal of the NOvA experiment is neutrino oscillation studies which require good identification for the nue and numu interactions. For this purpose, NOvA developed a convolutional neural network based particle identification algorithm CVN.
We check...
Mr
Ilnur Gabdrakhmanov
(JINR VBLHEP)
17/04/2019, 16:45
High Energy Physics
Oral
We review crossed channel Radon tomography of generalized parton distributions (GPD). We present a procedure to derive separate channel contributions to double distributions (DD) via limited angle inverse Radon transform (RT). The LO photon GPDs has been considered as a clear analytical test. Recently the pressure distribution inside proton has been derived where besides negative sign of the...
Mr
Anton Karpishkov
(Samara National Research University)
17/04/2019, 17:00
High Energy Physics
Oral
We study angular correlations in associated hadroproduction of Υ(1S) with the D± and D0 mesons at the LHC in the Leading Order of the parton Reggeization approach. This approach is based on the kT-factorisation and the gauge-ivariant effective field theory of L. N. Lipatov. Hadronization of a $\bar{b}b$-pair to Υ(1S) is described within the NRQCD-factorization framework. Production of D−mesons...
Mrs
Olena Mezhenska
(P. J. Šafárik University in Kosice)
17/04/2019, 17:15
High Energy Physics
Oral
The vector Ay and tensor analyzing powers Ayy and Axx for dp-elastic scattering were measured at the energy of 800 MeV and in the angular range from 60° to 140° in the center-of-mass system at the JINR Nuclotron. The experimental data are compared with the calculations obtained within framework of relativistic multiple scattering approach.
Mr
N MARI MUTHU
(Banaras Hindu University)
17/04/2019, 17:45
High Energy Physics
Oral
Relativistic nucleus-nucleus (A-A) and hadrons - nucleus (h-A) collisions are very useful to understand the particle production mechanism. The present work is devoted to the investigation on emitted charged pions from 84Kr36 - Emulsion interaction at 1 GeV/n. Here we have calculated the total number of wounded nucleons (W) and the total number of interactions (ν) using wounded nucleon model....
Alexey Chetverikov
(LNP)
18/04/2019, 14:00
High Energy Physics
Oral
Light collection module (LCM) is intended for registration a vacuum ultraviolet light in a liquid argon time projection chamber.
The core of the LCM is a WLS-fiber array, coated by TPB solution, which is fixed on a PVC plate.
LCM is being developed and made as a part of a light registration system of ArgonCube in Dzelepov Laboratory of nuclear problems at JINR.
ArgonCube is a...
Ms
Olga Golub
(NRNU MEPHi)
18/04/2019, 14:15
High Energy Physics
Oral
We present the energy dependence of the cross section for the inelastic interaction of protons and helium nuclei with the tungsten in the energy range from a few hundred MeV to a hundred GeV using the data of the PAMELA space experiment. It was intended for the precision measurements of the cosmic ray fluxes of different nature and include a set of detectors for the reliable determination of...
Mr
Ilya Moroz
(JINR, TGU)
18/04/2019, 14:30
High Energy Physics
Oral
In this work a stand to test preamplifiers for electromagnetic calorimeter of the MU2E experiment (Tevatron, Fermilab) is presented. For this stand the control board has been developed, assembled and tested. Methods to test preamplifiers are proposed. A software for stand is being debugged.
Mr
Aleksey Tishevskiy
(VBLHEP,JINR)
18/04/2019, 14:45
High Energy Physics
Oral
Modern silicon photomultipliers are widely used in detectors of a wide class of experiments CERN, FAIR and NICA/Nuclotron. One example of their application is electromagnetic and hadron calorimeters. In the Laboratory of high energy physics, 16-channel prototypes of detectors (with SIPM readout from Ketek, Sensl and Hamamatsu) were developed which can be used both in Zero Degree calorimetry...
Mr
Nikolay Karpushkin
(Institute for Nuclear Research of the Russian Academy of Sciences)
18/04/2019, 15:00
High Energy Physics
Oral
At present, new forward hadron lead/scintillator sampling calorimeters are constructed for the Compressed Baryonic Matter (CBM) experiment at the future Facility for Antiproton and Ion Research (FAIR) and the Multi Purpose Detector (MPD) at Nuclotron-based Ion Collider Facility (NICA). These calorimeters will be used for centrality and the reaction plane orientation measurements in heavy-ion...
Mr
Evgeny Kondratyuk
(IHEP)
18/04/2019, 15:15
High Energy Physics
Oral
The charged-particle veto (CPV) detector of the ALICE experiment is a multi-wire proportional chamber with pad readout. It is designed to improve photon identification in the photon spectrometer PHOS. One module of the CPV detector was put in operation during LHC Run2 in 2015. In this talk we will present the performance of the CPV during PbPb collisions at \sqrt{s}=5.02 TeV and compare these...
Mr
Ilya Butorov
(JINR)
18/04/2019, 15:30
High Energy Physics
Oral
Currently active work on preparation of JUNO reactor neutrino experiment in China is underway. The primary goal of the experiment is the determination of neutrino mass hierarchy. Alongside with that the precision of some other neutrino mixing parameters can be improved. In order to reach these ambitious goals the detector of the experiment is supposed to have unprecedented resolution on the...
Mr
Andrei Galavanov
(JINR, MEPhI)
18/04/2019, 15:45
High Energy Physics
Oral
BM@N (Baryonic Matter at the Nuclotron) is the fixed target experiment aimed to study nuclear matter in the relativistic heavy ion collisions at the Nuclotron accelerator in JINR. Detectors based on Gas Electron multipliers (GEM) have been identified as appropriate for the BM@N central tracking system, which is located inside the BM@N analyzing magnet. Cathode Strip Chamber (CSC) is installed...
Ms
Gaukhar Zhanabergen
(JINR)
18/04/2019, 16:30
High Energy Physics
Oral
Studying of the extremal hot and dense matter is the most pressing challenge of modern physics. The particular interest to such environments is connecting with the chance to learn new and until the poorly studied state of matter, so-called quark-gluon plasma. Is supposed by MPD installation to use all the advantages of the accelerator with high NICA luminosity. Installation MPD consists of...
Mr
Dmitrii Nesterov
(St Petersburg State University)
18/04/2019, 16:45
High Energy Physics
Oral
The Inner Tracking System (ITS) plays a key role in the precise determination of secondary vertices in high energy hadron collisions in A Large Ion Collider Experiment (ALICE) at the Large Hadron Collider (LHC). After the upgrade in 2020 the beam luminosity of the LHC will be increased by a factor of ten refers to Pb-Pb collisions. This will provide new opportunities of studies of rare...
Mr
Evgenii Mitrofanov
(JINR)
18/04/2019, 17:00
High Energy Physics
Oral
Cold nuclear matter effects such as parton energy loss in nuclear matter and nuclear modification of parton distribution functions in the Drell-Yan process in πA and pA collisions have been extensively studied during the last 30 years. Various theoretical models have been proposed to explain these effects, but its full understanding is still lacking.
COMPASS studies nuclear effects in...
Mr
Vladislav Alekseev
(Yaroslavl State University)
18/04/2019, 17:15
High Energy Physics
Oral
The sampling imaging electromagnetic calorimeter of $\approx 16.3$ radiation lengths and $\approx 0.6$ nuclear interaction length designed and constructed by the PAMELA collaboration as a part of the large magnetic spectrometer PAMELA. Calorimeter consists of 44 single-sided silicon sensor planes interleaved with 22 plates of tungsten absorber (thickness of each tungsten layer $0.26$ cm)....
Mr
Alexander Strijak
(INR RAS)
18/04/2019, 17:30
High Energy Physics
Oral
At present, in Dubna, Russia a new acceleration complex NICA is being constructed. One of its two detectors and most integral parts of the collider (NICA) is a Multi-Purpose Detector (MPD). MPD experiment is intended for study of properties of dense baryonic matter. One of the most important parts of MPD is Forward Hadron Calorimeter (FHCal), whose purpose is to measure centrality and...
Mr
Arseniy Shabanov
(INR RAS)
18/04/2019, 17:45
High Energy Physics
Oral
HADES is a large acceptance spectrometer operating at SIS18, GSI, Germany. It is aimed at exploration of QCD phase diagram at the ion beam energies of 1-2 AGeV in the region of high hadron densities. HADES setup includes a superconducting toroidal magnet, sets of drift chambers, ring-imaging Cherenkov detector, TOF systems and a new electromagnetic calorimeter (ECAL). The application of an...
Mr
Aman Phogat
(University of Delhi)
18/04/2019, 18:00
High Energy Physics
Oral
The present study includes the integration and commissioning of Resistive Plate Chambers (RPCs) detector with HARDROC front-end electronics. HARDROC is a 64 input channel ASIC that amplifies, shapes and discriminates the negative fast detector signals. This paper reports the performance of glass RPC detector under different R134a/i-C4H10/SF6 gas mixture compositions. The preamplifier gain, DAC...
Dr
Alexander Verkheev
(JINR)
18/04/2019, 18:15
The PANDA Experiment will be one of the key experiments at the Facility for Antiproton and Ion Research (FAIR) which is under construction now in the territory of the GSI Helmholtz Centre for Heavy Ion Research in Darmstadt, Germany. PANDA is aimed to study hadron spectroscopy and various topics of the weak and strong forces. Muon System is chosen as the most suitable technology for detecting...
