270 research outputs found
Radiative Corrections for Pion Polarizability Experiments
We use the semi-analytical program RCFORGV to evaluate radiative corrections
to one-photon radiative emission in the high-energy scattering of pions in the
Coulomb field of a nucleus with atomic number Z. It is shown that radiative
corrections can simulate a pion polarizability effect. The average effect was
estimated for pion energies 40-600 GeV. We also study the range of
applicability of the equivalent photon approximation in describing one-photon
radiative emission.Comment: 11 pages (LaTex), 6 figures, 1 table. No changes in the paper. New
submission because old files are corrupted in arXi
Quadrupole polarizabilities of the pion in the Nambu--Jona-Lasinio model
The electromagnetic dipole and quadrupole polarizabilities of the neutral and
charged pions are calculated in the Nambu--Jona-Lasinio model. Our results
agree with the recent experimental analysis of these quantities based on
Dispersion Sum Rules. Comparison is made with the results from the Chiral
Perturbation Theory.Comment: 9 pages, 1 fi
ĐĐżĐžĐŽĐ”ĐŒĐžĐŸĐ»ĐŸĐłĐžŃ ŃĐœĐŽĐŸĐżŃĐŸŃДзОŃĐŸĐČĐ°ĐœĐžŃ ŃĐ°Đ·ĐŸĐ±Đ”ĐŽŃĐ”ĐœĐœĐŸĐłĐŸ Đž ĐșĐŸĐ»Đ”ĐœĐœĐŸĐłĐŸ ŃŃŃŃĐ°ĐČĐŸĐČ Đž пДŃОпŃĐŸŃĐ”Đ·ĐœĐŸĐč ĐžĐœŃĐ”ĐșŃОО ĐČ Đ ĐŸŃŃĐžĐčŃĐșĐŸĐč ЀДЎДŃĐ°ŃОО
Background. Since there is no national arthroplasty registry in the Russian Federation, the exact number of arthroplasty operations performed is unknown. Aim of the study to evaluate the epidemiology of primary, revision hip and knee arthroplasty and periprosthetic joint infection in Russian Federation. Materials and Methods. The inquires were made to 85 subjects, 73 federal state budget institutions and 30 private hospitals. Results. Answers were received from 76 subjects of Russian Federation, 41 federal and 18 private hospitals. The studied indicators revealed to be pretty much heterogenic. The decrease of operations number from 20% to 40% in subjects of Russian Federation due to SARS-CoV-2 pandemic forced us to make no analysis for these 2020 indicators in Russian Federation generally. 147 061 primary hip and knee arthroplasties were performed in 2019 in Russian Federaion. 7 770 revison hip and knee arthroplasties were done. 6 606 cases of severe orthopaedic implant-assosiated infection were cured including 4 282 cases post hip and knee arthroplasties that constitutes 2,91 % from primary arthroplasties. Conclusions. The frequency of periprosthetic joint infection in Russian Federation correlates to the world data. High complexity for patients routing with implant-assosiated infection and strong demand for Federal Center of implant-assosiated orthopaedic infection are revealed.ĐĐșŃŃĐ°Đ»ŃĐœĐŸŃŃŃ. ĐĐŸŃĐșĐŸĐ»ŃĐșŃ ĐČ Đ ĐŸŃŃĐžĐčŃĐșĐŸĐč ЀДЎДŃĐ°ŃОО ĐŸŃŃŃŃŃŃĐČŃĐ”Ń ĐœĐ°ŃĐžĐŸĐœĐ°Đ»ŃĐœŃĐč ŃДгОŃŃŃ Đ°ŃŃŃĐŸĐżĐ»Đ°ŃŃĐžĐșĐž, ŃĐŸŃĐœĐŸĐ” ŃĐžŃĐ»ĐŸ ĐČŃĐżĐŸĐ»ĐœĐ”ĐœĐœŃŃ
ĐŸĐżĐ”ŃĐ°ŃĐžĐč ŃĐœĐŽĐŸĐżŃĐŸŃДзОŃĐŸĐČĐ°ĐœĐžŃ ĐœĐ”ĐžĐ·ĐČĐ”ŃŃĐœĐŸ. ĐŠĐ”Đ»Ń ĐžĐ·ŃŃĐžŃŃ ŃĐżĐžĐŽĐ”ĐŒĐžĐŸĐ»ĐŸĐłĐžŃ ŃĐœĐŽĐŸĐżŃĐŸŃДзОŃĐŸĐČĐ°ĐœĐžŃ ĐșĐŸĐ»Đ”ĐœĐœĐŸĐłĐŸ Đž ŃĐ°Đ·ĐŸĐ±Đ”ĐŽŃĐ”ĐœĐœĐŸĐłĐŸ ŃŃŃŃĐ°ĐČĐŸĐČ, Đ° ŃĐ°ĐșжД пДŃОпŃĐŸŃĐ”Đ·ĐœĐŸĐč ĐžĐœŃĐ”ĐșŃОО (ĐĐĐ) ĐČ Đ ĐŸŃŃĐžĐčŃĐșĐŸĐč ЀДЎДŃĐ°ŃОО (РЀ). ĐĐ°ŃĐ”ŃОал Đž ĐŒĐ”ŃĐŸĐŽŃ. ĐĄĐŽĐ”Đ»Đ°ĐœŃ Đ·Đ°ĐżŃĐŸŃŃ ĐČ 85 ŃŃбŃĐ”ĐșŃĐŸĐČ, 73 ŃДЎДŃĐ°Đ»ŃĐœŃŃ
ĐłĐŸŃŃĐŽĐ°ŃŃŃĐČĐ”ĐœĐœŃŃ
бŃЎжДŃĐœŃŃ
ŃŃŃĐ”Đ¶ĐŽĐ”ĐœĐžŃ Đž 30 ŃĐ°ŃŃĐœŃŃ
ŃŃŃĐ”Đ¶ĐŽĐ”ĐœĐžĐč Đ·ĐŽŃĐ°ĐČĐŸĐŸŃ
ŃĐ°ĐœĐ”ĐœĐžŃ. РДзŃĐ»ŃŃĐ°ŃŃ. ĐĐŸĐ»ŃŃĐ”ĐœŃ ĐŸŃĐČĐ”ŃŃ ĐžĐ· 76 ŃŃбŃĐ”ĐșŃĐŸĐČ Đ Đ€, 41 ŃДЎДŃĐ°Đ»ŃĐœĐŸĐłĐŸ Đž 18 ŃĐ°ŃŃĐœŃŃ
ŃŃŃĐ”Đ¶ĐŽĐ”ĐœĐžĐč Đ·ĐŽŃĐ°ĐČĐŸĐŸŃ
ŃĐ°ĐœĐ”ĐœĐžŃ. Đ 2020 Đł. ŃŃŃĐ°ĐœĐŸĐČĐ»Đ”ĐœĐ° Đ·ĐœĐ°ŃĐžŃДлŃĐœĐ°Ń ĐłĐ”ŃĐ”ŃĐŸĐłĐ”ĐœĐœĐŸŃŃŃ ĐžĐ·ŃŃĐ°Đ”ĐŒŃŃ
ĐżĐŸĐșĐ°Đ·Đ°ŃДлДĐč: ŃĐœĐžĐ¶Đ”ĐœĐžĐ” ŃĐžŃла ĐŸĐżĐ”ŃĐ°ŃĐžĐč ŃĐŸŃŃĐ°ĐČĐžĐ»ĐŸ ĐŸŃ 20 ĐŽĐŸ 40% ĐČ ŃазлОŃĐœŃŃ
ŃŃбŃĐ”ĐșŃĐ°Ń
РЀ ĐČ ŃĐČŃĐ·Đž Ń ĐżĐ°ĐœĐŽĐ”ĐŒĐžĐ”Đč SARS-CoV-2, ĐżĐŸŃŃĐŸĐŒŃ ĐżĐŸĐșĐ°Đ·Đ°ŃДлО 2020 Đł. ŃĐ”ŃĐ”ĐœĐŸ бŃĐ»ĐŸ ĐœĐ” Đ°ĐœĐ°Đ»ĐžĐ·ĐžŃĐŸĐČĐ°ŃŃ ĐżĐŸ Đ ĐŸŃŃОО ĐČ ŃĐ”Đ»ĐŸĐŒ. Đ 2019 Đł. ĐČ Đ Đ€ ĐČŃĐżĐŸĐ»ĐœĐ”ĐœĐŸ 147 061 ĐŸĐżĐ”ŃĐ°ŃĐžĐč пДŃĐČĐžŃĐœĐŸĐłĐŸ ŃĐœĐŽĐŸĐżŃĐŸŃДзОŃĐŸĐČĐ°ĐœĐžŃ ĐșĐŸĐ»Đ”ĐœĐœĐŸĐłĐŸ Đž ŃĐ°Đ·ĐŸĐ±Đ”ĐŽŃĐ”ĐœĐœĐŸĐłĐŸ ŃŃŃŃĐ°ĐČĐŸĐČ, 7 770 ŃĐ”ĐČĐžĐ·ĐžĐŸĐœĐœŃŃ
Đ°ŃŃŃĐŸĐżĐ»Đ°ŃŃĐžĐș ĐșĐŸĐ»Đ”ĐœĐœĐŸĐłĐŸ Đž ŃĐ°Đ·ĐŸĐ±Đ”ĐŽŃĐ”ĐœĐœĐŸĐłĐŸ ŃŃŃŃĐ°ĐČĐŸĐČ. Đ 2019 Đł. ĐżŃĐŸĐ»Đ”ŃĐ”ĐœĐŸ 6 606 ŃĐ»ŃŃĐ°Đ”ĐČ ŃŃĐ¶Đ”Đ»ĐŸĐč ĐŸŃŃĐŸĐżĐ”ĐŽĐžŃĐ”ŃĐșĐŸĐč ĐžĐŒĐżĐ»Đ°ĐœŃĐ°Ń-Đ°ŃŃĐŸŃООŃĐŸĐČĐ°ĐœĐœĐŸĐč ĐžĐœŃĐ”ĐșŃОО, ĐČ Ń.Ń. 4 282 ŃĐ»ŃŃĐ°Ń ĐżĐŸŃлД ŃĐœĐŽĐŸĐżŃĐŸŃДзОŃĐŸĐČĐ°ĐœĐžŃ ĐșĐŸĐ»Đ”ĐœĐœĐŸĐłĐŸ Đž ŃĐ°Đ·ĐŸĐ±Đ”ĐŽŃĐ”ĐœĐœĐŸĐłĐŸ ŃŃŃŃĐ°ĐČĐŸĐČ, ŃŃĐŸ ŃĐŸŃŃĐ°ĐČĐ»ŃĐ”Ń 2,91% ĐŸŃ ĐżĐ”ŃĐČĐžŃĐœŃŃ
ŃĐœĐŽĐŸĐżŃĐŸŃДзОŃĐŸĐČĐ°ĐœĐžĐč. ĐĐ°ĐșĐ»ŃŃĐ”ĐœĐžĐ”. ЧаŃŃĐŸŃĐ° ĐĐĐ ĐČ Đ Đ€ ĐșĐŸŃŃДлОŃŃĐ”Ń Ń ĐŒĐžŃĐŸĐČŃĐŒĐž ĐŽĐ°ĐœĐœŃĐŒĐž. ĐŃŃĐČĐ»Đ”ĐœĐ° ĐČŃŃĐŸĐșĐ°Ń ŃĐ»ĐŸĐ¶ĐœĐŸŃŃŃ ĐŒĐ°ŃŃŃŃŃОзаŃОО паŃĐžĐ”ĐœŃĐŸĐČ Ń ĐžĐŒĐżĐ»Đ°ĐœŃĐ°Ń-Đ°ŃŃĐŸŃООŃĐŸĐČĐ°ĐœĐœĐŸĐč ĐžĐœŃĐ”ĐșŃОДĐč Đž ŃŃĐŸĐčĐșĐ°Ń ĐœĐ”ĐŸĐ±Ń
ĐŸĐŽĐžĐŒĐŸŃŃŃ ĐČ ŃĐŸĐ·ĐŽĐ°ĐœĐžĐž ŃДЎДŃĐ°Đ»ŃĐœĐŸĐłĐŸ ŃĐ”ĐœŃŃĐ° ĐżĐŸ лДŃĐ”ĐœĐžŃ ĐžĐŒĐżĐ»Đ°ĐœŃĐ°Ń-Đ°ŃŃĐŸŃООŃĐŸĐČĐ°ĐœĐœĐŸĐč ĐŸŃŃĐŸĐżĐ”ĐŽĐžŃĐ”ŃĐșĐŸĐč ĐžĐœŃĐ”ĐșŃОО
Low-energy dynamics of the reaction
We calculate the one-quark-loop amplitude for the low energy
collision in the context of the Nambu and Jona-Lasinio
model with scalar and pseudoscalar four quark couplings to all orders in the
external momenta. We show that the NJL predictions for the
reaction are not far from the Born amplitude, which
is close to the data, and is compatible with the chiral perturbation theory
estimations. We determine the corrections given by the NJL model in leading
order of to the chiral loop amplitude for .
Numerical results for the cross sections and
for pion polarizabilities are given.Comment: 20 pages in LaTex, 3 figures in 1 Postscript fil
Cosmic ray tests of the D0 preshower detector
The D0 preshower detector consists of scintillator strips with embedded
wavelength-shifting fibers, and a readout using Visible Light Photon Counters.
The response to minimum ionizing particles has been tested with cosmic ray
muons. We report results on the gain calibration and light-yield distributions.
The spatial resolution is investigated taking into account the light sharing
between strips, the effects of multiple scattering and various systematic
uncertainties. The detection efficiency and noise contamination are also
investigated.Comment: 27 pages, 24 figures, submitted to NIM
The COMPASS Experiment at CERN
The COMPASS experiment makes use of the CERN SPS high-intensitymuon and
hadron beams for the investigation of the nucleon spin structure and the
spectroscopy of hadrons. One or more outgoing particles are detected in
coincidence with the incoming muon or hadron. A large polarized target inside a
superconducting solenoid is used for the measurements with the muon beam.
Outgoing particles are detected by a two-stage, large angle and large momentum
range spectrometer. The setup is built using several types of tracking
detectors, according to the expected incident rate, required space resolution
and the solid angle to be covered. Particle identification is achieved using a
RICH counter and both hadron and electromagnetic calorimeters. The setup has
been successfully operated from 2002 onwards using a muon beam. Data with a
hadron beam were also collected in 2004. This article describes the main
features and performances of the spectrometer in 2004; a short summary of the
2006 upgrade is also given.Comment: 84 papes, 74 figure
Measurement of (anti)deuteron and (anti)proton production in DIS at HERA
The first observation of (anti)deuterons in deep inelastic scattering at HERA
has been made with the ZEUS detector at a centre-of-mass energy of 300--318 GeV
using an integrated luminosity of 120 pb-1. The measurement was performed in
the central rapidity region for transverse momentum per unit of mass in the
range 0.3<p_T/M<0.7. The particle rates have been extracted and interpreted in
terms of the coalescence model. The (anti)deuteron production yield is smaller
than the (anti)proton yield by approximately three orders of magnitude,
consistent with the world measurements.Comment: 26 pages, 9 figures, 5 tables, submitted to Nucl. Phys.
Measurement of the top-quark mass using a leptonic invariant mass in pp collisions at sâ = 13 TeV with the ATLAS detector
A measurement of the top-quark mass (mt) in the ttÂŻ
â lepton + jets channel is presented, with an experimental technique which exploits semileptonic decays of b-hadrons produced in the top-quark decay chain. The distribution of the invariant mass mâÎŒ of the lepton, â (with â = e, ÎŒ), from the W-boson decay and the muon, ÎŒ, originating from the b-hadron decay is reconstructed, and a binned-template profile likelihood fit is performed to extract mt. The measurement is based on data corresponding to an integrated luminosity of 36.1 fbâ1 of sâ
= 13 TeV pp collisions provided by the Large Hadron Collider and recorded by the ATLAS detector. The measured value of the top-quark mass is mt = 174.41 ± 0.39 (stat.) ± 0.66 (syst.) ± 0.25 (recoil) GeV, where the third uncertainty arises from changing the PYTHIA8 parton shower gluon-recoil scheme, used in top-quark decays, to a recently developed setup
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