scholarly journals $$K^{*}(892)^0$$ meson production in inelastic p+p interactions at 158 $$\text{ Ge }\text{ V }\!/\!c$$ beam momentum measured by NA61/SHINEat the CERN SPS

2020 ◽  
Vol 80 (5) ◽  
Author(s):  
A. Aduszkiewicz ◽  
◽  
E. V. Andronov ◽  
T. Antićić ◽  
V. Babkin ◽  
...  
2009 ◽  
Vol 24 (02n03) ◽  
pp. 484-487
Author(s):  
◽  
QUIRIN WEITZEL

Diffractive dissociation reactions at COMPASS provide clean access to mesons with masses below ≈ 2.5 GeV /c2. This paper presents a partial wave analysis of about 420 000 π- Pb → π-π-π+ Pb events at 190 GeV/c beam momentum and with four-momentum transfer t' ∈ [0.1,1] GeV 2/c2. The well-known a1(1260), a2(1320) and π2(1670) mesons are resolved with high quality. Also the less established states π(1800) and a4(2040) are seen. In addition, a resonance in the spin-exotic JPC = 1-+ wave is observed. A mass-dependent fit results in a mass and width of [Formula: see text] and [Formula: see text], respectively, which is consistent with the disputed hybrid candidate π1(1600).


Author(s):  
C.J. Rossouw ◽  
L.J. Allen ◽  
P.R. Miller

An Einstein model for thermal diffuse scattering (TDS) has enabled quantitative calculation of the absorptive potential V'(r). This allows anomalous absorption to be accounted for in LACBED contrast. Fourier coefficients Vg-h of the absorptive component from each atom α are calculated from integrals of the formwhere fα is the scattering amplitude and M(Q) the Debye-Waller factor. Integration over the Ewald sphere (dΩ) requires the momentum transfer q to have values up to 2ko (the incident beam momentum). Dynamical ‘dechannelling’ is accounted for by the terms g ≠ h. The crystal absorptive potential is obtained by coherently summing over these atomic absorptive potentials within the unit cell. Unlike the elastic potential, the absorptive potential is a strong function of incident beam energy Eo, since the range of momentum transfer q and associated solid angles dΩ change with the Ewald sphere radius.Fig. 1 shows a LACBED pattern of the zeroth order beam from Si aligned along a <001> zone axis.


1974 ◽  
Author(s):  
A. Levy ◽  
D. Brick ◽  
M. Hodous ◽  
R. Hulsizer ◽  
V. Kistiakowsky ◽  
...  

2012 ◽  
Vol 349 ◽  
pp. 011001
Author(s):  
Giorgio Giardina ◽  
Fabio Bossi ◽  
Paolo Levi Sandri ◽  
Paolo Pedroni ◽  
Hartmut Schmieden

Particles ◽  
2021 ◽  
Vol 4 (3) ◽  
pp. 354-360
Author(s):  
Oleg Golosov ◽  
Ilya Selyuzhenkov ◽  
Evgeny Kashirin

The Compressed Baryonic Matter experiment (CBM) at FAIR aims to study the area of the QCD phase diagram at high net baryon densities and moderate temperatures with collisions of heavy ions at sNN=2.8–4.9 GeV. The anisotropic transverse flow is one of the most important observable phenomena in a study of the properties of matter created in such collisions. Flow measurements require the knowledge of the collision symmetry plane, which can be determined from the deflection of the collision spectators in the plane transverse to the direction of the moving ions. The CBM performance for projectile spectator symmetry plane estimation is studied with GEANT4 Monte Carlo simulations using collisions of gold ions with beam momentum of 12A GeV/c generated with the DCM-QGSM-SMM model. Different data-driven methods to extract the correction factor in flow analysis for the resolution of the spectator symmetry plane estimated with the CBM Projectile Spectator Detector are investigated.


2021 ◽  
Vol 104 (1) ◽  
Author(s):  
Marat Siddikov ◽  
Iván Schmidt
Keyword(s):  

2021 ◽  
Vol 2021 (3) ◽  
Author(s):  
Wen Qin ◽  
Ling-Yun Dai ◽  
Jorge Portolés

Abstract A coherent study of e+e− annihilation into two (π+π−, K+K−) and three (π+π−π0, π+π−η) pseudoscalar meson production is carried out within the framework of resonance chiral theory in energy region E ≲ 2 GeV. The work of [L.Y. Dai, J. Portolés, and O. Shekhovtsova, Phys. Rev. D88 (2013) 056001] is revisited with the latest experimental data and a joint analysis of two pseudoscalar meson production. Hence, we evaluate the lowest order hadronic vacuum polarization contributions of those two and three pseudoscalar processes to the anomalous magnetic moment of the muon. We also estimate some higher-order additions led by the same hadronic vacuum polarization. Combined with the other contributions from the standard model, the theoretical prediction differs still by (21.6 ± 7.4) × 10−10 (2.9σ) from the experimental value.


1989 ◽  
Author(s):  
V. D. Apokin ◽  
O. V. Astafiev ◽  
Yu. Sh. Bagaturia ◽  
N. I. Belikov ◽  
N. S. Borisov ◽  
...  

Author(s):  
G. C. Spalding ◽  
P. Dahl ◽  
Z. Yang ◽  
C. Démoré ◽  
A. Volovick ◽  
...  

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