scholarly journals Gluon polarization in $e^+e^-\rightarrow t\bar tG$ : polar angle dependence and beam polarization effects

1999 ◽  
Vol 7 (1) ◽  
pp. 49-59 ◽  
Author(s):  
S. Groote ◽  
J.G. Körner ◽  
J.A. Leyva
1974 ◽  
Vol 11 (3) ◽  
pp. 248-248
Author(s):  
D. R. Botteril ◽  
D. W. Braben ◽  
P. R. Norton ◽  
A. Del Guerra ◽  
A. Giazotto ◽  
...  

Author(s):  
Nhi M. U. Quach ◽  
Yoshimasa Kurihara ◽  
Khiem H. Phan ◽  
Takahiro Ueda

1974 ◽  
Vol 10 (14) ◽  
pp. 629-632 ◽  
Author(s):  
D. R. Botterill ◽  
D. W. Braben ◽  
P. R. Norton ◽  
A. Del Guerra ◽  
A. Giazotto ◽  
...  

2016 ◽  
Vol 40 ◽  
pp. 1660024
Author(s):  
Christopher J. Dilks

Longitudinally polarized [Formula: see text] scattering experiments provide access to gluon polarization via measurement of the double helicity asymmetry, [Formula: see text]. At the completion of the 2013 RHIC running period, a significant dataset of [Formula: see text]s corresponding to an integrated luminosity of 46 [Formula: see text] (2012) and 8 [Formula: see text] (2013) produced from polarized [Formula: see text] scattering at [Formula: see text] GeV with an average beam polarization of approximately [Formula: see text] was acquired. The [Formula: see text] kinematics were measured via isolation cones by the STAR Forward Meson Spectrometer, an electromagnetic calorimeter covering a forward pseudorapidity range of [Formula: see text]. The asymmetric [Formula: see text] subprocess becomes more dominant in this forward region than in the midrapidity region; furthermore, asymmetry measurements in the forward region are sensitive to low-[Formula: see text] gluons. Progress on [Formula: see text] determined from forward [Formula: see text] events, complementing previous midrapidity measurements, are presented.


2020 ◽  
Vol 30 (2) ◽  
pp. 171
Author(s):  
Hong Khiem Phan ◽  
Anh Thu Nguyen ◽  
Huu Nghia Nguyen

We calculate full \(\mathcal{O}(\alpha)\) electroweak radiative corrections and \(\mathcal{O}(\alpha^3)\) initial state radiation (ISR) corrections to \(e^-e^+ \rightarrow W^-W^+\) with initial beam polarization effects. In phenomenological results, we study the impact of electroweak and ISR corrections on cross-sections as well as their relevant distributions. We find that the corrections are order of 10% contributions. They are sizable contributions and should be taken into account at future lepton colliders.


2001 ◽  
Vol 50 (6) ◽  
pp. 405-410
Author(s):  
Singo HARADA ◽  
Takashi SUZUKI ◽  
Tethuro SUGIMURA ◽  
Jun KAWAI ◽  
Shinji OMORI ◽  
...  

1998 ◽  
Vol 5 (4) ◽  
pp. 1235-1239 ◽  
Author(s):  
D. Laundy ◽  
S. Brown ◽  
M. J. Cooper ◽  
D. Bowyer ◽  
P. Thompson ◽  
...  

The ratio of the magnetic to the charge form factors of nickel has been determined by white-beam X-ray diffraction. The measurements were made on the new UK magnetic scattering beamline (XMaS) on a dipole source at the ESRF. The data comprise the three (h,h,0) reflections (4,4,0), (6,6,0) and (8,8,0) and the seven high-order (h,0,0) reflections (6,0,0) to (18,0,0), which doubles the range of wavevectors compared to previous studies. The data have been analysed using Hartree–Fock free-ion wave functions and core electron polarization effects were included. The results support the interpretation of neutron data obtained at lower momentum transfer for the e g and t 2g orbital occupancies. The polarization of the dipole source is deduced to vary from 99.88 to 99.83% between 5 and 15 keV, respectively. This high value makes it an extremely suitable source for studies of ferromagnetism.


2003 ◽  
Vol 18 (16) ◽  
pp. 2807-2815
Author(s):  
V. A. Mossolov ◽  
N. M. Shumeiko ◽  
J. G. Suarez

Polarization effects including radiative corrections have been considered. Exact lowest-order covariant calculation of QED RC has been carried out and detailed numerical analysis is given. The hard photon contribution is calculated analytically. Exponentation procedure is used to consider multi-soft-photon contribution. Numerical analysis is perfomed for beam polarization measurements at Møller polarimeter.


2016 ◽  
Vol 139 (2) ◽  
Author(s):  
Robert A. Carson ◽  
Onkar Sahni

For large cannons, blast overpressure can have a detrimental effect on the crew in the near field (i.e., within a distance of 50 tube diameters or calibers from the muzzle center) as well as on the support personnel and equipment in the far field (i.e., at a distance greater than 50 calibers). Therefore, an efficient method to determine the peak overpressure due to a cannon blast is highly desired. In this study, we investigate scaling laws for the peak overpressure, due to the primary blast of a large cannon, with the aim that they can be applied as an efficient method to evaluate the peak overpressure in the far field. We explore two types of scaling laws; each type is based on a power-law model involving a prefactor and an exponent as model parameters. The two types of the power-law models differ in the way they incorporate the polar angle dependence. The first type was proposed by Fansler and Schmidt (1983, “The Prediction of Gun Muzzle Blast Properties Utilizing Scaling,” U.S. Army Ballistic Research Laboratory, Aberdeen Proving Ground, MD, Report No. ARBRL-TR-02504). They developed a muzzle-center based scaling law (MCSL) in which the polar angle dependence was incorporated through a reference length scale to define a nondimensional or scaled radial distance from the muzzle center and the model parameters were independent of the polar angle. They calibrated the parameters by employing least-squares fit to a wide range of experimental data. In this study, we recalibrated or updated the parameters for the current cannon by using the numerical simulation data for the cannon blast in the near field. Additionally, we developed a second type of scaling law in which the radial distance is defined from the blast center (in contrast to the muzzle center) and scaled using the inner tube diameter. In this model, the angular dependence is incorporated directly into the model parameters. For this model too, we calibrated the parameters by using the numerical simulation data. We observe that both the modified version of the muzzle-center based scaling law as well as the blast-center based scaling law (BCSL) show a significantly closer fit to the numerical and experimental data and achieve a similar level of accuracy. This indicates that the current form or structure of the two types of power-law based scaling models is able to fit well with the near-field data; however, the current methodology requires a calibration process for a given cannon of interest. In the future, with far field data, we plan to evaluate predictions in the far field.


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