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相关论文: Revisiting the $O(\alpha^2)$ Initial State QED Cor…

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We calculate the complete electroweak O(alpha) corrections to pp, pbar p -> l+l- X (l=e, mu) in the Standard Model of electroweak interactions. They comprise weak and photonic virtual one-loop corrections as well as real photon radiation to…

高能物理 - 唯象学 · 物理学 2010-04-06 U. Baur , O. Brein , W. Hollik , C. Schappacher , D. Wackeroth

Calculations of radiative corrections to the top quark width are reviewed. QCD effects are discussed for $t-\bar t$ systems produced in $e^+e^-$ annihilation near the energy threshold.}

高能物理 - 唯象学 · 物理学 2007-05-23 Marek Jeżabek , Johann H. Kühn , Thomas Teubner

We investigate the radiative quantum electrodynamic (QED) corrections to the lepton ($L=e, ~\mu $ and $\tau$) anomalous magnetic moment due to the contributions of diagrams with insertions of the photon vacuum polarisation operator…

高能物理 - 唯象学 · 物理学 2023-10-19 O. P. Solovtsova , V. I. Lashkevich , L. P. Kaptari

More than ten years ago a first step towards quantum error correction (QEC) was implemented [Phys. Rev. Lett. 81, 2152 (1998)]. The work showed there was sufficient control in nuclear magnetic resonance (NMR) to implement QEC, and…

量子物理 · 物理学 2011-09-23 Jingfu Zhang , Dorian Gangloff , Osama Moussa , Raymond Laflamme

Bound-muon decays are a powerful probe of new physics, making precise theoretical predictions for their spectra essential. While QED corrections significantly affect the shape of the spectra, their calculation is extremely challenging below…

高能物理 - 唯象学 · 物理学 2025-10-31 Duarte Fontes , Robert Szafron

We estimate the non-perturbative power-suppressed corrections to heavy flavour fragmentation and correlation functions in e^+e^- annihilation, using a model based on the analysis of one-loop Feynman graphs containing a massive gluon. This…

高能物理 - 唯象学 · 物理学 2009-10-30 P. Nason , B. R. Webber

We calculate the QCD radiative corrections to the production of supersymmetric scalar partners of quarks in e+e- annihilation. We include both the standard gluonic corrections and the genuine supersymmetric QCD corrections due to…

高能物理 - 唯象学 · 物理学 2009-10-28 A. Arhrib , M. Capdequi-Peyranere , A. Djouadi

We investigate the quantum chromodynamics (QCD) corrections to hadronic final states in electron-positron collisions at $\mathcal{O}(\alpha_s^3)$ in the strong coupling constant $\alpha_s$. Namely, we analytically compute the total cross…

高能物理 - 唯象学 · 物理学 2023-04-24 Petr Jakubčík , Matteo Marcoli , Giovanni Stagnitto

We compute the dominant QED correction to the neutrino-electron interaction rate in the vicinity of neutrino decoupling in the early universe, and estimate its impact on the effective number of neutrino species $N_{\rm eff}$ in cosmic…

高能物理 - 唯象学 · 物理学 2024-06-17 Marco Drewes , Yannis Georis , Michael Klasen , Luca Paolo Wiggering , Yvonne Y. Y. Wong

The production of W+ W- b bbar from e+ e- collisions at energies close to the t tbar threshold is dominated by the resonant process with a nearly on-shell t tbar intermediate state. The W b pairs in the final state can also be reached…

高能物理 - 唯象学 · 物理学 2022-09-21 M. Beneke , B. Jantzen , P. Ruiz-Femenia

Accurate results for nonrelativistic energy, relativistic, QED, and finite nuclear mass corrections are obtained for $2^1S_{1/2}$, $3^1S_{1/2}$ and $2^1P_{1/2}$ states of the Li atom and Be$^+$ ion. Our computational approach uses the…

原子物理 · 物理学 2009-11-13 Mariusz Puchalski , Krzysztof Pachucki

The quantum phase estimation algorithm stands as the primary method for determining the ground state energy of a molecular electronic Hamiltonian on a quantum computer. In this context, the ability to initialize a classically tractable…

It is shown that amplitude-based, exact resummation tames the un-cancelled IR divergences at O(alpha_s^2) in initial state radiation in QCD with massive quarks. Implications for precision predictions for LHC physics are discussed.

高能物理 - 唯象学 · 物理学 2008-11-07 B. F. L. Ward

We present the first complete $\mathcal{O}(\alpha_s^2)$ and $\mathcal{O}(\alpha_s^3)$ perturbative QCD corrections to all five heavy-to-light structure functions underlying the triple-differential semi-leptonic decay rates of heavy quarks.…

高能物理 - 唯象学 · 物理学 2026-02-13 Long Chen , Xiang Chen , Xin Guan , Yan-Qing Ma

Next-to-Leading-Order(NLO) QCD corrections to J/jpsi plus eta_c production in e+e- annihilation at sqrt{s}=10.6 GeV is calculated in this paper, and an analytic result is obtained. By choosing proper physical parameters, a K factor (ratio…

高能物理 - 唯象学 · 物理学 2008-11-26 Bin Gong , Jian-Xiong Wang

We provide analytical results for the $O(\alpha_s)$ corrections to the polar angle dependence of the longitudinal spin-spin correlation asymmetry in $e^+e^-\to q\bar q$. For top quark pair production the $O(\alpha_s)$ corrections to the…

高能物理 - 唯象学 · 物理学 2014-03-13 S. Groote , J. G. Körner , J. A. Leyva

We derive the initial condition for the perturbative fragmentation function of a heavy quark through order O(alpha_s^2) in the MS-bar scheme. This initial condition is useful for computing heavy quark (or lepton, in case of QED) energy…

高能物理 - 唯象学 · 物理学 2014-11-17 Kirill Melnikov , Alexander Mitov

The partial decay rate $\Gamma(Z\to b\bar{b})$ is significantly influenced by the mass of the top quark due to electroweak radiative corrections. The leading $\sim m_t^2$ and the next-to-leading contribution $\sim \ln m_t^2$ are known to be…

高能物理 - 唯象学 · 物理学 2011-04-20 A. Kwiatkowski , M. Steinhauser

We provide and discuss the precision predictions for the $W^+W^-\gamma$ production at the ILC including the full electroweak (EW) one-loop corrections and high order initial state radiation (ISR) contributions in the Standard Model. The…

高能物理 - 唯象学 · 物理学 2014-12-30 Chen Chong , Ma Wen-Gan , Zhang Ren-You , Zhang Yu , Chen Liang-Wen , Guo Lei

We discuss $1/Q$ corrections to hard processes in QCD where $Q$ is a large mass parameter like the total energy in $e^+e^-$ annihilation. The main problem we address ourselves to is whether these corrections to different processes…

高能物理 - 唯象学 · 物理学 2009-10-28 R. Akhoury , V. I. Zakharov