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Vacuum polarization integrals involve the vector spectral functions which can be experimentally determined from two sources: (i) e+e- annihilation cross sections and (ii) hadronic tau decays. Recently results with comparable precision have…

High Energy Physics - Phenomenology · Physics 2015-06-25 Andreas Hocker

The angular distributions and the differential branching fraction of the decay B0 to K*(892)0 mu+ mu- are studied using a data sample corresponding to an integrated luminosity of 5.2 inverse femtobarns collected with the CMS detector at the…

High Energy Physics - Experiment · Physics 2013-11-11 CMS Collaboration

Recently, the CMS and ATLAS collaborations have announced the results for $H\rightarrow Z[\rightarrow \ell^{+}\ell^{-}]\gamma$ with $\ell=e$ or $\mu$ \cite{CMS:2022ahq,CMS:2023mku}, where $H\rightarrow Z\gamma$ is a sub-process of…

High Energy Physics - Phenomenology · Physics 2024-05-22 Ishtiaq Ahmed , Usman Hasan , Shahin Iqbal , M. Junaid , Bilal Tariq , A. Uzair

We study the decay rate and the CP violating asymmetry of the exclusive B-> pi ell+ ell- and B-> rho ell+ ell- decays in the case where one of the final leptons is polarized. We calculate the contributions coming from the individual…

High Energy Physics - Phenomenology · Physics 2011-09-13 Guray Erkol , Gursevil Turan , Jan Willem Wagenaar

We calculate the complete differential decay distributions for the $B$ meson decays, $\bar B \to D^{(*)} \ell \bar{X}$, to a massive right-handed (RH) neutrino in the low-energy effective field theory (LEFT) framework. We find that a…

High Energy Physics - Phenomenology · Physics 2023-08-17 Alakabha Datta , Hongkai Liu , Danny Marfatia

The B -> X_s l+ l- decay rate is known at the next-to-next-to-leading order in QCD. It is proportional to alpha_em (mu)^2 and has a +- 4% scale uncertainty before including the O(alpha_em log(M_W^2/m_b^2)) electromagnetic corrections. We…

High Energy Physics - Phenomenology · Physics 2011-10-13 T. Huber , E. Lunghi , M. Misiak , D. Wyler

The weak localization correction and the mesoscopic fluctuations of the polarizability and the capacitance of a small disordered sample are studied systematically in 2D and 3D geometries. While the grand canonical ensemble calculation gives…

Mesoscale and Nanoscale Physics · Physics 2009-10-30 Ya. M. Blanter , A. D. Mirlin

We investigate the production of spin-3/2 hyperon pairs, $\Omega^- \bar{\Omega}^+$, in electron-positron annihilation within the helicity amplitude formalism. A refined selection of helicity basis matrices is proposed to relate polarization…

High Energy Physics - Phenomenology · Physics 2023-12-08 Zhe Zhang , Jiao Jiao Song , Ya-jin Zhou

A rigorous light-front formalism for electron deep inelastic scattering on unpolarized nuclei, in Bjorken limit, is reported. It preserves Poincar\'e covariance, macroscopic locality, both number of particles and momentum sum rules. The…

Nuclear Theory · Physics 2023-03-22 Emanuele Pace , Matteo Rinaldi , Giovanni Salme` , Sergio Scopetta

We present the first calculation of same-sign WW scattering at the LHC in the fully leptonic decay channel including the modelling of polarisation for intermediate electroweak bosons and radiative corrections up to NLO EW+QCD accuracy. The…

High Energy Physics - Phenomenology · Physics 2024-11-13 Ansgar Denner , Christoph Haitz , Giovanni Pelliccioli

The semileptonic decay $\Lambda_c \to \Lambda \ell \nu$ is considered in the framework of heavy quark effective theory beyond the leading order in the $1/m_c$ expansion. According to our estimate the polarization variable will receive only…

High Energy Physics - Phenomenology · Physics 2009-10-22 Guey-Lin Lin , Thomas Mannel

The double-polarization observable $E$ was studied for the reaction $\gamma p\to p\omega$ using the CEBAF Large Acceptance Spectrometer (CLAS) in Hall B at the Thomas Jefferson National Accelerator Facility and the longitudinally-polarized…

Nuclear Experiment · Physics 2019-08-13 Z. Akbar , P. Roy , S. Park , V. Crede , A. V. Anisovich , I. Denisenko , E. Klempt , V. A. Nikonov , A. V. Sarantsev , K. P. Adhikari , S. Adhikari , M. J. Amaryan , S. Anefalos Pereira , H. Avakian , J. Ball , M. Battaglieri , V. Batourine , I. Bedlinskiy , S. Boiarinov , W. J. Briscoe , J. Brock , W. K. Brooks , V. D. Burkert , F. T. Cao , C. Carlin , D. S. Carman , A. Celentano , G. Charles , T. Chetry , G. Ciullo , L. Clark , P. L. Cole , M. Contalbrigo , O. Cortes , A. D'Angelo , N. Dashyan , R. De Vita , E. De Sanctis , A. Deur , C. Djalali , M. Dugger , R. Dupre , H. Egiyan , L. El Fassi , P. Eugenio , G. Fedotov , R. Fersch , A. Filippi , A. Fradi , M. Garcon , N. Gevorgyan , K. L. Giovanetti , F. X. Girod , C. Gleason , W. Gohn , E. Golovach , R. W. Gothe , K. A. Griffioen , M. Guidal , L. Guo , K. Hafidi , H. Hakobyan , C. Hanretty , N. Harrison , M. Hattawy , D. Heddle , K. Hicks , G. Hollis , M. Holtrop , D. G. Ireland , B. S. Ishkhanov , E. L. Isupov , D. Jenkins , S. Joosten , C. D. Keith , D. Keller , G. Khachatryan , M. Khachatryan , M. Khandaker , A. Kim , W. Kim , A. Klein , F. J. Klein , V. Kubarovsky , L. Lanza , K. Livingston , I. J. D. MacGregor , N. Markov , B. McKinnon , D. G. Meekins , T. Mineeva , V. Mokeev , A. Movsisyan , C. Munoz Camacho , P. Nadel-Turonski , S. Niccolai , M. Osipenko , A. I. Ostrovidov , M. Paolone , R. Paremuzyan , K. Park , E. Pasyuk , W. Phelps , O. Pogorelko , J. W. Price , Y. Prok , D. Protopopescu , B. A. Raue , M. Ripani , B. G. Ritchie , A. Rizzo , G. Rosner , F. Sabatie , C. Salgado , R. A. Schumacher , Y. G. Sharabian , Iu. Skorodumina , G. D. Smith , D. I. Sober , D. Sokhan , N. Sparveris , S. Stepanyan , I. I. Strakovsky , S. Strauch , M. Taiuti , M. Ungaro , H. Voskanyan , E. Voutier , X. Wei , M. H. Wood , N. Zachariou , L. Zana , J. Zhang , Z. W. Zhao

The classical symmetry of the source-free Maxwell equations under electric-magnetic duality rotations leads to a conserved Noether charge, corresponding to the circular polarization of light. We show that, in quantum field theory, the…

General Relativity and Quantum Cosmology · Physics 2025-05-28 Adrián del Río

Vacuum polarization integrals involve the vector spectral functions which can be experimentally determined from two sources: (i) e+e- annihilation cross sections and (ii) hadronic tau decays. Recently results with comparable precision have…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Davier , S. Eidelman , A. Hocker , Z. Zhang

The differential decay spectrum $d\Gamma/dE_e dq^2$ for the semileptonic decay of an unpolarized hadron containing a b-quark, and the decay spectrum $d\Gamma/dE_e dq^2 d\!\cos\theta$ for polarized $\Lambda_b$ decay are computed to second…

High Energy Physics - Phenomenology · Physics 2010-11-01 Aneesh V. Manohar , Mark B. Wise

We calculate QED corrections to the semileptonic decays $H_1 \to H_2\ell^+\ell^-$ where $\ell=e, \mu$ and $H_{1,2}$ are hadrons. The soft and/or collinear divergences are regulated in a gauge-invariant manner and demonstrably cancel,…

High Energy Physics - Phenomenology · Physics 2023-07-18 Debajyoti Choudhury , Diganta Das , Jaydeb Das

Radiative corrections in the order ${\alpha\over{2\pi}}{{m^2_e}\over m^2_\mu}$ to $\mu $- and ${\alpha\over{2\pi}}{{m^2_\mu}\over m^2_\tau}$ to $\tau $- decays are calculated. The decay width is enhanced by $4.48\cdot 10^{-3}…

High Energy Physics - Phenomenology · Physics 2008-02-03 V. Konyshev , I. Polyubin

We perform a systematic study on the spin decomposition of an electron in QED at one-loop order. It is found that the electron orbital angular momentum defined in Jaffe-Manohar and Ji spin sum rules agrees with each other, and the so-called…

High Energy Physics - Phenomenology · Physics 2016-03-23 Xiangdong Ji , Andreas Schäfer , Feng Yuan , Jian-Hui Zhang , Yong Zhao

A complete experiment on decay $K_L \to l^+ l^-$ will not only consist of measurement of the decay rates but also lepton polarization etc. These additional observations will yield tests of CP invariance in these decays. In $K_L$ and $K_S$…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. Rai Choudhury , Naveen Gaur , Abhinav Gupta

We show that local parity violation due to chirality imbalance in relativistic nuclear collisions can be revealed by measuring the projection of the polarization vector onto the momentum, i.e. the helicity, of final state baryons. The…

High Energy Physics - Phenomenology · Physics 2021-10-08 F. Becattini , M. Buzzegoli , A. Palermo , G. Prokhorov