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Analytic formulae for the one-loop order QCD corrections to the differential width of the semileptonic b decay are given with the tau polarization taken into account. Thence the polarization of tau is expressed by its energy and the…

High Energy Physics - Phenomenology · Physics 2009-10-30 M. Jezabek , P. Urban

The radiative decay $ B_{q}^*\to B_{q}\gamma(q=u,d, or s) $ is reexamined with a modified light-cone QCD sum rule method, in which adequate chiral operators are chosen as the interpolating fields in the correlators used for a sum rule…

High Energy Physics - Phenomenology · Physics 2007-05-23 Zuo-Hong Li , Xiang-Yao Wu , Tao Huang

In this note radiative corrections to the total hadronic decay rate of the $\tau$-lepton are studied employing perturbative QCD and the operator product expansion. We calculate quadratic quark mass corrections to the decay rate ration…

High Energy Physics - Phenomenology · Physics 2015-06-25 K. G. Chetyrkin , A. Kwiatkowski

In this paper, we generally analyze the $\mu - \tau$ reflection symmetry modified by small mixings of charged leptons and how will future experiments verify deviations from the predictions of the symmetry. As an approximation, the…

High Energy Physics - Phenomenology · Physics 2025-09-03 Masaki J. S. Yang

We calculate the self-energy and the vertex radiative corrections to the effect of parity nonconservation in heavy atoms. The sum of the corrections is of the form ${\cal A}\ln(\lambda_C/r_0)+{\calB}$, where ${\cal A}$ and ${\cal B}$ are…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. I. Milstein , O. P. Sushkov , I. S. Terekhov

We briefly sketch the methods for a numerically stable evaluation of tensor one-loop integrals that have been used in the calculation of the complete electroweak one-loop corrections to $\Pep\Pem\to4 $fermions. In particular, the…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Denner , S. Dittmaier

We report the measurement of the ratio $\Gamma(\eta \to \pi^+\pi^-\gamma)/\Gamma(\eta \to \pi^+\pi^-\pi^0)$ analyzing a large sample of $\phi \to \eta \gamma$ decays recorded with the KLOE experiment at the DA$\Phi$NE $e^+ e^-$ collider,…

We point out that dynamics known from the observed CP violation in $K_L\to \pi^{\mp}l^{\pm}\nu$ generate a CP asymmetry of $3.3\cdot 10^{-3}$ in $\tau^{\pm} \to \nu K_L\pi^{\pm}$. CPT invariance requires the same asymmetry in the more…

High Energy Physics - Phenomenology · Physics 2010-04-05 I. I. Bigi , A. I. Sanda

We present the detailed analytical and numerical investigations of the one-loop radiative corrections of all quarks and squarks in the MSSM to the lightest chargino pair production via $\gamma \gamma$ fusion at the future NLC. The numerical…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhou Mian-Lai , Ma Wen-Gan , Han Liang , Jiang Yi , Zhou Hong

A self-consistent version of the left-right (LR) symmetric model is used to examine tree- as well as one-loop level radiative corrections to the muon decay. It is shown that constraints on the heavy sector of the model parameters are…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. Czakon , J. Gluza , J. Hejczyk

We review the physics of polarization observables in high energy reactions in general and discuss the status of \NLO one--loop corrections to these observables in specific. Many high order radiative corrections exists for rates but not many…

High Energy Physics - Phenomenology · Physics 2017-08-23 J. G. Körner , M. C. Mauser

The four-loop determination of the strong coupling from fully inclusive observables is reviewed. Special attention is given to the low-energy measurement extracted from the hadronic $\tau$ decay width. A recent exhaustive analysis of the…

High Energy Physics - Phenomenology · Physics 2017-04-05 Antonio Pich

We report the first measurement of the $\tau$ lepton polarization in the decay ${\bar B} \rightarrow D^* \tau^- {\bar\nu_{\tau}}$ as well as a new measurement of the ratio of the branching fractions $R(D^{*}) = \mathcal{B}({\bar B}…

High Energy Physics - Experiment · Physics 2016-08-24 A. Abdesselam , I. Adachi , K. Adamczyk , H. Aihara , S. Al Said , K. Arinstein , Y. Arita , D. M. Asner , T. Aso , H. Atmacan , V. Aulchenko , T. Aushev , R. Ayad , T. Aziz , V. Babu , I. Badhrees , S. Bahinipati , A. M. Bakich , A. Bala , Y. Ban , V. Bansal , E. Barberio , M. Barrett , W. Bartel , A. Bay , I. Bedny , P. Behera , M. Belhorn , K. Belous , M. Berger , D. Besson , V. Bhardwaj , B. Bhuyan , J. Biswal , T. Bloomfield , S. Blyth , A. Bobrov , A. Bondar , G. Bonvicini , C. Bookwalter , C. Boulahouache , A. Bozek , M. Bračko , F. Breibeck , J. Brodzicka , T. E. Browder , E. Waheed , D. Červenkov , M. -C. Chang , P. Chang , Y. Chao , V. Chekelian , A. Chen , K. -F. Chen , P. Chen , B. G. Cheon , K. Chilikin , R. Chistov , K. Cho , V. Chobanova , S. -K. Choi , Y. Choi , D. Cinabro , J. Crnkovic , J. Dalseno , M. Danilov , N. Dash , S. Di Carlo , J. Dingfelder , Z. Doležal , D. Dossett , Z. Drásal , A. Drutskoy , S. Dubey , D. Dutta , K. Dutta , S. Eidelman , D. Epifanov , S. Esen , H. Farhat , J. E. Fast , M. Feindt , T. Ferber , A. Frey , O. Frost , B. G. Fulsom , V. Gaur , N. Gabyshev , S. Ganguly , A. Garmash , D. Getzkow , R. Gillard , F. Giordano , R. Glattauer , Y. M. Goh , P. Goldenzweig , B. Golob , D. Greenwald , M. Grosse Perdekamp , J. Grygier , O. Grzymkowska , H. Guo , J. Haba , P. Hamer , Y. L. Han , K. Hara , T. Hara , Y. Hasegawa , J. Hasenbusch , K. Hayasaka , H. Hayashii , X. H. He , M. Heck , M. T. Hedges , D. Heffernan , M. Heider , A. Heller , T. Higuchi , S. Himori , S. Hirose , T. Horiguchi , Y. Hoshi , K. Hoshina , W. -S. Hou , Y. B. Hsiung , C. -L. Hsu , M. Huschle , H. J. Hyun , Y. Igarashi , T. Iijima , M. Imamura , K. Inami , G. Inguglia , A. Ishikawa , K. Itagaki , R. Itoh , M. Iwabuchi , M. Iwasaki , Y. Iwasaki , S. Iwata , W. W. Jacobs , I. Jaegle , H. B. Jeon , Y. Jin , D. Joffe , M. Jones , K. K. Joo , T. Julius , H. Kakuno , A. B. Kaliyar , J. H. Kang , K. H. Kang , P. Kapusta , S. U. Kataoka , E. Kato , Y. Kato , P. Katrenko , H. Kawai , T. Kawasaki , T. Keck , H. Kichimi , C. Kiesling , B. H. Kim , D. Y. Kim , H. J. Kim , H. -J. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , S. H. Kim , S. K. Kim , Y. J. Kim , K. Kinoshita , C. Kleinwort , J. Klucar , B. R. Ko , N. Kobayashi , S. Koblitz , P. Kodyš , Y. Koga , S. Korpar , D. Kotchetkov , R. T. Kouzes , P. Križan , P. Krokovny , B. Kronenbitter , T. Kuhr , R. Kulasiri , R. Kumar , T. Kumita , E. Kurihara , Y. Kuroki , A. Kuzmin , P. Kvasnička , Y. -J. Kwon , Y. -T. Lai , J. S. Lange , D. H. Lee , I. S. Lee , S. -H. Lee , M. Leitgab , R. Leitner , D. Levit , P. Lewis , C. H. Li , H. Li , J. Li , L. Li , X. Li , Y. Li , L. Li Gioi , J. Libby , A. Limosani , C. Liu , Y. Liu , Z. Q. Liu , D. Liventsev , A. Loos , R. Louvot , M. Lubej , P. Lukin , T. Luo , J. MacNaughton , M. Masuda , T. Matsuda , D. Matvienko , A. Matyja , S. McOnie , Y. Mikami , K. Miyabayashi , Y. Miyachi , H. Miyake , H. Miyata , Y. Miyazaki , R. Mizuk , G. B. Mohanty , S. Mohanty , D. Mohapatra , A. Moll , H. K. Moon , T. Mori , T. Morii , H. -G. Moser , T. Müller , N. Muramatsu , R. Mussa , T. Nagamine , Y. Nagasaka , Y. Nakahama , I. Nakamura , K. R. Nakamura , E. Nakano , H. Nakano , T. Nakano , M. Nakao , H. Nakayama , H. Nakazawa , T. Nanut , K. J. Nath , Z. Natkaniec , M. Nayak , E. Nedelkovska , K. Negishi , K. Neichi , C. Ng , C. Niebuhr , M. Niiyama , N. K. Nisar , S. Nishida , K. Nishimura , O. Nitoh , T. Nozaki , A. Ogawa , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , Y. Ono , Y. Onuki , W. Ostrowicz , C. Oswald , H. Ozaki , P. Pakhlov , G. Pakhlova , B. Pal , H. Palka , E. Panzenböck , C. -S. Park , C. W. Park , H. Park , K. S. Park , S. Paul , L. S. Peak , T. K. Pedlar , T. Peng , L. Pesántez , R. Pestotnik , M. Peters , M. Petrič , L. E. Piilonen , A. Poluektov , K. Prasanth , M. Prim , K. Prothmann , C. Pulvermacher , M. V. Purohit , J. Rauch , B. Reisert , E. Ribežl , M. Ritter , J. Rorie , A. Rostomyan , M. Rozanska , S. Rummel , S. Ryu , H. Sahoo , T. Saito , K. Sakai , Y. Sakai , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , J. Sasaki , N. Sasao , Y. Sato , V. Savinov , T. Schlüter , O. Schneider , G. Schnell , P. Schönmeier , M. Schram , C. Schwanda , A. J. Schwartz , B. Schwenker , R. Seidl , Y. Seino , D. Semmler , K. Senyo , O. Seon , I. S. Seong , M. E. Sevior , L. Shang , M. Shapkin , V. Shebalin , C. P. Shen , T. -A. Shibata , H. Shibuya , N. Shimizu , S. Shinomiya , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , R. Sinha , P. Smerkol , Y. -S. Sohn , A. Sokolov , Y. Soloviev , E. Solovieva , S. Stanič , M. Starič , M. Steder , J. F. Strube , J. Stypula , S. Sugihara , A. Sugiyama , M. Sumihama , K. Sumisawa , T. Sumiyoshi , K. Suzuki , K. Suzuki , S. Suzuki , S. Y. Suzuki , Z. Suzuki , H. Takeichi , M. Takizawa , U. Tamponi , M. Tanaka , S. Tanaka , K. Tanida , N. Taniguchi , G. N. Taylor , F. Tenchini , Y. Teramoto , I. Tikhomirov , K. Trabelsi , V. Trusov , Y. F. Tse , T. Tsuboyama , M. Uchida , T. Uchida , S. Uehara , K. Ueno , T. Uglov , Y. Unno , S. Uno , S. Uozumi , P. Urquijo , Y. Ushiroda , Y. Usov , S. E. Vahsen , C. Van Hulse , P. Vanhoefer , G. Varner , K. E. Varvell , K. Vervink , A. Vinokurova , V. Vorobyev , A. Vossen , M. N. Wagner , E. Waheed , C. H. Wang , J. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , R. Wedd , S. Wehle , E. White , E. Widmann , J. Wiechczynski , K. M. Williams , E. Won , B. D. Yabsley , S. Yamada , H. Yamamoto , J. Yamaoka , Y. Yamashita , M. Yamauchi , S. Yashchenko , H. Ye , J. Yelton , Y. Yook , C. Z. Yuan , Y. Yusa , C. C. Zhang , L. M. Zhang , Z. P. Zhang , L. Zhao , V. Zhilich , V. Zhukova , V. Zhulanov , M. Ziegler , T. Zivko , A. Zupanc , N. Zwahlen , O. Zyukova

General O(alpha) radiative corrections to lattice actions may be interpreted as counterterms that give additive contributions to the one-loop renormalisation of the anisotropy. The effect of changing the radiative coefficients is thus…

High Energy Physics - Lattice · Physics 2014-11-17 I. T. Drummond , A. Hart , R. R. Horgan , L. C. Storoni

Using a diagrammatic approach to Eulerian perturbation theory, we analytically calculate the variance and skewness of the density and velocity divergence induced by gravitational evolution from Gaussian initial conditions, including…

Astrophysics · Physics 2011-09-30 Roman Scoccimarro , Joshua Frieman

We point out that a simple test of the mechanism of CP violation can be performed by a measurement of the CP asymmetries in exclusive and inclusive radiative rare decays. We show that the rate asymmetries $\Delta \Gamma = \Gamma(B^- \to f…

High Energy Physics - Phenomenology · Physics 2014-11-17 Tobias Hurth , Thomas Mannel

This PhD thesis is a first step towards the control of the quantum corrections in the Resonance Chiral Theory, the suggested framework to handle QCD in the resonance region. After a theoretical introduction, Chapter 3 is devoted to…

High Energy Physics - Phenomenology · Physics 2007-05-23 I. Rosell

The QED radiative corrections to virtual Compton scattering (reaction $e p \to e p \gamma$) are calculated to first order in $\alpha_{em} \equiv e^2 / 4 \pi$. A detailed study is presented for the one-loop virtual corrections and for the…

High Energy Physics - Phenomenology · Physics 2016-09-06 M. Vanderhaeghen , J. M. Friedrich , D. Lhuillier , D. Marchand , L. Van Hoorebeke , J. Van de Wiele

Within an effective field theory framework we compute the most general structure of the one-loop corrections to the 4D gauge couplings in one- and two-dimensional orbifold compactifications with non-vanishing constant gauge background…

High Energy Physics - Theory · Physics 2014-11-18 D. M. Ghilencea

The hadronization structure of $\tau^- \to \eta \pi^- \pi^0 \nu_\tau$ decays is analyzed using Chiral Perturbation Theory with resonances, considering only the contribution of the lightest meson resonances at leading order in the $1/N_C$…

High Energy Physics - Phenomenology · Physics 2013-05-30 Daniel Gómez Dumm , Pablo Roig