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Related papers: Polarization transfer in SIDIS for Lambda producti…

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The studies of heavy quarkonium inclusive production and polarization at LHC are becoming crucial to solve the puzzle of hadron formation. The results by CMS and the other LHC experiments are compactly presented for the five S-wave states…

High Energy Physics - Experiment · Physics 2014-09-16 Alexis Pompili

We use the recombination and the Thomas Precession Model to obtain a prediction for the $\Lambda _0$ polarization in the $p+p \to \Lambda_0+X$ reaction. We study the effect of the recombination function on the $\Lambda_0$ polarization.

High Energy Physics - Phenomenology · Physics 2016-09-06 G. Herrera , J. Magnin , Luis M. Montaño , F. R. A. Simão

Based on the non-relativistic quantum chromodynamics factorization formalism, the polarization parameters $\lambda_{\theta\phi}$ and $\lambda_{\phi}$ of $J/\psi$ hadroproduction are analyzed in helicity frame and calculated at QCD…

High Energy Physics - Phenomenology · Physics 2019-02-06 Yu Feng , Bin Gong , Chao-Hsi Chang , Jian-Xiong Wang

We compute the $\Lambda$ and $\overline{\Lambda}$ global polarizations in semi-central heavy-ion collisions using the core-corona model where the source of $\Lambda$'s and $\overline{\Lambda}$'s is taken as consisting of a high-density core…

High Energy Physics - Phenomenology · Physics 2022-03-28 Alejandro Ayala , Isabel Domínguez , Ivonne Maldonado , María Elena Tejeda-Yeomans

Stimulated by the proton radius conundrum, measurements of the Lamb shift in various light muonic atoms are planned at PSI. The aim is to extract the rms charge radius with high precision, limited by the uncertainty in the nuclear…

Nuclear Theory · Physics 2013-11-06 Chen Ji , Nir Nevo Dinur , Sonia Bacca , Nir Barnea

Spin transfer in deep-inelastic Lambda electroproduction has been studied with the HERMES detector using the 27.6 GeV polarized positron beam in the HERA storage ring. For an average fractional energy transfer <z> = 0.45, the longitudinal…

High Energy Physics - Experiment · Physics 2009-04-15 HERMES Collaboration , A. Airapetian

We present new data for the polarization observables of the final state proton in the $^{1}H(\vec{\gamma},\vec{p})\pi^{0}$ reaction. These data can be used to test predictions based on hadron helicity conservation (HHC) and perturbative QCD…

Nuclear Experiment · Physics 2012-06-05 W. Luo , E. J. Brash , R. Gilman , M. K. Jones , M. Meziane , L. Pentchev , C. F. Perdrisat , A. J. R. Puckett , V. Punjabi , F. R. Wesselmann , A. Ahmidouch , I. Albayrak , K. A. Aniol , J. Arrington , A. Asaturyan , O. Ates , H. Baghdasaryan , F. Benmokhtar , W. Bertozzi , L. Bimbot , P. Bosted , W. Boeglin , C. Butuceanu , P. Carter , S. Chernenko , M. E. Christy , M. Commisso , J. C. Cornejo , S. Covrig , S. Danagoulian , A. Daniel , A. Davidenko , D. Day , S. Dhamija , D. Dutta , R. Ent , S. Frullani , H. Fenker , E. Frlez , F. Garibaldi , D. Gaskell , S. Gilad , Y. Goncharenko , K. Hafidi , D. Hamilton , D. W. Higinbotham , W. Hinton , T. Horn , B. Hu , J. Huang , G. M. Huber , E. Jensen , H. Kang , C. Keppel , M. Khandaker , P. King , D. Kirillov , M. Kohl , V. Kravtsov , G. Kumbartzki , Y. Li , V. Mamyan , D. J. Margaziotis , P. Markowitz , A. Marsh , Y. Matulenko , J. Maxwell , G. Mbianda , D. Meekins , Y. Melnik , J. Miller , A. Mkrtchyan , H. Mkrtchyan , B. Moffit , O. Moreno , J. Mulholland , A. Narayan , Nuruzzaman , S. Nedev , E. Piasetzky , W. Pierce , N. M. Piskunov , Y. Prok , R. D. Ransome , D. S. Razin , P. E. Reimer , J. Reinhold , O. Rondon , M. Shabestari , A. Shahinyan , K. Shestermanov , S. Sirca , I. Sitnik , L. Smykov , G. Smith , L. Solovyev , P. Solvignon , I. I. Strakovsky , R. Subedi , R. Suleiman , E. Tomasi-Gustafsson , A. Vasiliev , M. Veilleux , S. Wood , Z. Ye , Y. Zanevsky , X. Zhang , Y. Zhang , X. Zheng , L. Zhu

The processes $pp/ pbar p \to Z \gamma + X \to \ell^+ \ell^- \gamma + X$ ($\ell=e, \mu$) and $pp/ pbarp \to Z \gamma + X \to \bar\nu\nu\gamma + X$ are calculated to ${\cal O}(\alpha_s)$ for general $ZZ\gamma$ and $Z\gamma\gamma$ couplings.…

High Energy Physics - Phenomenology · Physics 2011-06-07 U. Baur , T. Han , J. Ohnemus

The new formalism for description of (un)polarized semi-inclusive DIS at moderate energies is developed. Hadron production is modeled as a product of distribution functions and hadronization functions (HFs) weighted by the hard scattering…

High Energy Physics - Phenomenology · Physics 2009-01-07 Aram Kotzinian

The surprising polarisation of Lambdas and other hyperons measured in many unpolarised hadronic processes, p N --> Lambda X, has been a long standing challenge for QCD phenomenology. One possible explanation was suggested, related to non…

High Energy Physics - Phenomenology · Physics 2019-08-07 Mauro Anselmino , Raj Kishore , Asmita Mukherjee

We investigate the chargino production process $\gamma\gamma\rightarrow\tilde{W}^{+}\tilde{W}^{-}$ at high energy $\gamma\gamma$ colliders in the framework of the minimal supersymmetric standard model (MSSM). Here the high energy $\gamma$…

High Energy Physics - Phenomenology · Physics 2019-08-15 Masayuki Koike , Toshihiko Nonaka , Tadashi Kon

The longitudinal polarization of hyperons in $e^+e^-$ annihilation at high energies depends on the longitudinal polarization of the quark produced at the $e^+e^-$ annihilation vertex whereas the spin alignment of vector mesons is…

High Energy Physics - Phenomenology · Physics 2017-02-22 Kai-bao Chen , Wei-hua Yang , Ya-jin Zhou , Zuo-tang Liang

In this work, we calculate the next-to-leading-order (NLO) QCD corrections to the process $p+p \to J/\psi + \gamma$ via the color-singlet mechanism at the LHC. The results show that the partial cross section ($p_t^{J/\psi}>$3GeV and…

High Energy Physics - Phenomenology · Physics 2009-02-02 Rong Li , Jian-Xiong Wang

Different phenomenological approaches for Lambda and Lambda-bar polarization in polarized semi-inclusive deep inelastic scattering and electron-positron annihilation at Z^0 pole are considered. Current and future experiments will soon…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. M. Kotzinian

In the fragmentation of a transversely polarized quark a left-right asymmetry, the Collins asymmetry, is expected for each hadron produced in the process $\mu N \rightarrow \mu ' h^{+} h^{-} X$. Similarly, an asymmetry is also expected for…

High Energy Physics - Experiment · Physics 2016-03-23 Franco Bradamante

The NRQCD factorization approach for quarkonium production at hadron colliders is reviewed. The prediction of J/psi and psi(2S) transverse polarization at large transverse momentum is confronted with recent experimental data, and potential…

High Energy Physics - Phenomenology · Physics 2009-04-13 Michael Krämer

The process $p p \to Z \gamma + X \to \ell^- \ell^+ \gamma + X$, where $\ell$ denotes a lepton, is calculated to order $\alpha_s$. Total and differential cross sections, with acceptance cuts imposed on the leptons and photon, are given for…

High Energy Physics - Phenomenology · Physics 2009-10-28 J. Ohnemus

The interaction of two laser pulses in an underdense plasma has proven to be able to inject electrons in plasma waves, thus providing a stable and tunable source of electrons. Whereas previous works focused on the "beatwave" injection…

Plasma Physics · Physics 2009-02-12 C. Rechatin , J. Faure , A. Lifschitz , X. Davoine , E. Lefebvre , V. Malka

We report the first observation of the spontaneous polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons transverse to the production plane in $e^+e^-$ annihilation, which is attributed to the effect arising from a polarizing fragmentation…

High Energy Physics - Experiment · Physics 2019-02-06 Belle Collaboration , Y. Guan , A. Vossen , I. Adachi , K. Adamczyk , J. K. Ahn , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , V. Aulchenko , T. Aushev , R. Ayad , V. Babu , I. Badhrees , A. M. Bakich , V. Bansal , P. Behera , C. Beleño , M. Berger , V. Bhardwaj , B. Bhuyan , T. Bilka , J. Biswal , A. Bobrov , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , L. Cao , D. Červenkov , P. Chang , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , K. Cho , S. -K. Choi , Y. Choi , D. Cinabro , S. Cunliffe , N. Dash , S. Di Carlo , J. Dingfelder , Z. Doležal , T. V. Dong , Z. Drásal , S. Eidelman , D. Epifanov , J. E. Fast , T. Ferber , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , M. Gelb , A. Giri , P. Goldenzweig , B. Golob , E. Guido , J. Haba , K. Hayasaka , H. Hayashii , S. Hirose , W. -S. Hou , T. Iijima , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , I. Jaegle , H. B. Jeon , S. Jia , Y. Jin , D. Joffe , K. K. Joo , T. Julius , K. H. Kang , T. Kawasaki , C. Kiesling , D. Y. Kim , H. J. Kim , J. B. Kim , K. T. Kim , S. H. Kim , K. Kinoshita , P. Kodyš , S. Korpar , D. Kotchetkov , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , R. Kulasiri , A. Kuzmin , Y. -J. Kwon , J. S. Lange , I. S. Lee , S. C. Lee , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , D. Liventsev , M. Lubej , T. Luo , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , H. Miyata , R. Mizuk , G. B. Mohanty , H. K. Moon , T. Mori , R. Mussa , M. Nakao , T. Nanut , K. J. Nath , Z. Natkaniec , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , S. Ogawa , S. Okuno , H. Ono , P. Pakhlov , G. Pakhlova , B. Pal , S. Pardi , H. Park , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , V. Popov , E. Prencipe , A. Rabusov , A. Rostomyan , G. Russo , D. Sahoo , Y. Sakai , M. Salehi , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , R. Seidl , Y. Seino , K. Senyo , O. Seon , M. E. Sevior , V. Shebalin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , F. Simon , A. Sokolov , E. Solovieva , M. Starič , J. F. Strube , M. Sumihama , T. Sumiyoshi , W. Sutcliffe , K. Suzuki , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , M. Uchida , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Usov , S. E. Vahsen , C. Van Hulse , R. Van Tonder , G. Varner , A. Vinokurova , V. Vorobyev , E. Waheed , B. Wang , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , S. Watanuki , E. Widmann , E. Won , H. Ye , J. Yelton , J. H. Yin , C. Z. Yuan , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov , A. Zupanc

We discuss the polarization of top quarks produced at a polarized linear e^+ e^- collider. Close-to-maximal values of the top quark polarization can be achieved with longitudinal beam polarizations (h_- = -0.80, h_+ = +0.625) or (h_- =…

High Energy Physics - Phenomenology · Physics 2011-12-06 S. Groote , J. G. Körner
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