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Related papers: Polarization in Hyperon Photo- and Electro- Produc…

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Despite decades of studies of the photoproduction of hyperons, both their production mechanisms and their spectra of excited states are still largely unknown. While the parity-violating weak decay of hyperons offers a means of measuring…

Nuclear Experiment · Physics 2018-07-11 J. Bono , L. Guo. , B. Raue

Recent measurements using the CLAS detector at Jefferson Lab of the reactions $\vec\gamma + p \to K^+ + \vec\Lambda$ and $\vec\gamma + p \to K^+ + \vec\Sigma^0$ have been used to extract the spin transfer coefficients $C_x$ and $C_z$ for…

Nuclear Experiment · Physics 2009-09-29 Reinhard Schumacher

Spin transfer from circularly polarized real photons to recoiling hyperons has been measured for the reactions $\vec\gamma + p \to K^+ + \vec\Lambda$ and $\vec\gamma + p \to K^+ + \vec\Sigma^0$. The data were obtained using the CLAS…

Nuclear Experiment · Physics 2010-04-06 R. Bradford , R. A. Schumacher , CLAS Collaboration

Background: Measurements of the polarization observables {\Sigma}, P, T, Ox, Oz for the reaction {\gamma}p {\rightarrow) KS0 {\Sigma}+ using a linearly polarized photon beam of energy 1.1 to 2.1 GeV are reported. Purpose: The measured data…

Nuclear Experiment · Physics 2024-05-01 CLAS Collaboration , L. Clark , B. McKinnon , D. G. Ireland , D. I. Glazier , K. Livingston , D. Rönchen

The CLAS collaboration has recently completed first measurements of the double polarization observables C_x and C_z for the reactions K^+Lambda and K^+Sigma^o photoproduction. C_x and C_z are the beam-recoil polarization asymmetries…

Nuclear Experiment · Physics 2017-08-23 Robert Bradford , Reinhard Schumacher

Developments in strangeness photo- and electro- production off the proton, as investigated using the CLAS system in Hall B at Jefferson Lab, are discussed in this paper. By measuring sufficient spin observables one can decompose the…

Nuclear Experiment · Physics 2011-02-01 Reinhard Schumacher

The CBELSA/TAPS experiment with a longitudinally or transversely polarized target and an energy tagged, linearly or circularly polarized photon beam allows the measurement of a large set of polarization observables. Due to its good energy…

Nuclear Experiment · Physics 2019-08-14 Jan Hartmann

The complete expression for the intensity in pseudo-scalar meson photoproduction with a polarized beam, target, and recoil baryon is derived using a density matrix approach that offers great economy of notation. A Cartesian basis with spins…

High Energy Physics - Phenomenology · Physics 2011-06-20 Biplab Dey , Michael E. McCracken , David G. Ireland , Curtis A. Meyer

We review the development of the most general analytic form of the cross section, dependent upon the three polarization vectors of the beam, target and recoil baryon, including all single, double and triple-polarization terms involving 16…

Nuclear Theory · Physics 2015-03-17 A. M. Sandorfi , S. Hoblit , H. Kamano , T. -S. H. Lee

Many excited nucleon states ($N^{*}$s) predicted by quark models, but not observed in $\pi N$ channels, are expected to couple strongly to kaon--hyperon ($KY$) channels. While in the last decade data have been published for $KY$…

Nuclear Experiment · Physics 2018-07-26 Colin Gleason , Yordanka Ilieva

[Background] A complete set is a minimum set of observables which allows one to determine the underlying reaction amplitudes unambiguously. Pseudoscalar-meson photoproduction from the nucleon is characterized by four such amplitudes and…

Nuclear Theory · Physics 2013-05-29 Tom Vrancx , Jan Ryckebusch , Tom Van Cuyck , Pieter Vancraeyveld

Hyperon recoil polarization measurements for the exclusive electroproduction of $K^+\Lambda$ and $K^+\Sigma^0$ final states from an unpolarized proton target have been carried out using the CLAS12 spectrometer at Jefferson Laboratory. The…

Nuclear Experiment · Physics 2025-05-20 D. S. Carman , A. D'Angelo , L. Lanza , V. I. Mokeev , P. Achenbach , J. S. Alvarado , M. J. Amaryan , H. Atac , H. Avakian , N. A. Baltzell , L. Barion , M. Bashkanov , M. Battaglieri , F. Benmokhtar , A. Bianconi , A. S. Biselli , M. Bondi , S. Boiarinov , F. Bossu , K. -Th. Brinkmann , W. J. Briscoe , S. Bueltmann , V. D. Burkert , T. Cao , R. Capobianco , A. Celentano , P. Chatagnon , V. Chesnokov , G. Ciullo , P. L. Cole , M. Contalbrigo , N. Dashyan , R. De Vita , A. Deur , S. Diehl , C. Dilks , C. Djalali , M. Dugger , R. Dupre , A. El Alaoui , L. El Fassi , L. Elouadrhiri , S. Fegan , A. Filippi , G. Gavalian , D. I. Glazier , R. W. Gothe , Y. Gotra , L. Guo , K. Hafidi , H. Hakobyan , M. Hattawy , F. Hauenstein , T. B. Hayward , D. Heddle , A. Hobart , M. Holtrop , Yu-Chun Hung , Y. Ilieva , D. G. Ireland , E. L. Isupov , H. Jiang , H. S. Jo , T. Kageya , V. Klimenko , A. Kripko , V. Kubarovsky , P. Lenisa , S. Liyanaarachchi , I. J. D. MacGregor , D. Marchand , V. Mascagna , D. Matamoros , M. Maynes , B. McKinnon , T. Mineeva , M. Mirazita , C. Munoz Camacho , P. Nadel-Turonski , T. Nagorna , K. Neupane , S. Niccolai , G. Niculescu , M. Osipenko , P. Pandey , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , S. J. Paul , W. Phelps , N. Pilleux , S. Polcher Rafael , J. W. Price , Y. Prok , B. A. Raue , T. Reed , M. Ripani , J. Ritman , P. Rossi , C. Salgado , S. Schadmand , A. Schmidt , M. B. C. Scott , Y. G. Sharabian , S. Shrestha , D. Sokhan , N. Sparveris , N. Spreafico , S. Stepanyan , I. I. Strakovsky , S. Strauch , J. A. Tan , N. Trotta , R. Tyson , M. Ungaro , S. Vallarino , L. Venturelli , T. Vittorini , H. Voskanyan , E. Voutier , Y. Wang , D P. Watts , U. Weerasinghe , X. Wei , M. H. Wood , L. Xu , N. Zachariou , Z. W. Zhao , M. Zurek

We study the polarization of hyperon in different processes in singly polarized $pp$ collisions, in particular its relation to the polarized parton distributions. We show that by measuring hyperon polarization in particularly chosen…

High Energy Physics - Phenomenology · Physics 2009-11-10 Qing-hua Xu , Zuo-tang Liang

A method to extract the polarization of $\Omega$ hyperons produced via the strong interaction is presented. Assuming they are spin 3/2 particles, the corresponding spin density matrix can be written in terms of seven non-zero polarization…

Nuclear Theory · Physics 2018-04-02 Elisabetta Perotti

Positivity constraints have proved to be important for spin observables of exclusive reactions involving polarized initial and final particles. Attention is focused in this note on the photoproduction of pseudoscalar mesons from spin 1/2…

Nuclear Theory · Physics 2008-11-26 Xavier Artru , Jean-Marc Richard , Jacques Soffer

Background: Measurements of polarization observables for the reactions $\vec{\gamma} p \rightarrow K^+ \Lambda$ and $\vec{\gamma} p \rightarrow K^+ \Sigma^0$ have been performed. This is part of a programme of measurements designed to study…

Nuclear Experiment · Physics 2016-06-22 CLAS Collaboration , C. A. Paterson , D. G. Ireland , K. Livingston , B. McKinnon

We develop polarization observables for the processes $\gamma N\to\pi\pi N$ and $\pi N\to\pi\pi N$, using both a helicity and hybrid helicity-transversity basis. Such observables are crucial if processes that produce final states consisting…

Nuclear Theory · Physics 2014-11-18 W. Roberts , T. Oed

A complete set for pseudoscalar-meson photoproduction is a minimum set of observables from which one can determine the underlying reaction amplitudes unambiguously. The complete sets considered in this work involve single- and…

Nuclear Theory · Physics 2015-06-23 Jannes Nys , Tom Vrancx , Jan Ryckebusch

A general analysis of polarization phenomena for coherent meson electroproduction on deuterons, $e+ d\to e+ d +P^0$, where $P^0$ is a pseudoscalar $\pi ^0$ or $\eta$-meson, is presented. The spin structure of the electromagnetic current for…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michail P. Rekalo , Egle Tomasi-Gustafsson , Jacques Arvieux
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