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Related papers: The Strangeness Physics Program at CLAS

200 papers

Two charged pion final states are studied for GeV photons incident on protons. The data come from Thomas Jefferson National Accelerator Facility using the CLAS detector. A tagged photon beam of 0.5-2.4 GeV/c was produced through…

High Energy Physics - Experiment · Physics 2019-08-14 Matt Bellis

The spectra of strange hadrons are measured in proton-proton collisions, recorded by the CMS experiment at the CERN LHC, at centre-of-mass energies of 0.9 and 7 TeV. The K^0_s, Lambda, and Xi^- particles and their antiparticles are…

High Energy Physics - Experiment · Physics 2012-08-27 The CMS Collaboration

We summarize the physics topics which can be addressed by measurements of high-Q^2 exclusive electroproduction of strange mesons, gamma* N -> phi N, K* Lambda, K Lambda, K Sigma, at Jefferson Lab with 11 GeV beam energy. The proposed…

High Energy Physics - Phenomenology · Physics 2008-04-04 M. Strikman , C. Weiss

In this contribution we discuss the physics of strange hadrons in low energy ($\simeq 1-2 \rm AGeV$) heavy ion collision. In this energy range the relevant strange particle are the kaons and anti-kaons. The most interesting aspect…

Nuclear Theory · Physics 2016-09-08 Volker Koch

The longitudinal and transverse components of the cross section for the $e p\to e^\prime p \rho^0$ reaction were measured in Hall B at Jefferson Laboratory using the CLAS detector. The data were taken with a 4.247 GeV electron beam and were…

High Energy Physics - Experiment · Physics 2010-04-06 C. Hadjidakis

First measurements of double-polarization observables in $\omega$ photoproduction off the proton are presented using transverse target polarization and data from the CEBAF Large Acceptance Spectrometer (CLAS) FROST experiment at Jefferson…

Nuclear Experiment · Physics 2019-05-02 P. Roy , S. Park , V. Crede , A. V. Anisovich , E. Klempt , V. A. Nikonov , A. V. Sarantsev , N. C. Wei , F. Huang , K. Nakayama , K. P. Adhikari , S. Adhikari , G. Angelini , H. Avakian , L. Barion , M. Battaglieri , I. Bedlinskiy , A. S. Biselli , S. Boiarinov , W. J. Briscoe , J. Brock , W. K. Brooks , V. D. Burkert , F. Cao , C. Carlin , D. S. Carman , A. Celentano , P. Chatagnon , T. Chetry , G. Ciullo , P. L. Cole , M. Contalbrigo , O. Cortes , A. D'Angelo , N. Dashyan , R. De Vita , E. De Sanctis , A. Deur , S. Diehl , C. Djalali , M. Dugger , R. Dupre , B. Duran , H. Egiyan , M. Ehrhart , A. El Alaoui , L. El Fassi , P. Eugenio , S. Fegan , A. Filippi , A. Fradi , G. P. Gilfoyle , F. X. Girod , E. Golovatch , R. W. Gothe , K. A. Griffioen , M. Guidal , L. Guo , K. Hafidi , C. Hanretty , N. Harrison , M. Hattawy , T. B. Hayward , D. Heddle , K. Hicks , M. Holtrop , Y. Ilieva , D. G. Ireland , B. S. Ishkhanov , E. L. Isupov , D. Jenkins , H. S. Jo , S. Johnston , S. Joosten , M. L. Kabir , C. D. Keith , D. Keller , G. Khachatryan , M. Khachatryan , A. Khanal , M. Khandaker , A. Kim , W. Kim , F. J. Klein , V. Kubarovsky , S. V. Kuleshov , M. C. Kunkel , L. Lanza , P. Lenisa , K. Livingston , I. J. D. MacGregor , D. Marchand , B. McKinnon , D. G. Meekins , C. A. Meyer , T. Mineeva , V. Mokeev , R. A. Montgomery , A Movsisyan , C. Munoz Camacho , P. Nadel-Turonski , S. Niccolai , G. Niculescu , M. Osipenko , A. I. Ostrovidov , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , D. Payette , W. Phelps , J. Pierce , O. Pogorelko , Y. Prok , D. Protopopescu , B. A. Raue , M. Ripani , D. Riser , B. G. Ritchie , A. Rizzo , G. Rosner , F. Sabatie , C. Salgado , R. A. Schumacher , M. L. Seely , Y. G. Sharabian , U. Shrestha , Iu. Skorodumina , D. Sokhan , O. Soto , N. Sparveris , I. I. Strakovsky , S. Strauch , M. Taiuti , J. A. Tan , B. Torayev , N. Tyler , M. Ungaro , H. Voskanyan , E. Voutier , N. K. Walford , R. Wang , D. P. Watts , X. Wei , M. H. Wood , N. Zachariou , J. Zhang , Z. W. Zhao

In this work we present the results of a theoretical analysis of the data on photoproduction of $f_0(980)$ meson in the laboratory photon energy between 3.0 and 3.8 GeV. A comparison is done to the measurements performed by the CLAS…

High Energy Physics - Phenomenology · Physics 2013-08-07 M. L. L. da Silva , M. V. T. Machado

Nuclear experiments near and below the threshold of hyperon production have shown that the production of Kaons is a sensitive probe for the dense QCD equation of state. At beam energies up to 1.5AGeV, strangeness production can probe the…

Nuclear Theory · Physics 2026-02-09 Jan Steinheimer , Tom Reichert , Marcus Bleicher

The recent Investigations in the chiral quark model show that kaon productions of nucleon play an important role in understanding the structure of baryons. The evidences of a third $S_{11}$ resonance in the second resonance region and two…

Nuclear Theory · Physics 2009-10-30 Zhenping Li

During the last two years several experimental approaches to strange systems have been realized at the spectrometer facility of the Mainz Microtron MAMI. An instrument of central importance for the strangeness electro-production program is…

Nuclear Experiment · Physics 2012-06-15 P. Achenbach

We measured the ratios of electroproduction cross-sections from a proton target for three exclusive meson-baryon final states: $\Lambda K^+$, $p\pi^0$, and $n\pi^+$, with the CLAS detector at Jefferson Lab. Using a simple model of quark…

Nuclear Experiment · Physics 2014-12-10 K. Park , M. D. Mestayer , the CLAS collaboration

Strangeness production is calculated in a pQCD-based model (including nuclear effects) in the high transverse momentum sector, where pQCD is expected to work well. We investigate pion, kaon, proton and lambda production in pp and heavy-ion…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. G. Barnafoldi , G. Fai , P. Levai , B. A. Cole , G. Papp

One of the most surprising discoveries made at Jefferson Lab has been the discrepancy in the determinations of the proton's form factor ratio $\mu_p G_E^p/G_M^p$ between unpolarized cross section measurements and the polarization transfer…

The GlueX experiment located at Jefferson Lab studies the spectrum of hadrons using photoproduction on a LH$_2$ target in a wide variety of final states. With its detector system capable of measuring neutral and charged final state…

High Energy Physics - Experiment · Physics 2022-11-30 Peter Pauli

We comment on the important phenomenological aspects of the recent high-statistics and wide-angle coverage $\phi$ photoproduction data from CLAS at Jefferson Lab. The most prominent feature is a localized structure at a center-of-mass (c.m)…

High Energy Physics - Experiment · Physics 2014-03-18 Biplab Dey

Strangeness production has long been proposed as a diagnostic tool for understanding the dynamics of relativistic heavy ion collisions. In this presentation we review the traditional picture of strangeness enhancement as a signature for…

High Energy Physics - Phenomenology · Physics 2017-08-23 J. L. Nagle

The COoler SYnchrotron COSY-J\"ulich delivers phase-space cooled, polarized proton and deuteron beams with momenta up to p=3.65 GeV/c. Various experiments on hadron-induced strangeness production on proton, neutron and nuclear targets have…

Nuclear Experiment · Physics 2009-11-10 M. Buescher

In this paper I highlight a few selected topics on strange particle production in heavy-ion collisions. By studying the yield and spectra of strange particles we hope to gain understanding of the conditions reached in, and the ensuing…

Nuclear Experiment · Physics 2009-11-10 Helen Caines

Kaon photo- and electroproduction off a proton near the production threshold are investigated by utilizing an isobar model. The background amplitude of the model is constructed from Feynman diagrams, whereas the resonance term is calculated…

Nuclear Theory · Physics 2011-01-19 T. Mart

Strange particles have been a very important observable in the search for a deconfined state of strongly interacting matter, the quark-gluon plasma (QGP), which is expected to be formed in ultra-relativistic heavy ion collisions. We review…

Nuclear Experiment · Physics 2015-05-28 Christoph Blume , Christina Markert