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Related papers: First Results on 12Lambda-C production at DAPHNE

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The HyperCP experiment (Fermilab E871) was designed to search for rare phenomena in the decays of charged strange particles, in particular CP violation in $\Xi$ and $\Lambda$ hyperon decays with a sensitivity of $10^{-4}$. Intense charged…

We first determine the Lambda-N S-wave phase shifts so as to reproduce the experimental Lambda separation energies of A=3, 4 Lambda-hypernuclei, and then construct three phase-equivalent Lambda-N potentials with different central repulsion.…

Nuclear Theory · Physics 2009-10-31 Hidekatsu Nemura , Yasuyuki Suzuki , Yoshikazu Fujiwara , Choki Nakamoto

In a recent paper [PLB 837 (2023) 137669] we showed that all measured ($1s_\Lambda$, $1p_\Lambda$) pairs of $\Lambda$ binding energies in $\Lambda$-hypernuclei across the periodic table, $12\leq A \leq 208$, can be obtained from a…

Nuclear Theory · Physics 2023-08-15 E. Friedman , A. Gal

We address the $\Lambda$-hypernuclear `overbinding problem' in light hypernuclei which stands for a 1--3 MeV excessive $\Lambda$ separation energy calculated in $_{\Lambda}^5$He. This problem arises in most few-body calculations that…

Nuclear Theory · Physics 2018-09-12 Lorenzo Contessi , Nir Barnea , Avraham Gal

Coherent pi0 photo- and electroproduction on 4He and 12C nuclei is investigated in the framework of a distorted wave impulse approximation in momentum space. The elementary process is described by the recently developed unitary isobar…

Nuclear Theory · Physics 2011-07-19 D. Drechsel , L. Tiator , S. S. Kamalov , Shin Nan Yang

Precise knowledge of hadron production rates in the generation of neutrino beams is necessary for accelerator-based neutrino experiments to achieve their physics goals. NA61/SHINE, a large-acceptance hadron spectrometer, has recorded…

High Energy Physics - Experiment · Physics 2020-01-20 SHINE Collaboration , A. Aduszkiewicz , E. V. Andronov , T. Antićić , V. Babkin , M. Baszczyk , S. Bhosale , A. Blondel , M. Bogomilov , A. Brandin , A. Bravar , W. Bryliński , J. Brzychczyk , M. Buryakov , O. Busygina , A. Bzdak , H. Cherif , M. Ćirković , M. Csanad , J. Cybowska , T. Czopowicz , A. Damyanova , N. Davis , M. Deliyergiyev , M. Deveaux , A. Dmitriev , W. Dominik , P. Dorosz , J. Dumarchez , R. Engel , G. A. Feofilov , L. Fields , Z. Fodor , A. Garibov , M. Gaździcki , O. Golosov , M. Golubeva , K. Grebieszkow , F. Guber , A. Haesler , S. N. Igolkin , S. Ilieva , A. Ivashkin , S. R. Johnson , K. Kadija , E. Kaptur , N. Kargin , E. Kashirin , M. Kiełbowicz , V. A. Kireyeu , V. Klochkov , V. I. Kolesnikov , D. Kolev , A. Korzenev , V. N. Kovalenko , K. Kowalik , S. Kowalski , M. Koziel , A. Krasnoperov , W. Kucewicz , M. Kuich , A. Kurepin , D. Larsen , A. László , T. V. Lazareva , M. Lewicki , K. Łojek , B. Łysakowski , V. V. Lyubushkin , M. Maćkowiak-Pawłowska , Z. Majka , B. Maksiak , A. I. Malakhov , A. Marchionni , A. Marcinek , A. D. Marino , K. Marton , H. -J. Mathes , T. Matulewicz , V. Matveev , G. L. Melkumov , A. O. Merzlaya , B. Messerly , Ł. Mik , G. B. Mills , S. Morozov , S. Mrówczyński , Y. Nagai , M. Naskręt , V. Ozvenchuk , V. Paolone , M. Pavin , O. Petukhov , R. Płaneta , P. Podlaski , B. A. Popov , B. Porfy , M. Posiadała-Zezula , D. S. Prokhorova , D. Pszczel , S. Puławski , J. Puzović , M. Ravonel , R. Renfordt , E. Richter-Wąs , D. Röhrich , E. Rondio , M. Roth , B. T. Rumberger , M. Rumyantsev , A. Rustamov , M. Rybczynski , A. Rybicki , A. Sadovsky , K. Schmidt , I. Selyuzhenkov , A. Yu. Seryakov , P. Seyboth , M. Słodkowski , A. Snoch , P. Staszel , G. Stefanek , J. Stepaniak , M. Strikhanov , H. Ströbele , T. Šuša , A. Taranenko , A. Tefelska , D. Tefelski , V. Tereshchenko , A. Toia , R. Tsenov , L. Turko , R. Ulrich , M. Unger , F. F. Valiev , D. Veberič , V. V. Vechernin , A. Wickremasinghe , Z. Włodarczyk , A. Wojtaszek-Szwarc , K. Wójcik , O. Wyszyński , L. Zambelli , E. D. Zimmerman , R. Zwaska

The KLOE detector at DAFNE, the Frascati Phi-factory, has collected about 8 millions phi decays in 1999. Measurements of Phi decays into pi0, eta, eta', f0(980), a0(980) and pi+pi-pi0 have been performed with statistical accuracy better…

High Energy Physics - Experiment · Physics 2012-08-27 The KLOE collaboration

Quark-model hyperon-nucleon and hyperon-hyperon interactions by the Kyoto-Niigata group are applied to the two-Lambda plus alpha system in a new three-cluster Faddeev formalism using two-cluster resonating-group method kernels. The model…

Nuclear Theory · Physics 2009-11-10 Y. Fujiwara , M. Kohno , K. Miyagawa , Y. Suzuki , J. -M. Sparenberg

The excellent particle identification capabilities of the ALICE detector, using the time projection chamber and the time-of-flight detector, allow the detection of light nuclei and anti-nuclei. Furthermore, the high tracking resolution…

Nuclear Experiment · Physics 2016-11-23 Natasha Sharma

We investigate the properties of the single Lambda hypernuclei within a Skyrme-Hartree-Fock (SHF) model. The parameters of the Skyrme type effective lambda-nucleon (Lambda N) interaction are obtained by fitting to the experimental Lambda…

Nuclear Theory · Physics 2012-06-01 Neelam Guleria , Shashi K. Dhiman , Radhey Shyam

Production of Lambda and Antilambda hyperons was measured in central Pb-Pb collisions at 40, 80, and 158 A$\cdot$GeV beam energy on a fixed target. Transverse mass spectra and rapidity distributions are given for all three energies. The…

Nuclear Experiment · Physics 2011-08-17 The NA49 Collaboration , T. Anticic

The asymmetry parameter alpha_p^NM for a proton exclusively emitted in the Lambda p -> np process was, for the first time, measured in the non-mesonic weak decay of a polarized 5_La,bda_He hypernucleus by selecting the proton-neutron pairs…

We present the first observation of $\mathrm{^{3}_\Lambda H}$ and $\mathrm{^{4}_\Lambda H}$ in Ag+Ag collisions at $\mathrm{\sqrt{s_{NN}}}$ = 2.55 GeV, emitted around mid-rapidity. The hypernuclei are reconstructed via their two-body decay…

Nuclear Experiment · Physics 2025-12-16 R. Abou Yassine , J. Adamczewski-Musch , C. Asal , M. Becker , A. Belounnas , A. Blanco , C. Blume , L. Chlad , P. Chudoba , I. Ciepał , J. Dreyer , W. A. Esmail , L. Fabbietti , H. Floersheimer , J. Förtsch , P. Fonte , J. Friese , I. Fröhlich , T. Galatyuk , R. Greifenhagen , M. Grunwald , M. Gumberidze , S. Harabasz , T. Heinz , C. Höhne , F. Hojeij , R. Holzmann , H. Huck , M. Idzik , B. Kämpfer , K-H. Kampert , B. Kardan , V. Kedych , S. Kim , I. Koenig , W. Koenig , M. Kohls , J. Kolas , G. Kornakov , R. Kotte , I. Kres , W. Krueger , A. Kugler , R. Lalik , S. Lebedev , S. Linev , F. Linz , L. Lopes , M. Lorenz , A. Malige , J. Markert , T. Matulewicz , S. Maurus , V. Metag , J. Michel , A. Molenda , C. Müntz , M. Nabroth , L. Naumann , K. Nowakowski , A. Opíchal , J. Orliński , J. -H. Otto , M. Parschau , C. Pauly , D. Pawlowska-Szymanska , V. Pechenov , O. Pechenova , D. Pfeifer , K. Piasecki , J. Pietraszko , T. Povar , K. Prościński , A. Prozorov , W. Przygoda , K. Pysz , B. Ramstein , N. Rathod , J. Ritman , A. Rost , A. Rustamov , P. Salabura , J. Saraiva , K. Scharmann , N. Schild , E. Schwab , F. Scozzi , F. Seck , I. Selyuzhenkov , U. Singh , L. Skorpil , J. Smyrski , S. Spies , A. Sreejith , H. Ströbele , J. Stroth , K. Sumara , O. Svoboda , M. Szala , P. Tlusty , M. Traxler , S. Treliński , I. C. Udrea , F. Ulrich-Pur , C. Ungethum , V. Wagner , A. A. Weber , C. Wendisch , J. Wirth , A. Władyszewska , H. P. Zbroszczyk , E. Zherebtsova , M. Zieliński , P. Zumbruch

The SIDDHARTA-2 collaboration at the INFN Laboratories of Frascati (LNF) aims to perform groundbreaking measurements on kaonic atoms. In parallel and beyond the ongoing kaonic deuterium, presently running on the DA$\Phi$NE collider at LNF,…

The $\phi$-meson production cross section is measured for the first time at a sub-threshold energy of 1.93 AGeV in \nuc{58}{Ni}+\nuc{58}{Ni} central collisions. The $\phi$ data were obtained within the acceptance of the CDC/Barrel subsystem…

Nuclear Experiment · Physics 2019-08-14 A. Mangiarotti , N. Herrmann , P. R. Maurenzig , A. Gobbi , R. Kotte , J. Kecskemeti , Y. Leifels

Photoproduction of $\Lambda$(1520) with liquid hydrogen and deuterium targets was examined at photon energies below 2.4 GeV in the SPring-8 LEPS experiment. For the first time, the differential cross sections were measured at low energies…

At the Frascati phi-factory DAPHNE the pion formfactor is measured by means of the 'radiative return', i.e. by using events in which one of the collider electrons (positrons) has radiated an initial state radiation photon, lowering in such…

High Energy Physics - Experiment · Physics 2007-05-23 Achim Denig , KLOE collaboration

Using data from the FOCUS (E831) experiment at Fermilab, we present a new measurement of the weak decay-asymmetry parameter alpha(Lambdac) in Lambdac --> Lambda pi decay. Comparing particle with antiparticle decays, we obtain the first…

High Energy Physics - Experiment · Physics 2008-11-26 J. M. Link

There are several potential advantages for a collider operation with a lattice with negative momentum compaction factor (alfa). Since the lattice of the Frascati e+e- Phi-factory DAFNE is flexible enough to provide collider operation even…

Accelerator Physics · Physics 2014-11-18 M. Zobov , D. Alesini , M. E. Biagini , A. Drago , A. Gallo , C. Milardi , P. Raimondi , B. Spataro , A. Stella