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Using the largest $J/\psi$ and $\psi(3686)$ data samples collected at the BESIII experiment, the hyperon anti-hyperon pairs are generated in their quantum entangle system. The polarization of hyperon has been observed, which makes it…

High Energy Physics - Experiment · Physics 2022-07-29 Liang Yan

A possible interpretation of the near-threshold enhancement in the $(p\bar{p})$-mass spectrum in $J/\psi{\to}\gamma p{\bar p}$ is the of existence of a narrow baryonium resonance X(1860). Mesonic decays of the $(p\bar{p})$-bound state…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gui-Jun Ding , Mu-Lin Yan

The newly found states Y(4260), Y(4361), Y(4664) and Z$^\pm$(4430) stir broad interest in the study of spectroscopy in a typical charmonium scale. The Y(4260) which was observed earlier has been interpreted as hybrid, molecular state, and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Cong-Feng Qiao

The importance of Born terms and resonance exchange for eta and eta-prime photoproduction off both the proton and neutron within U(3) baryon chiral perturbation theory is investigated. Low-lying resonances such as the vector mesons and J^P=…

High Energy Physics - Phenomenology · Physics 2009-11-07 B. Borasoy

Protons and neutrons are the building blocks of matter, glued together in nuclei by strong interactions. They can be excited by pions, real and virtual photons, neutrinos and other probes. These excitations are referred to as light baryon…

Nuclear Theory · Physics 2025-10-16 Michael Döring

We searched for proton decay via $p \to e^{+}\pi^{0}\pi^{0}$ and $p \to \mu^{+}\pi^{0}\pi^{0}$ in 0.401 megaton-years of data collected in all pure water detector phases of Super-Kamiokande (SK) I-V. A theoretical study predicts proton…

High Energy Physics - Experiment · Physics 2026-04-17 Kamiokande Collaboration , K. Abe , S. Abe , Y. Asaoka , M. Harada , Y. Hayato , K. Hiraide , T. H. Hung , K. Hosokawa , K. Ieki , M. Ikeda , J. Kameda , Y. Kanemura , R. Kaneshima , Y. Kashiwagi , Y. Kataoka , S. Miki , S. Mine , M. Miura , S. Moriyama , K. Nakagiri , M. Nakahata , S. Nakayama , Y. Noguchi , G. Pronost , K. Okamoto , K. Sato , H. Sekiya , H. Shiba , K. Shimizu , R. Shinoda , M. Shiozawa , Y. Sonoda , Y. Suzuki , A. Takeda , Y. Takemoto , A. Takenaka , H. Tanaka , T. Yano , S. Chen , Y. Itow , T. Kajita , R. Nishijima , K. Okumura , T. Tashiro , T. Tomiya , X. Wang , S. Yoshida , P. Fernandez , L. Labarga , D. Samudio , B. Zaldivar , F. G. Garay , B. W. Pointon , C. Yanagisawa , B. Jargowsky , E. Kearns , J. Mirabito , J. L. Raaf , L. Wan , T. Wester , J. Bian , B. Cortez , N. J. Griskevich , Y. Jiang , S. Locke , M. B. Smy , H. W. Sobel , V. Takhistov , H. G. Berns , J. Hill , M. C. Jang , S. H. Lee , D. H. Moon , R. G. Park , B. S. Yang , B. Bodur , K. Scholberg , C. W. Walter , A. Beauchêne , O. Drapier , A. Ershova , M. Ferey , A. Giampaolo , Z. Hu , E. Le Blévec , Th. A. Mueller , A. D. Santos , P. Paganini , C. Quach , R. Rogly , T. Nakamura , J. S. Jang , R. P. Litchfield , L. N. Machado , F. J. P. Soler , J. G. Learned , K. Choi , N. Iovine , S. Cao , L. H. V. Anthony , D. Martin , N. W. Prouse , M. Scott , A. A. Sztuc , Y. Uchida , V. Berardi , N. F. Calabria , M. G. Catanesi , N. Ospina , E. Radicioni , A. Langella , G. De Rosa , G. Collazuol , M. Feltre , F. Iacob , M. Mattiazzi , L. Ludovici , M. Gonin , L. Périssé , B. Quilain , M. Fukazawa , C. Fujisawa , S. Horiuchi , A. Kawabata , M. Kobayashi , Y. M. Liu , Y. Maekawa , Y. Nishimura , A. Oka , R. Okazaki , R. Akutsu , M. Friend , T. Hasegawa , Y. Hino , T. Ishida , T. Kobayashi , M. Jakkapu , T. Matsubara , T. Nakadaira , K. Nakamura , Y. Oyama , A. Portocarrero Yrey , K. Sakashita , T. Sekiguchi , T. Tsukamoto , N. Bhuiyan , G. T. Burton , F. Di Lodovico , J. Gao , A. Goldsack , T. Katori , R. Kralik , N. Latham , J. Migenda , R. M. Ramsden , V. Siccardi , S. Zsoldos , S. Aoyama , H. Bambara , H. Ito , T. Sone , A. T. Suzuki , Y. Takagi , Y. Takeuchi , S. Wada , H. Zhong , M. Nishigami , Y. Inaba , J. Feng , L. Feng , S. Han , J. Hikida , J. R. Hu , M. Kawaue , T. Kikawa , T. Nakaya , T. V. Ngoc , R. A. Wendell , K. Yasutome , S. J. Jenkins , N. McCauley , P. Mehta , A. Tarrant , M. Fanì , M. J. Wilking , Z. Xie , Y. Fukuda , H. Menjo , K. Ninomiya , Y. Yoshioka , J. Lagoda , M. Mandal , P. Mijakowski , J. Zalipska , M. Mori , M. Jia , J. Jiang , C. K. Jung , W. Shi , K. Hamaguchi , H. Ishino , Y. Koshio , F. Nakanishi , S. Sakai , T. Tada , T. Tano , Y. Asano , S. Ohshita , T. Ishizuka , G. Barr , D. Barrow , L. Cook , S. Samani , D. Wark , A. Holin , F. Nova , M. Jo , S. Jung , J. Y. Yang , J. Yoo , J. E. P. Fannon , L. Kneale , M. Malek , J. M. McElwee , T. Peacock , P. Stowell , M. D. Thiesse , L. F. Thompson , S. T. Wilson , H. Okazawa , S. M. Lakshmi , S. Hong , S. B. Kim , E. Kwon , M. W. Lee , J. W. Seo , I. Yu , Y. Ashida , A. K. Ichikawa , K. D. Nakamura , S. Tairafune , A. Eguchi , S. Goto , H. Hayasaki , S. Kodama , Y. Kong , Y. Masaki , Y. Mizuno , T. Muro , M. Sekiyama , T. Yamazumi , Y. Nakajima , S. Shima , N. Taniuchi , E. Watanabe , M. Yokoyama , P. de Perio , S. Fujita , C. Jesús-Valls , K. Martens , Ll. Marti , K. M. Tsui , M. R. Vagins , J. Xia , M. Kuze , S. Izumiyama , R. Matsumoto , K. Terada , R. Asaka , M. Ishitsuka , C. Ise , Y. Ommura , N. Shigeta , M. Shinoki , M. Sugo , M. Wako , K. Yamauchi , T. Yoshida , Y. Nakano , A. Yankelevich , F. Cormier , R. Gaur , V. Gousy-Leblanc , M. Hartz , A. Konaka , X. Li , B. R. Smithers , S. Chen , Y. Wu , B. D. Xu , A. Q. Zhang , B. Zhang , H. Adhikary , M. Girgus , P. Govindaraj , M. Posiadala-Zezula , Y. S. Prabhu , S. B. Boyd , R. Edwards , D. Hadley , M. Nicholson , M. O'Flaherty , B. Richards , A. Ali , B. Jamieson , S. Amanai , C. Bronner , D. Horiguchi , A. Minamino , Y. Sasaki , R. Shibayama , R. Shimamura , S. Suzuki

Pentaquark states have been extensively investigated theoretically in the context of the constituent quark model. In this paper results of an experimental search for pentaquarks in the \Xim\pim, \Xim\pip, \Xip\pim and \Xip\pip invariant…

High Energy Physics - Experiment · Physics 2020-06-04 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 , V. Golovatyuk , M. Golubeva , K. Grebieszkow , F. Guber , A. Haesler , S. N. Igolkin , S. Ilieva , A. Ivashkin , S. R. Johnson , K. Kadija , N. Kargin , E. Kashirin , M. Kiełbowicz , V. A. Kireyeu , V. Klochkov , V. I. Kolesnikov , D. Kolev , A. Korzenev , V. N. Kovalenko , S. Kowalski , M. Koziel , A. Krasnoperov , W. Kucewicz , M. Kuich , A. Kurepin , D. Larsen , A. László , T. V. Lazareva , M. Lewicki , K. Łojek , V. V. Lyubushkin , M. Maćkowiak-Pawłowska , Z. Majka , B. Maksiak , A. I. Malakhov , A. Marcinek , A. D. Marino , K. Marton , H. -J. Mathes , T. Matulewicz , V. Matveev , G. L. Melkumov , A. O. Merzlaya , B. Messerly , Ł. Mik , S. Morozov , S. Mrówczyński , Y. Nagai , M. Naskręt , V. Ozvenchuk , V. Paolone , 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 , 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 , 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 , O. Wyszyński , E. D. Zimmerman , R. Zwaska

The uncertainties of the Standard Model prediction of the anomalous magnetic moment of the muon are currently completely dominated by hadronic contributions. The largest contribution is due to the hadronic vacuum polarization. Hadronic…

High Energy Physics - Experiment · Physics 2018-12-05 C. F. Redmer

Results of resonance searches in the Xi- pi-, Xi- pi+, antiXi+ pi- and antiXi+ pi+ invariant mass spectra in proton-proton collisions at sqrt{s}=17.2 GeV are presented. Evidence is shown for the existence of a narrow Xi- pi- baryon…

High Energy Physics - Experiment · Physics 2012-08-27 NA49 Collaboration

We calculate the decay of pionium atoms into two photons. The pion polarizability gives rise to a 10% correction to the corresponding decay width for pointlike pions. This opens the possibility to obtain the difference between the electric…

High Energy Physics - Phenomenology · Physics 2011-07-19 H. -W. Hammer , J. N. Ng

In this talk, we present a new interpretation for the recently observed $\Xi(1820)$ resonance. We recall that the chiral unitary approach for the interaction of pseudoscalar mesons with the baryons of the decuplet predicts two states for…

High Energy Physics - Phenomenology · Physics 2024-11-15 R. Molina , Wei-Hong Liang , Chu-Wen Xiao , Zhi-Feng Sun , E. Oset

Data are recalled on the relative yields of charged pions,charged kaons,protons,antiprotons,tritiun nuclei, anti-tritium, He3 nuclei and anti-He3 antinuclei produced at 0 degrees by 200-240 GeV/c protons on Beryllium and Aluminium targets.…

Nuclear Experiment · Physics 2013-07-25 Giorgio Giacomelli

The BESIII experiment at the Beijing Electron Positron collider, run as a ``hyperon factory'', recently reported the first measurement of the asymmetry parameter of the $\Lambda\to n\gamma$ decay and updated its branching fraction, which…

High Energy Physics - Phenomenology · Physics 2023-04-03 Rui-Xiang Shi , Li-Sheng Geng

The aim of this work is experimental discovery and research of a rare neutron mode, the radiative beta-decay, where a new particle, the radiative gamma-quantum, is formed along with the expected decay products beta-electron, recoil proton…

The electromagnetic form factors are fundamental observables that parametrise the electric and magnetic structure of hadrons and provide a key to the strong interaction. The Beijing Spectrometer (BESIII) is located at the Beijng Electron…

High Energy Physics - Experiment · Physics 2017-06-26 Cristina Morales Morales

The three body pion decays ${\pi}^+{\rightarrow}l^+{\nu}X~(l=e,{\mu})$, where $X$ is a weakly interacting neutral boson, were searched for using the full data set from the PIENU experiment. An improved limit on…

With about 12 fb$^{-1}$ collected XYZ data sets, BESIII continues the exploration of the exotic charmonium-like states. In this talk, recent results on the measurements of the spin-parity determination of $Z_{\rm c}(3900)$, as well as on…

High Energy Physics - Experiment · Physics 2018-06-28 Frank Nerling

The baryon-antibaryon SU(3) nonets are proposed as a scheme to classify the increased number of experimentally observed enhancements near the baryon antibaryon mass threshold. The scheme is similar to the Fermi-Yang-Sakata model, which was…

High Energy Physics - Phenomenology · Physics 2009-11-11 C. Z. Yuan , X. H. Mo , P. Wang

The first observation of the decay $\Xi^-_\mathrm{b}$ $\to$ $\psi$(2S)$\Xi^-$ and measurement of the branching ratio of $\Xi^-_\mathrm{b}$ $\to$ $\psi$(2S)$\Xi^-$ to $\Xi^-_\mathrm{b}$ $\to$ J/$\psi$$\Xi^-$ are presented. The J/$\psi$ and…

High Energy Physics - Experiment · Physics 2024-08-12 CMS Collaboration

We consider the early binary neutron star inspiral phase as a scenario to probe environmental axion--photon resonant conversion. For this we approximately model the merger site electromagnetic fields as the superposition of two rotating…

High Energy Astrophysical Phenomena · Physics 2026-02-18 D. Suárez-Fontanella , M. Ángeles Pérez-García , C. Albertus
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