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To study fundamental questions of hadron and nuclear physics in interactions of antiprotons with nucleons and nuclei, the universal PANDA detector will be built. Gluonic excitations, the physics of strange and charm quarks and nucleon…

High Energy Physics - Experiment · Physics 2019-08-17 PANDA Collaboration , W. Erni , I. Keshelashvili , B. Krusche , M. Steinacher , Y. Heng , Z. Liu , H. Liu , X. Shen , O. Wang , H. Xu , J. Becker , F. Feldbauer , F. -H. Heinsius , T. Held , H. Koch , B. Kopf , M. Pelizaeus , T. Schroeder , M. Steinke , U. Wiedner , J. Zhong , A. Bianconi , M. Bragadireanu , D. Pantea , A. Tudorache , V. Tudorache , M. De Napoli , F. Giacoppo , G. Raciti , E. Rapisarda , C. Sfienti , E. Bialkowski , A. Budzanowski , B. Czech , M. Kistryn , S. Kliczewski , A. Kozela , P. Kulessa , K. Pysz , W. Schaefer , R. Siudak , A. Szczurek , W. Czy. zycki , M. Domagala , M. Hawryluk , E. Lisowski , F. Lisowski , L. Wojnar , D. Gil , P. Hawranek , B. Kamys , St. Kistryn , K. Korcyl , W. Krzemien , A. Magiera , P. Moskal , Z. Rudy , P. Salabura , J. Smyrski , A. Wronska , M. Al-Turany , I. Augustin , H. Deppe , H. Flemming , J. Gerl , K. Goetzen , R. Hohler , D. Lehmann , B. Lewandowski , J. Luehning , F. Maas , D. Mishra , H. Orth , K. Peters , T. Saito , G. Schepers , C. J. Schmidt , L. Schmitt , C. Schwarz , B. Voss , P. Wieczorek , A. Wilms , K. -T. Brinkmann , H. Freiesleben , R. Jaekel , R. Kliemt , T. Wuerschig , H. -G. Zaunick , V. M. Abazov , G. Alexeev , A. Arefiev , V. I. Astakhov , M. Yu. Barabanov , B. V. Batyunya , Yu. I. Davydov , V. Kh. Dodokhov , A. A. Efremov , A. G. Fedunov , A. A. Feshchenko , A. S. Galoyan , S. Grigoryan , A. Karmokov , E. K. Koshurnikov , V. Ch. Kudaev , V. I. Lobanov , Yu. Yu. Lobanov , A. F. Makarov , L. V. Malinina , V. L. Malyshev , G. A. Mustafaev , A. Olshevski , M. A. Pasyuk , E. A. Perevalova , A. A. Piskun , T. A. Pocheptsov , G. Pontecorvo , V. K. Rodionov , Yu. N. Rogov , R. A. Salmin , A. G. Samartsev , M. G. Sapozhnikov , A. Shabratova , G. S. Shabratova , A. N. Skachkova , N. B. Skachkov , E. A. Strokovsky , M. K. Suleimanov , R. Sh. Teshev , V. V. Tokmenin , V. V. Uzhinsky , A. S. Vodopianov , S. A. Zaporozhets , N. I. Zhuravlev , A. G. Zorin , D. Branford , K. Foehl , D. Glazier , D. Watts , P. Woods , W. Eyrich , A. Lehmann , A. Teufel , S. Dobbs , Z. Metreveli , K. Seth , B. Tann , A. Tomaradze , D. Bettoni , V. Carassiti , A. Cecchi , P. Dalpiaz , E. Fioravanti , I. Garzia , M. Negrini , M. Savri`e , G. Stancari , B. Dulach , P. Gianotti , C. Guaraldo , V. Lucherini , E. Pace , A. Bersani , M. Macri , M. Marinelli , R. F. Parodi , I. Brodski , W. Doering , P. Drexler , M. Dueren , Z. Gagyi-Palffy , A. Hayrapetyan , M. Kotulla , W. Kuehn , S. Lange , M. Liu , V. Metag , M. Nanova , R. Novotny , C. Salz , J. Schneider , P. Schoenmeier , R. Schubert , S. Spataro , H. Stenzel , C. Strackbein , M. Thiel , U. Thoering , S. Yang , T. Clarkson , E. Cowie , E. Downie , G. Hill , M. Hoek , D. Ireland , R. Kaiser , T. Keri , I. Lehmann , K. Livingston , S. Lumsden , D. MacGregor , B. McKinnon , M. Murray , D. Protopopescu , G. Rosner , B. Seitz , G. Yang , M. Babai , A. K. Biegun , A. Bubak , E. Guliyev , V. S. Jothi , M. Kavatsyuk , H. Loehner , J. Messchendorp , H. Smit , J. C. van der Weele , F. Garcia , D. -O. Riska , M. Buescher , R. Dosdall , R. Dzhygadlo , A. Gillitzer , D. Grunwald , V. Jha , G. Kemmerling , H. Kleines , A. Lehrach , R. Maier , M. Mertens , H. Ohm , D. Prasuhn , T. Randriamalala , J. Ritman , M. Roeder , T. Stockmanns , P. Wintz , P. Wuestner , J. Kisiel , S. Li , Z. Li , Z. Sun , H. Xu , S. Fissum , K. Hansen , L. Isaksson , M. Lundin , B. Schroeder , P. Achenbach , M. C. Mora Espi , J. Pochodzalla , S. Sanchez , A. Sanchez-Lorente , V. I. Dormenev , A. A. Fedorov , M. V. Korzhik , O. V. Missevitch , V. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , V. Goryachev , A. Boukharov , O. Malyshev , I. Marishev , A. Semenov , C. Hoeppner , B. Ketzer , I. Konorov , A. Mann , S. Neubert , S. Paul , Q. Weitzel , A. Khoukaz , T. Rausmann , A. Taeschner , J. Wessels , R. Varma , E. Baldin , K. Kotov , S. Peleganchuk , Yu. Tikhonov , J. Boucher , T. Hennino , R. Kunne , S. Ong , J. Pouthas , B. Ramstein , P. Rosier , M. Sudol , J. Van de Wiele , T. Zerguerras , K. Dmowski , R. Korzeniewski , D. Przemyslaw , B. Slowinski , G. Boca , A. Braghieri , S. Costanza , A. Fontana , P. Genova , L. Lavezzi , P. Montagna , A. Rotondi , N. I. Belikov , A. M. Davidenko , A. A. Derevschikov , Y. M. Goncharenko , V. N. Grishin , V. A. Kachanov , D. A. Konstantinov , V. A. Kormilitsin , V. I. Kravtsov , Y. A. Matulenko , Y. M. Melnik , A. P. Meschanin , N. G. Minaev , V. V. Mochalov , D. A. Morozov , L. V. Nogach , S. B. Nurushev , A. V. Ryazantsev , P. A. Semenov , L. F. Soloviev , A. V. Uzunian , A. N. Vasiliev , A. E. Yakutin , T. Baeck , B. Cederwall , C. Bargholtz , L. Geren , P. E. Tegner , S. Belostotski , G. Gavrilov , A. Itzotov , A. Kisselev , P. Kravchenko , S. Manaenkov , O. Miklukho , Y. Naryshkin , D. Veretennikov , V. Vikhrov , A. Zhadanov , L. Fava , D. Panzieri , D. Alberto , A. Amoroso , E. Botta , T. Bressani , S. Bufalino , M. P. Bussa , L. Busso , F. De Mori , M. Destefanis , L. Ferrero , A. Grasso , M. Greco , T. Kugathasan , M. Maggiora , S. Marcello , G. Serbanut , S. Sosio , R. Bertini , D. Calvo , S. Coli , P. De Remigis , A. Feliciello , A. Filippi , G. Giraudo , G. Mazza , A. Rivetti , K. Szymanska , F. Tosello , R. Wheadon , O. Morra , M. Agnello , F. Iazzi , K. Szymanska , R. Birsa , F. Bradamante , A. Bressan , A. Martin , H. Clement , C. Ekstroem , H. Calen , S. Grape , B. Hoeistad , T. Johansson , A. Kupsc , P. Marciniewski , E. Thome , J. Zlomanczuk , J. Diaz , A. Ortiz , S. Borsuk , A. Chlopik , Z. Guzik , J. Kopec , T. Kozlowski , D. Melnychuk , M. Plominski , J. Szewinski , K. Traczyk , B. Zwieglinski , P. Buehler , A. Gruber , P. Kienle , J. Marton , E. Widmann , J. Zmeskal , M. F. M. Lutz , B. Pire , O. Scholten , R. Timmermans

There is a strong experimental program searching for massive sterile neutrinos. Here we focus on the heavy regime above the GeV scale, where their existence can be probed in either high-energy colliders or in high-precision facilities. We…

High Energy Physics - Phenomenology · Physics 2024-05-20 Xabier Marcano

Nuclear interactions of antiprotons in atomic states are discussed. The total as well as partial widths for single nucleon capture events are calculated. These are compared to the X-ray and recent single nucleon capture data. The rates of…

High Energy Physics - Phenomenology · Physics 2011-04-15 S. Wycech , R. Smolanczuk

Moving highly-charged ions carry strong electromagnetic fields that act as a field of photons. In collisions at large impact parameters, hadronic interactions are not possible, and the ions interact through photon-ion and photon-photon…

Nuclear Experiment · Physics 2009-07-10 Carlos A. Bertulani , Spencer R. Klein , Joakim Nystrand

We report on a search for elementary particles with charges much smaller than the electron charge using a data sample of proton-proton collisions provided by the CERN Large Hadron Collider in 2018, corresponding to an integrated luminosity…

Collisions of atomic nuclei at relativistic velocities allow to recreate the conditions encountered in neutron stars or in the early universe micro-seconds after the Big Bang. These reactions are performed in today's largest accelerator…

Popular Physics · Physics 2022-01-04 Hannah Vormann , Tom Reichert , Christian Spieles , Jan Steinheimer , Marcus Bleicher

Due to their penetrating nature, electromagnetic probes, i.e., lepton-antilepton pairs (dileptons) and photons are unique tools to gain insight into the nature of the hot and dense medium of strongly-interacting particles created in…

High Energy Physics - Phenomenology · Physics 2015-06-23 H. van Hees , J. Weil , S. Endres , M. Bleicher

A search for new heavy particles that decay into top-quark pairs is performed using data collected from proton-proton collisions at a centre-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The integrated…

High Energy Physics - Experiment · Physics 2018-09-25 ATLAS Collaboration

A search for a heavy neutral lepton N of Majorana nature decaying into a W boson and a charged lepton is performed using the CMS detector at the LHC. The targeted signature consists of three prompt charged leptons in any flavor combination…

High Energy Physics - Experiment · Physics 2018-06-06 CMS Collaboration

Four models are considered which contain heavy leptons beyond the three families of the standard model. Two are fourth-generation extensions of the standard model in which the right-handed heavy leptons are either isosinglets or in an…

High Energy Physics - Phenomenology · Physics 2010-11-01 Paul H. Frampton , Daniel Ng , Marc Sher , Yao Yuan

The recent Auger results suggest that although coincidences of arrival directions with 'nearby' AGN and HiRes discovery of the GZK cut-off indicate protons, the measured longitudinal propagation characteristics indicate heavy nuclei, if the…

High Energy Physics - Phenomenology · Physics 2008-10-30 Tadeusz Wibig

We analyze a thought neutrino oscillation experiment in which neutrinos are produced by electrons colliding with atomic nuclei of a target. The neutrinos are detected by observing charged leptons, which are produced by neutrinos colliding…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. D. Dolgov , L. B. Okun , M. V. Rotaev , M. G. Schepkin

We are at the verge of a new impact from hypernuclear experiments planned or already operative at various laboratories all over the world. The complementary of these different experimental approaches to hypernuclei provides a wide basis for…

Nuclear Experiment · Physics 2015-03-17 Josef Pochodzalla

The number of hydrogen-like atoms produced when heavy nuclei collide is estimated for central collisions at the Relativistic Heavy Ion Collider using the sudden approximation of Baym et al. As first suggested by Schwartz, a simultaneous…

Nuclear Theory · Physics 2009-10-31 Joseph Kapusta , Agnes Mocsy

We consider the high energy advantages, disadvantages and luminosity requirements of hadrons, leptons and photon-photon colliders. Technical problems in obtaining increased energy in each type of machine are presented. The machines relative…

Accelerator Physics · Physics 2008-02-03 R. B. Palmer , J. C. Gallardo

We show that heavy ion collisions at the LHC provide a promising environment to search for new long lived particles in well-motivated New Physics scenarios. One advantage lies in the possibility to operate the main detectors with looser…

High Energy Physics - Phenomenology · Physics 2020-02-25 Marco Drewes , Andrea Giammanco , Jan Hajer , Michele Lucente , Olivier Mattelaer

Nuclei are nearly transparent to each other when they collide at high energy, but the collisions do produce high energy density matter in the central rapidity region where most experimental measurements are made. What happens to the…

Nuclear Theory · Physics 2019-02-11 Ming Li , Joseph I. Kapusta

We demonstrate that next generation high-energy neutrino telescopes may reveal the existence of interactions induced by standard model electroweak instantons. The energy spectrum, the angular distribution, and the quark and lepton…

High Energy Physics - Phenomenology · Physics 2010-04-05 Tao Han , Dan Hooper

We explore the feasibility of detecting heavy neutrinos by the existing facilities of neutrino experiments. A heavy neutrino in the mass range 1 MeV < M < 500 MeV is produced by pion or kaon decay, and decays to charged particles which…

High Energy Physics - Phenomenology · Physics 2015-06-12 Takehiko Asaka , Shintaro Eijima , Atsushi Watanabe

The Large Hadron Collider (LHC) at CERN will provide proton-proton collisions at a centre-of-mass energy of 14 TeV with a design luminosity of 10**34/cm**2/s. The exploitation of the rich physics potential offered by the LHC will be…

High Energy Physics - Experiment · Physics 2007-05-23 Felicitas Pauss , Michael Dittmar