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The fine-sampling electromagnetic calorimeter prototype has been experimentally tested using the 1-19 GeV/c tagged beams of negatively charged particles at the U70 accelerator at IHEP, Protvino. The energy resolution measured by electrons…

PANDORA, Plasmas for Astrophysics, Nuclear Decays Observation and Radiation for Archaeometry, is planned as a new facility based on a state-of-the-art plasma trap confining energetic plasma for performing interdisciplinary research in the…

Instrumentation and Detectors · Physics 2017-08-02 D. Mascali , A. Musumarra , F. Leone , F. P. Romano , A. Galatà , S. Gammino , C. Massimi

Antiprotonic helium, a neutral exotic three-body system consisting of a helium nucleus, an electron and an antiproton, is being studied at the Antiproton Decelerator of CERN by the ASAUCSA collaboration. Using laser spectroscopy of the…

Atomic Physics · Physics 2007-05-23 Eberhard Widmann

We study the formation of single- and double-$\Lambda$ hypernuclei in antiproton-induced reactions relevant for the forthcoming PANDA experiment at FAIR. We use the Giessen Boltzmann-Uehling-Uhlenbeck (GiBUU) transport model with…

Nuclear Theory · Physics 2015-06-03 T. Gaitanos , A. B. Larionov , H. Lenske , U. Mosel

A large number of high-energy and heavy-ion experiments successfully used Time Projection Chamber (TPC) as central tracker and particle identification detector. However, the performance requirements on TPC for new high-rate particle…

Instrumentation and Detectors · Physics 2013-02-14 M. Poli Lener , M. Bazzi , G. Corradi , C. Curceanu , A. D'Uffizi , C. Paglia , A. Romero Vidal , E. Sbardella , A. Scordo , D. Tagnani , J. Zmeskal

The document describes the physics case of the PAX experiment using polarized antiprotons, which has recently been proposed for the new Facility for Antiprotons and Ions Research (FAIR) at GSI--Darmstadt. Polarized antiprotons provide…

High Energy Physics - Experiment · Physics 2019-08-14 Paolo Lenisa , Frank Rathmann

The detection of exclusive processes induced by antiproton beams in the GeV range at PANDA(FAIR) opens possibilities for testing QCD predictions on the nucleon structure. In particular, the measurement of electromagnetic nucleon form…

High Energy Physics - Phenomenology · Physics 2010-11-18 E. Tomasi-Gustafsson , E. ~A. ~Kuraev , Yu. ~M. ~Bystritskiy

AMANDA (Antarctic Muon And Neutrino Detector Array) is a neutrino telescope built under the southern polar icecap and its scope is to explore the possibility to detect high energy cosmic neutrinos. This should generate insight into the…

Astrophysics · Physics 2019-08-14 Peter Niessen

Two measurements of the energy resolution were performed at MAX-Lab in Lund, Sweden, with an array of 3$\times$3 PbWO4 crystals using a tagged photon beam with energies between 19 and 56 MeV. The crystals were cooled down to -15 and -25…

Nuclear Experiment · Physics 2008-05-08 Sophie Grape

The space-time picture of hadron formation in high-energy collisions with nuclear targets is still poorly known. The tests of hadron formation was suggested for the first stage of SPD running. They will require measuring charged pion and…

Instrumentation and Detectors · Physics 2024-08-22 R. Pandey

We report on the design and characterization of an antiproton deceleration beamline, based on a pulsed drift tube, for the PUMA experiment at the Antimatter Factory at CERN. The design has been tailored to high-voltage (100 kV) and…

Instrumentation and Detectors · Physics 2024-06-04 J. Fischer , A. Schmidt , N. Azaryan , F. Butin , J. Ferreira Somoza , A. Husson , C. Klink , A. Obertelli , M. Schlaich , A. Sinturel , N. Thaus , F. Wienholtz

Fermilab operates the world's most intense antiproton source. Newly proposed experiments can use those antiprotons either parasitically during Tevatron Collider running or after the end of the Tevatron Collider program. For example, the…

High Energy Physics - Experiment · Physics 2019-08-14 Daniel M. Kaplan

The prospects of the future PANDA experiment at FAIR in Darmstadt/Germany in the field of charmonium and charm spectroscopy are discussed.

High Energy Physics - Experiment · Physics 2012-10-18 Marc Pelizaeus

This paper describes the energy scale procedures and germanium detectors performance in the LEGEND-200 experiment, a critical component for the first unblinding in the search for neutrinoless double beta decay. We detail the digital signal…

Instrumentation and Detectors · Physics 2026-05-25 The LEGEND Collaboration , H. Acharya , M. Agostini , A. Alexander , C. Alvarez-Garcia , V. Aures , F. T. Avignone , M. Babicz , W. Bae , M. Balata , A. S. Barabash , P. S. Barbeau , C. J. Barton , L. Baudis , C. Bauer , S. Bellman , E. Bernieri , J. P. Ulloa Beteta , L. Bezrukov , K. H. Bhimani , V. Biancacci , A. Biondi , R. Biondi , E. Blalock , P. Bongratz , S. J. Borden , G. Borghi , F. Borra , B. Bos , A. Boston , G. Botogoske , R. Bouabid , R. Brugnera , T. Bürger , N. Burlac , M. Busch , S. Calgaro , N. Canci , L. Canonica , S. Capra , M. Carminati , R. M. D. Carney , L. Carroll , C. Cattadori , R. Cesarano , Y. -D. Chan , J. R. Chapman , A. Chernogorov , P. -J. Chiu , O. Chkvorets , C. D. Christofferson , A. I. Colon-Rivera , F. Confortini , D. D'Agostino , V. D'Andrea , G. De Gregorio , R. Deckert , J. A. Detwiler , N. Di Marco , F. Di Capua , C. Di Fraia , A. Di Giacinto , D. Di Leo , T. Dixon , K. -M. Dong , A. Drobizhev , G. Duran , Yu. Efremenko , S. R. Elliott , T. Elmikawy , C. H. J. Emmanuel , E. Engelhardt , E. Esch , L. Favilla , M. Febbraro , F. Ferella , R. Feriozzi , D. E. Fields , C. Fiorini , M. Fomina , N. Fuad , R. Gala , A. Galindo-Uribarri , A. Gangapshev , A. Garfagnini , S. Gazzana , A. Geraci , L. Gessler , C. Ghiano , A. Gieb , S. Giri , A. Gogosha , M. Gold , M. P. Green , G. Grünauer , J. Gruszko , I. Guinn , V. E. Guiseppe , Y. Gurov , K. Gusev , B. Hackett , F. Hagemann , M. Haranczyk , F. Henkes , R. Henning , J. Herrera , D. Hervas Aguilar , J. Hinton , R. Hodák , H. F. R. Hoffmann , M. Huber , M. Hult , A. Iorio , U. T. Islek , A. Jany , J. Jochum , D. S. Judson , M. Junker , J. Kaizer , V. Kazalov , M. F. Kidd , T. Kihm , K. Kilgus , A. Klimenko , K. T. Knöpfle , I. Kochanek , O. Kochetov , I. Kontul , V. N. Kornoukhov , A. B. Kowaleswska , P. Krause , H. Krishnamoorthy , V. V. Kuzminov , K. Lang , M. Laubenstein , N. N. P. N. Lay , A. Leder , B. Lehnert , A. Leonhardt , N. Levashko , A. Li , L. Y. Li , Y. -R. Lin , I. Lippi , A. Love , A. Lubashevskiy , B. Lubsandorzhiev , N. Lusardi , B. Majorovits , F. Mamedov , G. G. Marshall , E. L. Martin , R. D. Martin , R. Massarczyk , A. Mazumdar , G. McDowell , D. -M. Mei , M. Menzel , S. Mertens , E. Miller , I. Mirza , M. Misiaszek , M. Morella , B. Morgan , D. Muenstermann , C. J. Nave , M. Neuberger , N. O'Briant , F. Paissan , L. Papp , K. Pelczar , L. Pertoldi , W. Pettus , F. Piastra , M. Pichotta , P. Piseri , A. W. P. Poon , P. P. Povinec , A. Pullia , W. S. Quinn , D. C. Radford , Y. A. Ramachers , A. L. Reine , S. Riboldi , E. Richards , K. Rielage , C. Romo-Luque , B. Rossi , N. Rossi , S. Rozov , N. Rumyantseva , R. Saakyan , S. Sailer , G. Salamanna , F. Salamida , G. Saleh , E. Sanchez Garcia , C. Savarese , D. C. Schaper , J. Schlegel , S. J. Schleich , L. Schlüter , S. Schönert , O. Schulz , A. -K. Schütz , M. Schwarz , M. Schweizer , B. Schwingenheuer , C. Seibt , G. Senatore , A. Serafini , K. Shakhov , E. Shevchik , H. Shi , M. Shirchenko , Y. Shitov , N. Sierig , H. Simgen , F. Šimkovic , S. Simonaitis-Boyd , M. Singh , M. Skorokhvatov , M. Slavíčková , J. A. Solomon , G. Song , A. C. Sousa , A. R. Sreekala , L. Steinhart , I. Štekl , T. Sterr , M. Stommel , R. Stroili , S. A. Sullivan , R. R. Sumathi , K. Szczepaniec , L. Taffarello , D. Tagnani , V. Tretyak , M. Turqueti , E. E. van Nieuwenhuizen , L. J. Varriano , S. Vasilyev , V. Vatsa , C. Vignoli , C. Vogl , I. Wang , A. Warren , J. N. Warren , D. Waters , S. L. Watkins , C. Wiesinger , J. F. Wilkerson , M. Willers , M. Wojcik , D. Xu , E. Yakushev , T. Ye , C. -H. Yu , V. Yumatov , D. Zinatulina , K. Zuber , G. Zuzel

The future accelerator facility for beams of ions and antiprotons at Darmstadt will provide antiproton beams of intensities that are two orders of magnitude higher than currently available. Within the foreseen scheme, antiprotons can be…

Nuclear Experiment · Physics 2015-06-26 E. Widmann

This project exploits charged particles confined as a storage ring beam (proton, deuteron, possibly $^3$He) to search for an intrinsic electric dipole moment (EDM, $\vec d$) aligned along the particle spin axis. Statistical sensitivities…

The EDDA-Detector at the Cooler-Synchrotron COSY/J\"ulich has been operated with an internal CH$_2$ fiber target to measure proton-proton elastic scattering differential cross sections. For the data analysis knowledge of beam parameters,…

The local magnetic field in a Penning-Malmberg trap is found by measuring the temperatures that result when electron plasmas are illuminated by microwaves pulses. Multiple heating resonances are observed as the pulse frequencies are swept.…

Plasma Physics · Physics 2020-03-18 E. D. Hunter , A. Christensen , J. Fajans , T. Friesen , E. Kur , J. S. Wurtele

In the years between 2000 and 2002 several pre-series and series modules of the ATLAS EM barrel and end-cap calorimeter were exposed to electron, photon and pion beams. The performance of the calorimeter with respect to its finely segmented…

Instrumentation and Detectors · Physics 2019-08-14 Roberto Sacco

The measurement of cosmic rays at energies exceeding 100 TeV per nucleon is crucial for enhancing the understanding of high-energy particle propagation and acceleration models in the Galaxy. HERD is a space-borne calorimetric experiment…

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