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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 study transitions between ground and low-energy excited states of heavy ions corresponding to s-d single-electron transitions or s^2-d^2 double-electron transitions. The large nuclear charge Z and significant change in angular momentum…

Atomic Physics · Physics 2011-12-02 J. C. Berengut , V. A. Dzuba , V. V. Flambaum

To explore the structure of the QCD phase diagram in high baryon density domain, several high-energy nuclear collision experiments in a wide range of beam energies are currently performed or planned using many accelerator facilities. In…

Ten years after its discovery at the Tevatron collider, we still know little about the top quark. Its large mass suggests it may play a key role in the mechanism of Electroweak Symmetry Breaking (EWSB), or open a window of sensitivity to…

High Energy Physics - Experiment · Physics 2010-04-22 A. Juste

A comparative analysis of the secondary particles output of the main hadronic interaction packages used in simulations of extensive air showers is presented. Special attention is given to the study of events with very energetic leading…

High Energy Astrophysical Phenomena · Physics 2009-03-24 C. A. Garcia Canal , S. J. Sciutto , T. Tarutina

New experimental research programs in the field of neutrino physics are calling for new detectors with large masses, high energy resolution and good background rejection capabilities. This paper presents a novel hybrid organic/inorganic…

Instrumentation and Detectors · Physics 2018-07-03 S. Wagner , M. Grassi , A. Cabrera

To assess the degree of equilibration of the matter created in heavy-ion reactions at low to intermediate beam energies, a hadronic transport approach (SMASH) is employed. By using a coarse-graining method, we compute the energy momentum…

High Energy Physics - Phenomenology · Physics 2022-09-12 Gabriele Inghirami , Hannah Elfner

The collisional shift of a transition constitutes an important systematic effect in high-precision spectroscopy. Accurate values for van der Waalsinteraction coefficients are required in order to evaluate the distance-dependent frequency…

Atomic Physics · Physics 2017-11-29 U. D. Jentschura , C. M. Adhikari

Comparing the measurements of the hadronic final state from partonic showers in proton-proton and heavy-ion collisions will reveal the modifications generated by the medium on partons produced in hard scatterings. This can be achieved by…

High Energy Physics - Experiment · Physics 2019-08-13 Yaxian Mao

We investigate the potential of future tau neutrino experiments for identifying the $\nu_\tau$ appearance in probing secret neutrino interactions. The reference experiments include the DUNE far detector utilizing the atmospheric data, which…

High Energy Physics - Phenomenology · Physics 2023-11-28 Pouya Bakhti , Meshkat Rajaee , Seodong Shin

We present a model for the metal-insulator transition in 2D, observed in the recent years. Our starting point consists of two ingredients only, which are ubiquitous in the experiments: Coulomb interactions and weak disorder spin-orbit…

Disordered Systems and Neural Networks · Physics 2015-06-24 George Kastrinakis

The Dark Matter Particle Explorer (DAMPE) has made significant progress in measuring the fluxes of cosmic rays. These new measurements are pivotal in advancing our understanding of the origins and propagation mechanisms of cosmic rays. The…

High Energy Physics - Experiment · Physics 2025-09-23 F. Alemanno , Q. An , P. Azzarello , F. C. T. Barbato , P. Bernardini , X. J. Bi , H. Boutin , I. Cagnoli , M. S. Cai , E. Casilli , E. Catanzani , J. Chang , D. Y. Chen , J. L. Chen , Z. F. Chen , Z. X. Chen , P. Coppin , M. Y. Cui , T. S. Cui , Y. X. Cui , I. De Mitri , F. de Palma , A. Di Giovanni , T. K. Dong , Z. X. Dong , G. Donvito , J. L. Duan , K. K. Duan , R. R. Fan , Y. Z. Fan , F. Fang , K. Fang , C. Q. Feng , L. Feng , P. Fusco , M. Gao , F. Gargano , E. Ghose , K. Gong , Y. Z. Gong , D. Y. Guo , J. H. Guo , S. X. Han , Y. M. Hu , G. S. Huang , X. Y. Huang , Y. Y. Huang , M. Ionica , L. Y. Jiang , Y. Z. Jiang , W. Jiang , J. Kong , A. Kotenko , D. Kyratzis , S. J. Lei , M. B. Li , W. H. Li , W. L. Li , X. Li , X. Q. Li , Y. M. Liang , C. M. Liu , H. Liu , J. Liu , S. B. Liu , Y. Liu , F. Loparco , C. N. Luo , M. Ma , P. X. Ma , T. Ma , X. Y. Ma , G. Marsella , M. N. Mazziotta , D. Mo , Y. Nie , X. Y. Niu , A. Parenti , W. X. Peng , X. Y. Peng , C. Perrina , E. Putti-Garcia , R. Qiao , J. N. Rao , Y. Rong , R. Sarkar , P. Savina , A. Serpolla , Z. Shangguan , W. H. Shen , Z. Q. Shen , Z. T. Shen , L. Silveri , J. X. Song , H. Su , M. Su , H. R. Sun , Z. Y. Sun , A. Surdo , X. J. Teng , A. Tykhonov , G. F. Wang , J. Z. Wang , L. G. Wang , S. Wang , X. L. Wang , Y. F. Wang , D. M. Wei , J. J. Wei , Y. F. Wei , D. Wu , J. Wu , S. S. Wu , X. Wu , Z. Q. Xia , Z. Xiong , E. H. Xu , H. T. Xu , J. Xu , Z. H. Xu , Z. L. Xu , Z. Z. Xu , G. F. Xue , H. B. Yang , P. Yang , Y. Q. Yang , H. J. Yao , M. Y. Yan , Y. H. Yu , Q. Yuan , C. Yue , J. J. Zang , S. X. Zhang , W. Z. Zhang , Y. Zhang , Y. Zhang , Y. J. Zhang , Y. L. Zhang , Y. P. Zhang , Y. Q. Zhang , Z. Zhang , Z. Y. Zhang , C. Zhao , H. Y. Zhao , X. F. Zhao , C. Y. Zhou , Y. Zhu

Experiments aimed at direct searches for WIMP dark matter require highly effective reduction of backgrounds and control of any residual radioactive contamination. In particular, neutrons interacting with atomic nuclei represent an important…

Instrumentation and Detectors · Physics 2024-10-15 20k Collaboration , F. Acerbi , P. Adhikari , P. Agnes , I. Ahmad , S. Albergo , I. F. Albuquerque , T. Alexander , A. K. Alton , P. Amaudruz , M. Angiolilli , E. Aprile , R. Ardito , M. Atzori Corona , D. J. Auty , M. Ave , I. C. Avetisov , O. Azzolini , H. O. Back , Z. Balmforth , A. Barrado Olmedo , P. Barrillon , G. Batignani , P. Bhowmick , V. Bocci , W. Bonivento , B. Bottino , M. G. Boulay , A. Buchowicz , S. Bussino , J. Busto , M. Cadeddu , M. Cadoni , R. Calabrese , V. Camillo , A. Caminata , N. Canci , A. Capra , M. Caravati , M. Cárdenas-Montes , N. Cargioli , M. Carlini , A. Castellani , P. Castello , P. Cavalcante , D. Cavallo , S. Cebrian , J. Cela Ruiz , S. Chashin , A. Chepurnov , L. Cifarelli , D. Cintas , M. Citterio , B. Cleveland , Y. Coadou , V. Cocco , D. Colaiuda , E. Conde Vilda , L. Consiglio , B. S. Costa , M. Czubak , S. D'Auria , M. D. Da Rocha Rolo , G. Darbo , S. Davini , S. De Cecco , G. De Guido , G. Dellacasa , A. V. Derbin , A. Devoto , F. Di Capua , A. Di Ludovico , L. Di Noto , P. Di Stefano , L. K. Dias , D. Díaz Mairena , X. Ding , C. Dionisi , G. Dolganov , F. Dordei , V. Dronik , A. Elersich , E. Ellingwood , T. Erjavec , M. Fernandez Diaz , A. Ficorella , G. Fiorillo , P. Franchini , D. Franco , H. Frandini Gatti , E. Frolov , F. Gabriele , D. Gahan , C. Galbiati , G. Galinski , G. Gallina , M. Garbini , P. Garcia Abia , A. Gawdzik , A. Gendotti , A. Ghisi , G. K. Giovanetti , V. Goicoechea Casanueva , A. Gola , L. Grandi , G. Grauso , G. Grilli di Cortona , A. Grobov , M. Gromov , M. Guerzoni , M. Gulino , C. Guo , B. R. Hackett , A. Hallin , A. Hamer , M. Haranczyk , B. Harrop , T. Hessel , S. Hill , S. Horikawa , J. Hu , F. Hubaut , J. Hucker , T. Hugues , E. V. Hungerford , A. Ianni , V. Ippolito , A. Jamil , C. Jillings , R. Keloth , N. Kemmerich , A. Kemp , C. L. Kendziora , M. Kimura , K. Kondo , G. Korga , L. Kotsiopoulou , S. Koulosousas , A. Kubankin , M. Kuss , M. Kuzniak , M. Kuzwa , M. La Commara , M. Lai , E. Le Guirriec , E. Leason , A. Leoni , L. Lidey , M. Lissia , L. Luzzi , O. Lychagina , O. Macfadyen , I. N. Machulin , S. Manecki , I. Manthos , L. Mapelli , A. Marasciulli , S. M. Mari , C. Mariani , J. Maricic , A. Marini , M. Martinez , C. J. Martoff , G. Matteucci , K. Mavrokoridis , A. B. McDonald , J. Mclaughlin , S. Merzi , A. Messina , R. Milincic , S. Minutoli , A. Mitra , A. Moharana , S. Moioli , J. Monroe , E. Moretti , M. Morrocchi , T. Mroz , V. N. Muratova , M. Murphy , M. Murra , C. Muscas , P. Musico , R. Nania , M. Nessi , G. Nieradka , K. Nikolopoulos , E. Nikoloudaki , J. Nowak , K. Olchanski , A. Oleinik , V. Oleynikov , P. Organtini , A. Ortiz de Solórzano , M. Pallavicini , L. Pandola , E. Pantic , E. Paoloni , D. Papi , G. Pastuszak , G. Paternoster , D. Peddis , P. A. Pegoraro , K. Pelczar , L. A. Pellegrini , R. Perez , F. Perotti , V. Pesudo , S. I. Piacentini , N. Pino , G. Plante , A. Pocar , M. Poehlmann , S. Pordes , P. Pralavorio , D. Price , S. Puglia , M. Queiroga Bazetto , F. Ragusa , Y. Ramachers , A. Ramirez , S. Ravinthiran , M. Razeti , A. L. Renshaw , M. Rescigno , F. Retiere , L. P. Rignanese , A. Rivetti , A. Roberts , C. Roberts , G. Rogers , L. Romero , M. Rossi , A. Rubbia , D. Rudik , M. Sabia , S. Sadashivajois , P. Salomone , O. Samoylov , E. Sandford , S. Sanfilippo , D. Santone , R. Santorelli , E. M. Santos , C. Savarese , E. Scapparone , G. Schillaci , F. G. Schuckman , G. Scioli , D. A. Semenov , A. Sheshukov , M. Simeone , P. Skensved , M. D. Skorokhvatov , S. Slimani , O. Smirnov , T. Smirnova , B. Smith , A. Sotnikov , F. Spadoni , M. Spangenberg , R. Stefanizzi , A. Steri , V. Stornelli , S. Stracka , S. Sulis , A. Sung , C. Sunny , Y. Suvorov , A. M. Szelc , O. Taborda , R. Tartaglia , A. Taylor , J. Taylor , S. Tedesco , G. Testera , K. Thieme , A. Thompson , A. Tonazzo , S. Torres-Lara , S. Tosi , A. Tricomi , E. V. Unzhakov , T. J. Vallivilayil , M. Van Uffelen , L. Velazquez-Fernandez , T. Viant , S. Vicini , S. Viel , A. Vishneva , R. B. Vogelaar , J. Vossebeld , B. Vyas , M. Wada , M. B. Walczak , H. Wang , Y. Wang , S. Westerdale , L. Williams , R. Wojaczynski , M. M. Wojcik , M. Wojcik , T. Wright , Y. Xie , C. Yang , J. Yin , A. Zabihi , P. Zakhary , A. Zani , Y. Zhang , T. Zhu , A. Zichichi , G. Zuzel , M. P. Zykova

A second major LHCb detector upgrade will be installed during long shutdown 4 (LS4) of the CERN Large Hadron Collider. The new detector will provide excellent performance for studies of Quantum Chromodynamics at high temperature and…

High Energy Physics - Experiment · Physics 2025-04-01 LHCb collaboration

Recently it was suggested that transient excitonic instability can be realized in optically-pumped two-dimensional (2D) Dirac materials (DMs), such as graphene and topological insulator surface states. Here we discuss the possibility of…

Materials Science · Physics 2018-02-14 Anna Pertsova , Alexander V. Balatsky

I review some important results from RHIC experiments. They were obtained in a unique environment for studying QCD bulk matter at temperatures and densities that surpass the limits where hadrons can exist as individual entities, raising the…

Nuclear Experiment · Physics 2009-01-08 Rachid Nouicer

Heavy Ion Collisions (HIC) represent a unique tool to probe the in-medium nuclear interaction in regions away from saturation and at high nucleon momenta. In this report we present a selection of reaction observables particularly sensitive…

Nuclear Theory · Physics 2008-11-26 M. Di Toro , V. Baran , M. Colonna , G. Ferini , T. Gaitanos , V. Greco , J. Rizzo , H. H. Wolter

We are preparing for an ultra-high resolution x-ray spectroscopy of kaonic atoms using an x-ray spectrometer based on an array of superconducting transition-edge-sensor microcalorimeters developed by NIST. The instrument has excellent…

Instrumentation and Detectors · Physics 2014-03-06 S. Okada , D. A. Bennett , W. B. Doriese , J. W. Fowler , K. D. Irwin , S. Ishimoto , M. Sato , D. R. Schmidt , D. S. Swetz , H. Tatsuno , J. N. Ullom , S. Yamada

The invention of laser immediately enabled us to detect nonlinearities of photon interaction in matter, as manifested for example by Franken et al.'s detection of second harmonic generation and the excitation of the Brillouin forward…

Quantum Physics · Physics 2010-06-24 Kensuke Homma , Dieter Habs , Toshiki Tajima

Recent experimental and theoretical developments have motivated interest in a more detailed exploration of heavy ion collisions in the range sqrt(sNN)=5-15 GeV. In contrast to interactions at the full RHIC energy of sqrt(sNN)=200 GeV, such…

Nuclear Experiment · Physics 2009-11-11 G S F Stephans