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Related papers: The Large-Angle Photon Veto System for the NA62 Ex…

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The different data-sorting modes of the phoswich detector array PARIS used for detecting high-energy (4$-$10 MeV) $\gamma$ rays are investigated. The characteristics including time resolution, energy resolution and detection efficiency…

The GERDA experiment searches for neutrinoless double beta ($0\nu\beta\beta$) decay in $^{76}$Ge using an array of high purity germanium (HPGe) detectors immersed in liquid argon (LAr). Phase II of the experiment uses 30 new broad energy…

Instrumentation and Detectors · Physics 2016-08-06 Björn Lehnert

The NA48/2 experiment at CERN collected a large sample of charged kaon decays to final states with multiple charged particles in 2003--2004. A new upper limit on the rate of the lepton number violating decay…

High Energy Physics - Experiment · Physics 2017-03-24 2 collaboration

The NA61/SHINE experiment is a fixed-target, broad acceptance facility at the CERN SPS. This contribution summarizes the most recent results from the strong interactions NA61/SHINE programme and presents news on the detector upgrade in…

Nuclear Experiment · Physics 2022-12-21 Antoni Marcinek

Using the NA48 detector at the CERN SPS, 31 KS->pi0 gamma gamma candidates with an estimated background of 13.7 +- 3.2 events have been observed. This first observation leads to a branching ratio of BR(KS->pi0 gamma gamma) = (4.9 +-…

High Energy Physics - Experiment · Physics 2012-08-27 NA48 Collaboration

The Nab experiment will measure the ratio of the weak axial-vector and vector coupling constants $\lambda=g_A/g_V$ with precision $\delta\lambda/\lambda\sim3\times10^{-4}$ and search for a Fierz term $b_F$ at a level $\Delta b_F<10^{-3}$.…

The NA48/2 Collaboration at CERN has accumulated unprecedented statistics of rare kaon decays in the Ke4 modes: Ke4(+-) ($K^\pm \to \pi^+ \pi^- e^\pm \nu$) and Ke4(00) ($K^\pm \to \pi^0 \pi^0 e^\pm \nu$) with nearly one percent background…

High Energy Physics - Experiment · Physics 2016-08-10 NA48/2 , NA62 Collaborations , : , F. Ambrosino , A. Antonelli , G. Anzivino , R. Arcidiacono , W. Baldini , S. Balev , J. R. Batley , M. Behler , S. Bifani , C. Biino , A. Bizzeti , B. Bloch-Devaux , G. Bocquet , V. Bolotov , F. Bucci , N. Cabibbo , M. Calvetti , N. Cartiglia , A. Ceccucci , P. Cenci , C. Cerri , C. Cheshkov , J. B. Chèze , M. Clemencic , G. Collazuol , F. Costantini , A. Cotta Ramusino , D. Coward , D. Cundy , A. Dabrowski , G. D'Agostini , P. Dalpiaz , C. Damiani , H. Danielsson , M. De Beer , G. Dellacasa , J. Derré , H. Dibon , D. Di Filippo , L. DiLella , N. Doble , V. Duk , J. Engelfried , K. Eppard , V. Falaleev , R. Fantechi , M. Fidecaro , L. Fiorini , M. Fiorini , T. Fonseca Martin , P. L. Frabetti , A. Fucci , S. Gallorini , L. Gatignon , E. Gersabeck , A. Gianoli , S. Giudici , A. Gonidec , E. Goudzovski , S. Goy Lopez , E. Gushchin , B. Hallgren , M. Hita-Hochgesand , M. Holder , P. Hristov , E. Iacopini , E. Imbergamo , M. Jeitler , G. Kalmus , V. Kekelidze , K. Kleinknecht , V. Kozhuharov , W. Kubischta , V. Kurshetsov , G. Lamanna , C. Lazzeroni , M. Lenti , E. Leonardi , L. Litov , D. Madigozhin , A. Maier , I. Mannelli , F. Marchetto , G. Marel , M. Markytan , P. Marouelli , M. Martini , L. Masetti , P. Massarotti , E. Mazzucato , A. Michetti , I. Mikulec , M. Misheva , N. Molokanova , E. Monnier , U. Moosbrugger , C. Morales Morales , M. Moulson , S. Movchan , D. J. Munday , M. Napolitano , A. Nappi , G. Neuhofer , A. Norton , T. Numao , V. Obraztsov , V. Palladino , M. Patel , M. Pepe , A. Peters , F. Petrucci , M. C. Petrucci , B. Peyaud , R. Piandani , M. Piccini , G. Pierazzini , I. Polenkevich , I. Popov , Yu. Potrebenikov , M. Raggi , B. Renk , F. Retière , P. Riedler , A. Romano , P. Rubin , G. Ruggiero , A. Salamon , G. Saracino , M. Savrié , M. Scarpa , V. Semenov , A. Sergi , M. Serra , M. Shieh , S. Shkarovskiy , M. W. Slater , M. Sozzi , T. Spadaro , S. Stoynev , E. Swallow , M. Szleper , M. Valdata-Nappi , P. Valente , B. Vallage , M. Velasco , M. Veltri , S. Venditti , M. Wache , H. Wahl , A. Walker , R. Wanke , L. Widhalm , A. Winhart , R. Winston , M. D. Wood , S. A. Wotton , O. Yushchenko , A. Zinchenko , M. Ziolkowski

A search for heavy neutral lepton ($N$) production in $K^+\to e^+N$ decays using the data sample collected by the NA62 experiment at CERN in 2017--2018 is reported. Upper limits of the extended neutrino mixing matrix element $|U_{e4}|^2$…

High Energy Physics - Experiment · Physics 2020-07-08 NA62 collaboration

Vector-like top partners with electric charge $+2/3$ are predicted in many extensions of the Standard Model and are actively searched for at the LHC through their electroweak decays $T\to Wb$, $Zt$, and $Ht$. More general scenarios,…

High Energy Physics - Phenomenology · Physics 2026-04-16 Mohammad Sahraei , Yasaman Hosseini , Mojtaba Mohammadi Najafabadi

As liquid argon (LAr) detectors are made at progressively larger sizes, accurate models of LAr optical properties become increasingly important for simulating light transport, understanding signals, and developing analyses. The refractive…

Instrumentation and Detectors · Physics 2024-01-04 Shawn Westerdale

High power, relativistic electron beams from energy recovery linacs have great potential to realize new experimental paradigms for pioneering innovation in fundamental and applied research. A major design consideration for this new…

In a sample of 467 million $B\overline B$ pairs collected with the BABAR detector at the PEP-II collider at SLAC we have observed the decay $\overline{B}^0\rightarrow\Lambda_c^+{\overline p} \pi^0$ and measured the branching fraction to be…

High Energy Physics - Experiment · Physics 2014-11-21 The BABAR Collaboration , B. Aubert et al.

A sample of $1.69\times 10^7$ fully reconstructed $\pi^0\to\gamma e^+e^-$ decay candidates collected by the NA48/2 experiment at CERN in 2003--2004 is analysed to search for the dark photon ($A'$) production in the $\pi^0\to\gamma A'$ decay…

High Energy Physics - Experiment · Physics 2015-05-01 2 collaboration

The upcoming operation of the Extra Low ENergy Antiprotons (ELENA) ring at CERN, the upgrade of the anti-proton decelerator (AD), and the installation in the AD hall of an intense slow positron beam with an expected flux of $10^{8}$ e$^+$/s…

Atomic Physics · Physics 2016-09-21 P. Crivelli , D. Cooke , M. W. Heiss

The experimental status of the $K \to \pi \nu \bar{\nu}$ search is presented. The $K \to \pi \nu \bar{\nu}$ decay is sensitive to New Physics because it is theoretically pristine and highly suppressed. The $K_L^0 \to \pi^0 \nu \bar{\nu}$…

High Energy Physics - Experiment · Physics 2022-08-04 Chieh Lin

(ABRIDGED) The Gamma-ray Large Area Space Telescope (GLAST) will measure the spectra of distant extragalactic sources of high energy gamma-rays. GLAST can look for energy dependent propagation effects from such sources as a signal of…

Astrophysics · Physics 2008-11-26 F. W. Stecker

We developed a low-mass and high-efficiency charged particle detector for an experimental study of the rare decay $K_L \rightarrow \pi^0 \nu \bar{\nu}$. The detector is important to suppress the background with charged particles to the…

Instrumentation and Detectors · Physics 2016-02-03 D. Naito , Y. Maeda , N. Kawasaki , T. Masuda , H. Nanjo , T. Nomura , M. Sasaki , N. Sasao , S. Seki , K. Shiomi , Y. Tajima

The NA62 experiment is designed to measure the ultra-rare decay $K^+ \rightarrow \pi^+ \nu \bar{\nu}$ branching ratio with a precision of $\sim 10\%$ at the CERN Super Proton Synchrotron (SPS). The trigger system of NA62 consists in three…

Instrumentation and Detectors · Physics 2018-05-23 Dario Soldi , Stefano Chiozzi

Very-high-energy (VHE) BL Lac spectra extending above $10 \, \rm TeV$ provide a unique opportunity for testing physics beyond the standard model of elementary particle and alternative blazar emission models. We consider the hadron beam, the…

High Energy Astrophysical Phenomena · Physics 2020-01-08 Giorgio Galanti , Fabrizio Tavecchio , Marco Landoni

If neutrinoless double beta decay is discovered, the next natural step would be understanding the lepton number violating physics responsible for it. Several alternatives exist beyond the exchange of light neutrinos. Some of these…

High Energy Physics - Experiment · Physics 2025-06-13 NEXT Collaboration , M. Martínez-Vara , K. Mistry , F. Pompa , B. J. P. Jones , J. Martín-Albo , M. Sorel , C. Adams , H. Almazán , V. Álvarez , B. Aparicio , A. I. Aranburu , L. Arazi , I. J. Arnquist , F. Auria-Luna , S. Ayet , C. D. R. Azevedo , K. Bailey , F. Ballester , M. del Barrio-Torregrosa , A. Bayo , J. M. Benlloch-Rodríguez , F. I. G. M. Borges , A. Brodolin , N. Byrnes , S. Cárcel , A. Castillo , E. Church , L. Cid , C. A. N. Conde , T. Contreras , F. P. Cossío , R. Coupe , E. Dey , G. Díaz , C. Echevarria , M. Elorza , J. Escada , R. Esteve , R. Felkai , L. M. P. Fernandes , P. Ferrario , A. L. Ferreira , F. W. Foss , Z. Freixa , J. García-Barrena , J. J. Gómez-Cadenas , J. W. R. Grocott , R. Guenette , J. Hauptman , C. A. O. Henriques , J. A. Hernando Morata , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , Y. Ifergan , F. Kellerer , L. Larizgoitia , A. Larumbe , P. Lebrun , F. Lopez , N. López-March , R. Madigan , R. D. P. Mano , A. P. Marques , G. Martínez-Lema , R. L. Miller , J. Molina-Canteras , F. Monrabal , C. M. B. Monteiro , F. J. Mora , K. E. Navarro , P. Novella , A. Nuñez , D. R. Nygren , E. Oblak , J. Palacio , B. Palmeiro , A. Para , I. Parmaksiz , A. Pazos , J. Pelegrin , M. Pérez Maneiro , M. Querol , J. Renner , I. Rivilla , C. Rogero , L. Rogers , B. Romeo , C. Romo-Luque , V. San Nacienciano , F. P. Santos , J. M. F. dos Santos , M. Seemann , I. Shomroni , P. A. O. C. Silva , A. Simón , S. R. Soleti , J. Soto-Oton , J. M. R. Teixeira , S. Teruel-Pardo , J. F. Toledo , C. Tonnelé , S. Torelli , J. Torrent , A. Trettin , A. Usón , P. R. G. Valle , J. F. C. A. Veloso , J. Waiton , A. Yubero-Navarro