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Low-lying electric-dipole ($E1$) strength of a neutron-rich nucleus contains information on neutron-skin thickness, deformation, and shell evolution. We discuss the possibility of making use of total reaction cross sections on $^{40}$Ca,…

Nuclear Theory · Physics 2017-09-13 W. Horiuchi , S. Hatakeyama , S. Ebata , Y. Suzuki

The energy spectra of light-mass kaonic nuclei were investigated using the theoretical framework of the $0s$-orbital model with zero-range $\bar{K} N$ and $\bar{K}\bar{K}$ interactions of effective single-channel real potentials. The…

Nuclear Theory · Physics 2021-06-30 Yoshiko Kanada-En'yo

The interplay between the $^{22}$Ne$(\alpha,\gamma)^{26}$Mg and the competing $^{22}$Ne$(\alpha,n)^{25}$Mg reactions determines the efficiency of the latter as a neutron source at the temperatures of stellar helium burning. In both cases,…

Light $s$-shell hypernuclei ($^{3,4}_{\Lambda}\text{H}$) and their ground-state properties are crucial benchmarks in hypernuclear physics. In particular, comparing the production cross sections of $^{3}_{\Lambda}\text{H}$ and…

The experiment E97-006 was performed at Jefferson Lab to measure the momentum and energy distribution of protons in the nucleus far from the region of the (approximate) validity of the mean field description, i.e. at high momentum and…

Nuclear Experiment · Physics 2014-11-18 Daniela Rohe

A Skyrme-type effective potential is determined to describe the interaction between $\Lambda$ hyperons in nuclear medium. Experimental data of the binding energies of the double-$\Lambda$ ($\Lambda\Lambda$) nuclei with mass numbers…

Nuclear Theory · Physics 2023-09-06 Soonchul Choi , Emiko Hiyama , Chang Ho Hyun , Myung-Ki Cheoun

Photon-nuclear reaction in a transport model frame, namely an Extended Quantum Molecular Dynamics (EQMD) model, has been realised at the photon energy of 70-140 MeV in the quasi-deuteron (QD) regime. For an important application, we pay a…

Nuclear Theory · Physics 2018-03-22 B. S. Huang , Y. G. Ma , W. B. He

In an emulsion-counter hybrid experiment performed at J-PARC, a $\Xi^-$ absorption event was observed which decayed into twin single-$\Lambda$ hypernuclei. Kinematic calculations enabled a unique identification of the reaction process as…

We have revisited the possible existence and the binding mechanism of heavy hyperhydrogen 6^H_Lambda. This Lambda hypernucleus is enriched in information about Lambda hypernuclear dynamics which would shed a light on significant role of…

Nuclear Theory · Physics 2012-11-27 Theingi , Khin Swe Myint , Y. Akaishi

Neutron spectra from the reaction $K^-+d\rightarrow \pi+\Sigma+n$ were calculated in the energy range $E^{cm}_{K^-}= 0-50\ MeV$ using coupled channel Faddeev equations for the description of the $\bar KNN-\pi\Sigma N$ three-body system. The…

Nuclear Theory · Physics 2013-03-11 János Révai

In experimental nuclear physics (NP), high-precision electromagnetic calorimetry typically requires a good energy resolution and linear photosensor response on the level of (1-2)% over a full dynamic range of the detector. The beam of…

Instrumentation and Detectors · Physics 2025-10-22 Vladimir V. Berdnikov , Alexander Somov

We extend the microscopic particle-rotor model for hypernuclear low-lying states by including the derivative and tensor coupling terms in the point-coupling nucleon-$\Lambda$ particle ($N\Lambda$) interaction. Taking $^{13}_{~\Lambda}$C as…

Nuclear Theory · Physics 2016-05-04 H. Mei , K. Hagino , J. M. Yao , T. Motoba

We theoretically analyze the $K^{-} {}^{3} \text{He} \to \Lambda p n$ reaction for the $\bar{K} N N$ bound-state search in the J-PARC E15 experiment. We find that, by detecting a fast and forward neutron in the final state, an almost…

Nuclear Theory · Physics 2018-02-21 Takayasu Sekihara , Eulogio Oset , Angels Ramos

A theoretical investigation is done to clarify the origin of the peak structure observed near the $K^{-} p p$ threshold in the in-flight ${}^{3}\text{He} ( K^{-}, \, \Lambda p ) n$ reaction of the J-PARC E15 experiment, which could be a…

High Energy Physics - Phenomenology · Physics 2019-12-06 Takayasu Sekihara , Eulogio Oset , Angels Ramos

The $^7$Li(p,n)$^7$Be reaction is widely used as neutron source for neutron induced reaction cross section measurements, and for $^7$Be radioactive source production. There are two prominent structures in the excitation function, a narrow…

Nuclear Experiment · Physics 2023-11-06 Á. Tóth , Gy. Gyürky , E. Papp , T. Szücs

The existing Nuclear Resonance Fluorescence (NRF) setup at the HI{\gamma}S facility at the Triangle Universities Nuclear Laboratory at Duke University has been extended in order to perform {\gamma}-{\gamma} coincidence experiments. The new…

Following the completion of the second neutron beam line and the related experimental area (EAR2) at the n_TOF spallation neutron source at CERN, several experiments were planned and performed. The high instantaneous neutron flux available…

Instrumentation and Detectors · Physics 2018-03-14 M. Barbagallo , J. Andrzejewski , M. Mastromarco , J. Perkowski , L. A. Damone , A. Gawlik , L. Cosentino , P. Finocchiaro , E. A. Maugeri , A. Mazzone , R. Dressler , S. Heinitz , N. Kivel , D. Schumann , N. Colonna , O. Aberle , S. Amaducci , L. Audouin , M. Bacak , J. Balibrea , F. Bečvář , G. Bellia , E. Berthoumieux , J. Billowes , D. Bosnar , A. Brown , M. Caamaño , F. Calviño , M. Calviani , D. Cano-Ott , R. Cardella , A. Casanovas , F. Cerutti , Y. H. Chen , E. Chiaveri , G. Cortés , M. A. Cortés-Giraldo , S. Cristallo , M. Diakaki , M. Dietz , C. Domingo-Pardo , E. Dupont , I. Durán , B. Fernández-Domínguez , A. Ferrari , P. Ferreira , V. Furman , K. Göbel , A. R. García , S. Gilardoni , T. Glodariu , I. F. Gonçalves , E. González-Romero , E. Griesmayer , C. Guerrero , F. Gunsing , H. Harada , J. Heyse , D. G. Jenkins , E. Jericha , K. Johnston , F. Käppeler , Y. Kadi , A. Kalamara , P. Kavrigin , A. Kimura , M. Kokkoris , M. Krtička , D. Kurtulgil , C. Lederer , H. Leeb , J. Lerendegui-Marco , S. Lo Meo , S. J. Lonsdale , D. Macina , A. Manna , J. Marganiec , T. Martínez , J. G. Martins-Correia , A. Masi , C. Massimi , P. Mastinu , E. Mendoza , A. Mengoni , P. M. Milazzo , F. Mingrone , A. Musumarra , A. Negret , R. Nolte , A. Oprea , A. D. Pappalardo , N. Patronis , A. Pavlik , M. Piscopo , I. Porras , J. Praena , J. M. Quesada , D. Radeck , T. Rauscher , R. Reifarth , M. S. Robles , C. Rubbia , J. A. Ryan , M. Sabaté-Gilarte , A. Saxena , J. Schell , P. Schillebeeckx , P. Sedyshev , A. G. Smith , N. V. Sosnin , A. Stamatopoulos , G. Tagliente , J. L. Tain , A. Tarifeño-Saldivia , L. Tassan-Got , S. Valenta , G. Vannini , V. Variale , P. Vaz , A. Ventura , V. Vlachoudis , R. Vlastou , A. Wallner , S. Warren , C. Weiss , P. J. Woods , T. Wright , P. Žugec

The newly built second experimental area EAR2 of the n_TOF spallation neutron source at CERN allows to perform (n, charged particles) experiments on short-lived highly radioactive targets. This paper describes a detection apparatus and the…

Instrumentation and Detectors · Physics 2016-06-01 L. Cosentino , A. Musumarra , M. Barbagallo , A. Pappalardo , N. Colonna , L. Damone , M. Piscopo , P. Finocchiaro , E. Maugeri , S. Heinitz , D. Schumann , R. Dressler , N. Kivel , O. Aberle , J. Andrzejewski , L. Audouin , M. Ayranov , M. Bacak , S. Barros , J. Balibrea-Correa , V. Beecares , F. Becvar , C. Beinrucker , E. Berthoumieux , J. Billowes , D. Bosnar , M. Brugger , M. Caamano , M. Calviani , F. Calvino , D. Cano-Ott , R. Cardella , A. Casanovas , D. M. Castelluccio , F. Cerutti , Y. H. Chen , E. Chiaveri , G. Cortes , M. A. Cortes-Giraldo , M. Diakaki , C. Domingo-Pardo , E. Dupont , I. Duran , B. Fernandez-Dominguez , A. Ferrari , P. Ferreira , W. Furman , S. Ganesan , A. Garcia-Rios , A. Gawlik , I. Gheorghe , T. Glodariu , K. Goebel , I. F. Goncalves , E. Gonzalez-Romero , E. Griesmayer , C. Guerrero , F. Gunsing , H. Harada , T. Heftrich , J. Heyse , D. G. Jenkins , E. Jericha , F. Kaeppeler , T. Katabuchi , P. Kavrigin , A. Kimura , M. Kokkoris , M. Krticka , E. Leal-Chidonca , J. Lerendegui , C. Lederer , H. Leeb , S. Lo Meo , S. Lonsdale , R. Losito , D. Macina , J. Marganiec , T. Martinez , C. Massimi , P. Mastinu , M. Mastromarco , F. Matteucci , A. Mazzone , E. Mendoza , A. Mengoni , P. M. Milazzo , F. Mingrone , M. Mirea , S. Montesano , R. Nolte , A. Oprea , N. Patronis , A. Pavlik , J. Perkowski , J. Praena , J. Quesada , K. Rajeev , T. Rauscher , R. Reifarth , A. Riego-Perez , P. Rout , C. Rubbia , J. Ryan , M. Sabate-Gilarte , A. Saxena , P. Schillebeeckx , S. Schmidt , P. Sedyshev , A. Stamatopoulos , G. Tagliente , J. L. Tain , A. Tarifeno-Saldivia , L. Tassan-Got , A. Tsinganis , S. Valenta , G. Vannini , V. Variale , P. Vaz , A. Ventura , V. Vlachoudis , R. Vlastou , J. Vollaire , A. Wallner , S. Warren , M. Weigand , C. Weiß , C. Wolf , P. J. Woods , T. Wright , P. Zugec , n_TOF collaboration

At the Mainz Microtron MAMI, the first high-resolution pion spectroscopy from decays of strange systems was performed by electron scattering off a Be-9 target in order to study the ground-state masses of Lambda-hypernuclei. Positively…

Big bang nucleosynthesis provides the earliest probe of standard model physics, at a time when the universe was less than a thousand seconds old. It determines the abundances of the lightest nuclides, which give rise to the subsequent…

Cosmology and Nongalactic Astrophysics · Physics 2020-05-27 Rafael S. de Souza , Tan Hong Kiat , Alain Coc , Christian Iliadis
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