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Related papers: Neutron Knockout on Beams of $^{108,106}$Sn and $^…

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The heaviest N=Z doubly-magic nucleus, $^{100}$Sn, and the neighboring nuclei offer unique opportunities to investigate the properties of nuclear interaction in extreme conditions. In particular, the Cd isotopes are expected to present…

We report on the in-beam gamma spectroscopy of $^{102}$Sn and $^{100}$Cd produced via two-neutron removal from carbon and CH$_2$ targets at about 150 MeV/nucleon beam energy. New transitions assigned to the decay of a second 2$^+$ excited…

Direct reaction techniques are powerful tools to study the single-particle nature of nuclei. Performing direct reactions on short-lived nuclei requires radioactive ion beams produced either via fragmentation or the Isotope Separation OnLine…

The single-particle structure of the $N=27$ isotones provides insights into the shell evolution of neutron-rich nuclei from the doubly-magic $^{48}$Ca toward the drip line. $^{43}$S was studied employing the one-neutron knockout reaction…

For the last few decades, one-nucleon knockout reactions on light composite targets -- $^9$Be or $^{12}$C -- have been extensively used to study the single-particle (s.p.) structure of nuclei far from stability. To determine which…

Nuclear Theory · Physics 2023-11-21 Chloë Hebborn , Pierre Capel

The one-neutron knockout reaction 9Be(57Cr,56Cr + gamma)X has been measured in inverse kinematics with an intermediate-energy beam. Cross sections to individual states in 56Cr were partially untangled through the detection of the…

Cross sections and photon asymmetries of the exclusive 16O(\gamma,pn)14N and 16O(\gamma,pp)14C knockout reactions are calculated for transitions to the low-lying discrete final states of the residual nucleus in the photon-energy range…

Nuclear Theory · Physics 2009-10-31 C. Giusti , F. D. Pacati

One of the main ingredients in nuclear structure studies using shell model are the single-particle energy (spe). In order to obtain these values accurately, experimental data is needed. The region around the doubly magic nuclide 100Sn is…

Nuclear Theory · Physics 2022-07-11 Abderrahmane Yakhelef , Serkan Akkoyun

The region around neutron number N = 60 in the neutron-rich Sr and Zr nuclei is one of the most dramatic examples of a ground state shape transition from (near) spherical below N = 60 to strongly deformed shapes in the heavier isotopes. The…

Our understanding of nuclear properties in the vicinity of $^{100}$Sn, suggested to be the heaviest doubly magic nucleus with equal numbers of protons (Z=50) and neutrons (N=50), has been a long-standing challenge for experimental and…

Simpson and Tostevin proposed that the width and shape of exclusive parallel momentum distributions of the A-2 residue in direct two-nucleon knockout reactions carry a measurable sensitivity to the nucleon single-particle configurations and…

The contributions of short-range nucleon-nucleon correlations, meson exchange current (MEC) corrections and the influence of Delta isobar excitations (isobaric currents, IC) on photon induced two-nucleon knockout reactions are investigated.…

Nuclear Theory · Physics 2007-05-23 D. Knödler , H. Müther

The single-particle structure of $^{57}$Ni and level structure of $^{56}$Ni were investigated with the \mbox{$^{9}$Be ($^{57} $Ni,$^{56}$Ni+$\gamma$)$\it{X}$} reaction at 73 MeV/nucleon. An inclusive cross section of 41.4(12) mb was…

From superconductors to atomic nuclei, strongly-interacting many-body systems are ubiquitous in nature. Measuring the microscopic structure of such systems is a formidable challenge, often met by particle knockout scattering experiments.…

Nuclear Experiment · Physics 2021-06-10 M. Patsyuk , J. Kahlbow , G. Laskaris , M. Duer , V. Lenivenko , E. P. Segarra , T. Atovullaev , G. Johansson , T. Aumann , A. Corsi , O. Hen , M. Kapishin , V. Panin , E. Piasetzky , Kh. Abraamyan , S. Afanasiev , G. Agakishiev , P. Alekseev , E. Atkin , T. Aushev , V. Babkin , V. Balandin , D. Baranov , N. Barbashina , P. Batyuk , S. Bazylev , A. Beck , C. A. Bertulani , D. Blaschke , D. Blau , D. Bogoslovsky , A. Bolozdynya , K. Boretzky , V. Burtsev , M. Buryakov , S. Buzin , A. Chebotov , J. Chen , A. Ciszewski , R. Cruz-Torres , B. Dabrowska , D. Dabrowski A. Dmitriev , A. Dryablov , P. Dulov , D. Egorov , A. Fediunin , I. Filippov , K. Filippov , D. Finogeev , I. Gabdrakhmanov , A. Galavanov , I. Gasparic , O. Gavrischuk , K. Gertsenberger , A. Gillibert , V. Golovatyuk , M. Golubeva , F. Guber , Yu. Ivanova , A. Ivashkin , A. Izvestnyy , S. Kakurin , V. Karjavin , N. Karpushkin , R. Kattabekov , V. Kekelidze , S. Khabarov , Yu. Kiryushin , A. Kisiel , V. Kolesnikov , A. Kolozhvari , Yu. Kopylov , I. Korover , L. Kovachev , A. Kovalenko , Yu. Kovalev , A. Kugler , S. Kuklin , E. Kulish , A. Kuznetsov , E. Ladygin , N. Lashmanov , E. Litvinenko , S. Lobastov , B. Loher , Y. -G. Ma , A. Makankin , A. Maksymchyuk , A. Malakhov , I. Mardor , S. Merts , A. Morozov , S. Morozov , G. Musulmanbekov , R. Nagdasev , D. Nikitin , V. Palchik , D. Peresunko , M. Peryt , O. Petukhov , Yu. Petukhov , S. Piyadin , V. Plotnikov , G. Pokatashkin , Yu. Potrebenikov , O. Rogachevsky , V. Rogov , K. Roslon , D. Rossi , I. Rufanov , P. Rukoyatkin , M. Rumyantsev , D. Sakulin , V. Samsonov , H. Scheit , A. Schmidt , S. Sedykh , I. Selyuzhenkov , P. Senger , S. Sergeev , A. Shchipunov , A. Sheremeteva , M. Shitenkov , V. Shumikhin , A. Shutov , V. Shutov , H. Simon , I. Slepnev , V. Slepnev , I. Slepov , A. Sorin , V. Sosnovtsev , V. Spaskov , T. Starecki , A. Stavinskiy , E. Streletskaya , O. Streltsova , M. Strikhanov , N. Sukhov , D. Suvarieva , J. Tanaka , A. Taranenko , N. Tarasov , O. Tarasov , V. Tarasov , A. Terletsky , O. Teryaev , V. Tcholakov , V. Tikhomirov , A. Timoshenko , N. Topilin , B. Topko , H. Tornqvist , I. Tyapkin , V. Vasendina , A. Vishnevsky , N. Voytishin , V. Wagner , O. Warmusz , I. Yaron , V. Yurevich , N. Zamiatin , Song Zhang , E. Zherebtsova , V. Zhezher , N. Zhigareva , A. Zinchenko , E. Zubarev , M. Zuev

The single-nucleon knockout reactions 9Be(14B, 13B + gamma)X and 197Au(14B, 13B + gamma)X, at an incident energy of 60 MeV per nucleon, have been used to probe the structure of 14B and of the core fragment 13B. A dominant 2s configuration…

Since a long time electron scattering has been envisaged as a powerful and preferential tool to investigate nuclear properties. In particular, the (e,e'p) knockout reaction has provided a wealth of information on the single particle (s.p.)…

Nuclear Theory · Physics 2017-09-29 Carlotta Giusti

We report on the first detailed study of the mechanisms involved in knockout reactions, via a coincidence measurement of the residue and fast proton in one-proton knockout reactions, using the S800 spectrograph in combination with the HiRA…

First experimental evidence of the population of the first 2- state in 16C above the neutron threshold is obtained by neutron knockout from 17C on a hydrogen target. The invariant mass method combined with in-beam gamma-ray detection is…

Neutron-unbound resonant states of 11Be were populated in neutron knock-out reactions from 12Be and identified by 10Be-n coincidence measurements. A resonance in the decay-energy spectrum at 80(2) keV was attributed to a highly excited…

Background: Neutron-rich nuclei around neutron number N = 60 show a dramatic shape transition from spherical ground states to prolate deformation in 98Sr and heavier nuclei. Purpose: The purpose of this study is to investigate the…

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