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NSR database version of April 11, 2024.

Search: Author = J.Vesic

Found 7 matches.

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2022DA06      Phys.Rev. C 105, L031304 (2022)

B.Das, B.Cederwall, C.Qi, M.Gorska, P.H.Regan, O.Aktas, H.M.Albers, A.Banerjee, M.M.R.Chishti, J.Gerl, N.Hubbard, S.Jazrawi, J.Jolie, A.K.Mistry, M.Polettini, A.Yaneva, S.Alhomaidhi, J.Zhao, T.Arici, S.Bagchi, G.Benzoni, P.Boutachkov, T.Davinson, T.Dickel, E.Haettner, O.Hall, Ch.Hornung, J.P.Hucka, P.R.John, I.Kojouharov, R.Knobel, D.Kostyleva, N.Kuzminchuk, I.Mukha, W.R.Plass, B.S.Nara Singh, J.Vasiljevic, S.Pietri, Zs.Podolyak, M.Rudigier, H.Rosch, E.Sahin, H.Schaffner, C.Scheidenberger, F.Schirru, A.Sharma, R.Shearman, Y.Tanaka, J.Vesic, H.Weick, H.J.Wollersheim, U.Ahmed, A.Algora, C.Appleton, J.Benito, A.Blazhev, A.Bracco, A.M.Bruce, M.Brunet, R.Canavan, A.Esmaylzadeh, L.M.Fraile, G.Hafner, H.Heggen, D.Kahl, V.Karayonchev, R.Kern, A.Korgul, G.Kosir, N.Kurz, R.Lozeva, M.Mikolajczuk, P.Napiralla, R.Page, C.M.Petrache, N.Pietralla, J.-M.Regis, P.Ruotsalainen, L.Sexton, V.Sanchez-Temble, M.Si, J.Vilhena, V.Werner, J.Wiederhold, W.Witt, P.J.Woods, G.Zimba

Nature of seniority symmetry breaking in the semimagic nucleus 94Ru

RADIOACTIVITY 95mPd(β+p)[from 9Be(124Xe, F), E=850 MeV/nucleon];measured Eγ, Iγ, Ep, Ip, γγ-coin, pγ-coin. 94Ru; deduced T1/2 of low-lying excited states, B(E2). Comparison to shell-model calculations. Ions were separated with FRS at GSI and implanted in the Advanced Implantation Detector Array (AIDA), composed of three double-sided silicon strip detectors (DSSSDs) situated at the center of the DEcay SPECtroscopy (DESPEC) setup, comprised of a hybrid array of six triple cluster high-purity germanium (HPGe) detectors and 36 LaBr3(Ce) detectors of the FAst TIMing Array (FATIMA).

doi: 10.1103/PhysRevC.105.L031304
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Data from this article have been entered in the XUNDL database. For more information, click here.

2019TI06      Eur.Phys.J. A 55, 137 (2019)

I.Tisma, M.Lipoglavsek, M.Mihovilovic, S.Markelj, M.Vencelj, J.Vesic

Experimental cross section and angular distribution of the 2H(p, γ)3He reaction at Big-Bang nucleosynthesis energies

doi: 10.1140/epja/i2019-12816-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0969.

2017LI33      Phys.Lett. B 773, 553 (2017)

M.Lipoglavsek, S.Markelj, M.Mihovilovic, T.Petrovic, S.Stajner, M.Vencelj, J.Vesic

Observation of electron emission in the nuclear reaction between protons and deuterons

NUCLEAR REACTIONS 2H(p, X)3He, E=260 keV; measured reaction products, Eβ, Iβ, X-rays; deduced electron yields.

doi: 10.1016/j.physletb.2017.09.004
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2015CV01      Appl.Radiat.Isot. 104, 160 (2015)

A.Cvetinovic, A.Likar, M.Lipoglavsek, A.Mihelic, T.Petrovic, J.Vesic, B.Vodenik

Precise measurement of the half-life of 61Cu

RADIOACTIVITY 61Cu(β+), (EC) [from 60Ni(p, γ)]; measured decay products, Eγ, Iγ; deduced T1/2, level energies, J, π. Comparison with theoretical calculations.

doi: 10.1016/j.apradiso.2015.07.005
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Data from this article have been entered in the XUNDL database. For more information, click here.

2015CV02      Phys.Rev. C 92, 065801 (2015)

A.Cvetinovic, M.Lipoglavsek, S.Markelj, J.Vesic

Molecular screening in nuclear reactions

NUCLEAR REACTIONS 1H(7Li, α)4He, E=0.4-2 MeV; 1H(11B, 2α)4He, E=1.79 MeV; 1H(19F, αγ)16O, E=6.47 MeV; measured Eα, Iα, Eγ, Iγ, integrated enhancement factors, γ-ray yields S-factor, resonance strength in different hydrogen-containing targets; deduced electron screening potential.

doi: 10.1103/PhysRevC.92.065801
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2015VE03      Acta Phys.Pol. B46, 467 (2015)

J.Vesic, A.Cvetinovic, T.Petrovic, M.Lipoglavsek

Effect of Electron Screening on Nuclear Reaction Rates

NUCLEAR REACTIONS 2H(p, γ), E=0.24-0.44 MeV; measured reaction products, Eγ, Iγ; deduced σ, lack of sensitivity for the value of the electron screening potential.

doi: 10.5506/APhysPolB.46.467
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2014VE03      Eur.Phys.J. A 50, 153 (2014)

J.Vesic, A.Cvetinovic, M.Lipoglavsek, T.Petrovic

Influence of electronic environment on nuclear reaction rates

NUCLEAR REACTIONS 1H(7Li, α), E=0.34-2.07 MeV; measured reaction products for hydrogen-implanted Ni, Zn, Pt, Pd targets; deduced screening potential, astrophysical S-factor. 55Mn(p, n), (p, γ), E=1500-1595 keV; measured reaction products; deduced thick target γ yield ratio for Mn and MnO targets, neutron number near 1.54 MeV resonance. 115Cd(p, n), E=1560-2600 keV; measured Eγ, Iγ, nγ-coin for Cd and CdO; deduced neutron number per 299 keV γ transition. 51V(p, γ)(p, n), E=700-1600 keV; measured thick target Eγ, Iγ, nγ-coin for V and VO2 targets; deduced ratio of 1434 keV γ yields. 115In(p, n), E=1750-2500 keV; measured neutrons, X-ray, nX-coin for In and In2O3 targets; deduced neutron number per 24 keV X-ray.

doi: 10.1140/epja/i2014-14153-3
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