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Sökning: WFRF:(Fülöp Zs.) > (2015-2019) > Resonance strengths...

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FältnamnIndikatorerMetadata
00004047naa a2200421 4500
001oai:DiVA.org:ltu-75596
003SwePub
008190820s2019 | |||||||||||000 ||eng|
024a https://urn.kb.se/resolve?urn=urn:nbn:se:ltu:diva-755962 URI
024a https://doi.org/10.1103/PhysRevC.100.0158052 DOI
040 a (SwePub)ltu
041 a engb eng
042 9 SwePub
072 7a ref2 swepub-contenttype
072 7a art2 swepub-publicationtype
100a Gyürky, Gy.u Institute for Nuclear Research (Atomki), Debrecen, Hungary4 aut
2451 0a Resonance strengths in the 14N( p,γ)15O astrophysical key reaction measured with activation
264 1b American Physical Society,c 2019
338 a print2 rdacarrier
500 a Validerad;2019;Nivå 2;2019-08-20 (johcin)
520 a Background: The 14N(p,γ)15O reaction plays a vital role in various astrophysical scenarios. Its reaction rate must be accurately known in the present era of high precision astrophysics. The cross section of the reaction is often measured relative to a low energy resonance, the strength of which must therefore be determined precisely.Purpose: The activation method, based on the measurement of 15O decay, has not been used in modern measurements of the 14N(p,γ)15O reaction. The aim of the present work is to provide strength data for two resonances in the 14N(p,γ)15O reaction using the activation method. The obtained values are largely independent from previous data measured by in-beam γ spectroscopy and are free from some of their systematic uncertainties.Method: Solid state TiN targets were irradiated with a proton beam provided by the Tandetron accelerator of Atomki using a cyclic activation. The decay of the produced 15O isotopes was measured by detecting the 511 keV positron annihilation γ rays.Results: The strength of the Ep=278keV resonance was measured to be ωγ278=(13.4±0.8)meVwhile for the Ep=1058keV resonance ωγ1058=(442±27)meV.Conclusions: The obtained Ep=278 keV resonance strength is in fair agreement with the values recommended by two recent works. However, the Ep=1058keV resonance strength is about 20% higher than the previous value. The discrepancy may be caused in part by a previously neglected finite target thickness correction. As only the low energy resonance is used as a normalization point for cross section measurements, the calculated astrophysical reaction rate of the 14N(p,γ)15O reaction and therefore the astrophysical consequences are not changed by the present results.
650 7a NATURVETENSKAPx Fysikx Annan fysik0 (SwePub)103992 hsv//swe
650 7a NATURAL SCIENCESx Physical Sciencesx Other Physics Topics0 (SwePub)103992 hsv//eng
653 a Experimentell fysik
653 a Experimental Physics
700a Halász, Z.u Institute for Nuclear Research (Atomki), Debrecen, Hungary4 aut
700a Kiss, G.Gu Institute for Nuclear Research (Atomki), Debrecen, Hungary4 aut
700a Szücs, T.u Institute for Nuclear Research (Atomki), Debrecen, Hungary4 aut
700a Csík, A.u Institute for Nuclear Research (Atomki), Debrecen, Hungary4 aut
700a Török, Zs.u Institute for Nuclear Research (Atomki), Debrecen, Hungary4 aut
700a Huszánk, R.u Institute for Nuclear Research (Atomki), Debrecen, Hungary4 aut
700a Gilzad Kohan, Mojtabau Luleå tekniska universitet,Materialvetenskap4 aut0 (Swepub:ltu)mojgil
700a Wagner, L.u Helmholtz-Zentrum Dresden-Rossendorf (HZDR), Dresden, Germany. Technische Universität Dresden, Dresden, Germany4 aut
700a Fülöp, Zs.u Institute for Nuclear Research (Atomki), Debrecen, Hungary4 aut
710a Institute for Nuclear Research (Atomki), Debrecen, Hungaryb Materialvetenskap4 org
773t Physical Review Cd : American Physical Societyg 100:1q 100:1x 2469-9985x 2469-9993
8564 8u https://urn.kb.se/resolve?urn=urn:nbn:se:ltu:diva-75596
8564 8u https://doi.org/10.1103/PhysRevC.100.015805

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