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Statements

Subject Item
n2:RIV%2F00216208%3A11320%2F13%3A10191515%21RIV14-MSM-11320___
rdf:type
n17:Vysledek skos:Concept
rdfs:seeAlso
http://dx.doi.org/10.1088/0031-8949/2013/T154/014019
dcterms:description
The toroidal, compression and vortical dipole strength functions in semi- magic Sn-124 (and partly in doubly magic (100),Sn-132) are analyzed within the random-phase-approximation method with the SkT6, SkI3, SLy6, SV-bas and SkM(+) Skyrme forces. The isoscalar (T = 0), isovector (T = 1) and electromagnetic ('elm') channels are considered. Both convection j(c) and magnetization j(m) nuclear currents are taken into account. The calculations basically confirm the previous results obtained for Pb-208 with the force SLy6. In particular, it is shown that the vortical and toroidal strengths are dominated by jc in the T = 0 channel and by jm in the T = 1 and 'elm' channels. The compression strength is always determined by j(c). It is also shown that the 'elm' strength (relevant for the (e,e') reaction) is very similar to the T = 1 one. The toroidal mode resides in the region of the pygmy resonance. So, perhaps, this region embraces both irrotational (pygmy) and vortical (toroidal) flows. The toroidal, compression and vortical dipole strength functions in semi- magic Sn-124 (and partly in doubly magic (100),Sn-132) are analyzed within the random-phase-approximation method with the SkT6, SkI3, SLy6, SV-bas and SkM(+) Skyrme forces. The isoscalar (T = 0), isovector (T = 1) and electromagnetic ('elm') channels are considered. Both convection j(c) and magnetization j(m) nuclear currents are taken into account. The calculations basically confirm the previous results obtained for Pb-208 with the force SLy6. In particular, it is shown that the vortical and toroidal strengths are dominated by jc in the T = 0 channel and by jm in the T = 1 and 'elm' channels. The compression strength is always determined by j(c). It is also shown that the 'elm' strength (relevant for the (e,e') reaction) is very similar to the T = 1 one. The toroidal mode resides in the region of the pygmy resonance. So, perhaps, this region embraces both irrotational (pygmy) and vortical (toroidal) flows.
dcterms:title
Toroidal, compression and vortical dipole strengths in Sn-124 Toroidal, compression and vortical dipole strengths in Sn-124
skos:prefLabel
Toroidal, compression and vortical dipole strengths in Sn-124 Toroidal, compression and vortical dipole strengths in Sn-124
skos:notation
RIV/00216208:11320/13:10191515!RIV14-MSM-11320___
n17:predkladatel
n18:orjk%3A11320
n3:aktivita
n13:Z n13:I
n3:aktivity
I, Z(MSM0021620859)
n3:cisloPeriodika
1
n3:dodaniDat
n4:2014
n3:domaciTvurceVysledku
n9:8940991 n9:8850836
n3:druhVysledku
n21:J
n3:duvernostUdaju
n16:S
n3:entitaPredkladatele
n15:predkladatel
n3:idSjednocenehoVysledku
111295
n3:idVysledku
RIV/00216208:11320/13:10191515
n3:jazykVysledku
n8:eng
n3:klicovaSlova
densities; modes; parametrization; nuclei; giant-resonances; skyrme forces; phase-approximation description
n3:klicoveSlovo
n5:parametrization n5:densities n5:nuclei n5:giant-resonances n5:modes n5:skyrme%20forces n5:phase-approximation%20description
n3:kodStatuVydavatele
SE - Švédské království
n3:kontrolniKodProRIV
[AF4EA7220752]
n3:nazevZdroje
Physica Scripta
n3:obor
n12:BG
n3:pocetDomacichTvurcuVysledku
2
n3:pocetTvurcuVysledku
6
n3:rokUplatneniVysledku
n4:2013
n3:svazekPeriodika
T154
n3:tvurceVysledku
Kleinig, W. Reinhard, P-G Repko, Anton Kvasil, Jan Lo Iudice, N. Nesterenko, V. O.
n3:wos
000319336900019
n3:zamer
n7:MSM0021620859
s:issn
0031-8949
s:numberOfPages
5
n19:doi
10.1088/0031-8949/2013/T154/014019
n11:organizacniJednotka
11320