Microscopic analysis of low-energy spin and orbital magnetic dipole excitations in deformed nuclei
Identifikátory výsledku
Kód výsledku v IS VaVaI
<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F00216208%3A11320%2F21%3A10439384" target="_blank" >RIV/00216208:11320/21:10439384 - isvavai.cz</a>
Výsledek na webu
<a href="https://verso.is.cuni.cz/pub/verso.fpl?fname=obd_publikace_handle&handle=B6_ms~_yRd" target="_blank" >https://verso.is.cuni.cz/pub/verso.fpl?fname=obd_publikace_handle&handle=B6_ms~_yRd</a>
DOI - Digital Object Identifier
<a href="http://dx.doi.org/10.1103/PhysRevC.103.064313" target="_blank" >10.1103/PhysRevC.103.064313</a>
Alternativní jazyky
Jazyk výsledku
angličtina
Název v původním jazyce
Microscopic analysis of low-energy spin and orbital magnetic dipole excitations in deformed nuclei
Popis výsledku v původním jazyce
A low-energy magnetic dipole (M1) spin-scissors resonance (SSR) located just below the ordinary orbital scissors resonance (OSR) was recently predicted in deformed nuclei within the Wigner function moments (WFM) approach. We analyze this prediction using fully self-consistent Skyrme quasiparticle random phase approximation (QRPA) method. Skyrme forces SkM*, SVbas, and SG2 are implemented to explore SSR and OSR in Dy-160,Dy-162,Dy-164 and Th-232. Accuracy of the method is justified by a good description of M1 spin-flip giant resonance. The calculations show that isotopes Dy-160,Dy-162,Dy-164 indeed have at 1.5-2.4 MeV (below OSR) (IK)-K-pi = 1(+)1 states with a large M1 spin strength (K is the projection of the total nuclear moment to the symmetry z axis). These states are almost fully exhausted by pp[411 up arrow, 411 down arrow] and nn[521 up arrow, 521.] spin-flip configurations corresponding to pp[2d(3/2), 2d(5/2)] and nn[2 f(5/2), 2 f(7/2)] structures in the spherical limit. So the predicted SSR is actually reduced to low-orbital (l = 2, 3) spin-flip states. Following our analysis and in contradiction with WFM spin-scissors picture, deformation is not the principle origin of the low-energy spin M1 states but only a factor affecting their features. The spin and orbital strengths are generally mixed and exhibit interference: weakly destructive in SSR range and strongly constructive in OSR range. In Th-232, the M1 spin strength is very small. Two groups of I-pi = 1(+) states observed experimentally at 2.4-4 MeV in Dy-160,Dy-162,Dy-164 and at 2-4 MeV in Th-232 are mainly explained by fragmentation of the orbital strength. Distributions of nuclear currents in QRPA states partly correspond to the isovector orbital-scissors flow but not to the spin-scissors one.
Název v anglickém jazyce
Microscopic analysis of low-energy spin and orbital magnetic dipole excitations in deformed nuclei
Popis výsledku anglicky
A low-energy magnetic dipole (M1) spin-scissors resonance (SSR) located just below the ordinary orbital scissors resonance (OSR) was recently predicted in deformed nuclei within the Wigner function moments (WFM) approach. We analyze this prediction using fully self-consistent Skyrme quasiparticle random phase approximation (QRPA) method. Skyrme forces SkM*, SVbas, and SG2 are implemented to explore SSR and OSR in Dy-160,Dy-162,Dy-164 and Th-232. Accuracy of the method is justified by a good description of M1 spin-flip giant resonance. The calculations show that isotopes Dy-160,Dy-162,Dy-164 indeed have at 1.5-2.4 MeV (below OSR) (IK)-K-pi = 1(+)1 states with a large M1 spin strength (K is the projection of the total nuclear moment to the symmetry z axis). These states are almost fully exhausted by pp[411 up arrow, 411 down arrow] and nn[521 up arrow, 521.] spin-flip configurations corresponding to pp[2d(3/2), 2d(5/2)] and nn[2 f(5/2), 2 f(7/2)] structures in the spherical limit. So the predicted SSR is actually reduced to low-orbital (l = 2, 3) spin-flip states. Following our analysis and in contradiction with WFM spin-scissors picture, deformation is not the principle origin of the low-energy spin M1 states but only a factor affecting their features. The spin and orbital strengths are generally mixed and exhibit interference: weakly destructive in SSR range and strongly constructive in OSR range. In Th-232, the M1 spin strength is very small. Two groups of I-pi = 1(+) states observed experimentally at 2.4-4 MeV in Dy-160,Dy-162,Dy-164 and at 2-4 MeV in Th-232 are mainly explained by fragmentation of the orbital strength. Distributions of nuclear currents in QRPA states partly correspond to the isovector orbital-scissors flow but not to the spin-scissors one.
Klasifikace
Druh
J<sub>imp</sub> - Článek v periodiku v databázi Web of Science
CEP obor
—
OECD FORD obor
10300 - Physical sciences
Návaznosti výsledku
Projekt
<a href="/cs/project/GA19-14048S" target="_blank" >GA19-14048S: Zkoumání nových vlastností jaderných elektromagnetických excitací</a><br>
Návaznosti
P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)
Ostatní
Rok uplatnění
2021
Kód důvěrnosti údajů
S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů
Údaje specifické pro druh výsledku
Název periodika
Physical Review C
ISSN
2469-9985
e-ISSN
—
Svazek periodika
103
Číslo periodika v rámci svazku
6
Stát vydavatele periodika
US - Spojené státy americké
Počet stran výsledku
14
Strana od-do
064313
Kód UT WoS článku
000661755200002
EID výsledku v databázi Scopus
2-s2.0-85108220907