Elastic α transfer in the 16O+12C scattering and its impact on the nuclear rainbow
Elastic 16 O + 12 C scattering is known to exhibit the nuclear rainbow pattern at incident energies E lab ≳ 200 MeV, with the Airy structure of the far-side scattering cross section clearly seen at medium and large angles. Such a rainbow pattern is well described by the deep real optical potential (...
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Published in | The European physical journal. A, Hadrons and nuclei Vol. 57; no. 1 |
---|---|
Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
01.01.2021
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
ISSN | 1434-6001 1434-601X |
DOI | 10.1140/epja/s10050-020-00325-3 |
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Abstract | Elastic
16
O
+
12
C
scattering is known to exhibit the nuclear rainbow pattern at incident energies
E
lab
≳
200
MeV, with the Airy structure of the far-side scattering cross section clearly seen at medium and large angles. Such a rainbow pattern is well described by the deep real optical potential (OP) given by the double-folding model (DFM). At lower energies, the extensive elastic
16
O
+
12
C
scattering data show consistently that the nuclear rainbow pattern at backward angles is deteriorated by an oscillating enhancement of elastic cross section that is difficult to describe in the conventional optical model (OM). Given a significant
α
spectroscopic factor predicted for the dissociation
16
O
→
α
+
12
C by the shell model and
α
-cluster models, the contribution of the elastic
α
transfer (or the core-core exchange) to the elastic
16
O
+
12
C
scattering should not be negligible and is expected to account for the enhanced elastic cross section at backward angles. To reveal the impact of the elastic
α
transfer, a systematic coupled reaction channels analysis of the elastic
16
O
+
12
C
scattering has been performed, with the coupling between the elastic scattering and elastic
α
transfer channels treated explicitly, using the real OP given by the DFM. We found that the elastic
α
transfer enhances the near-side scattering significantly at backward angles, giving rise to an oscillating distortion of the smooth Airy structure. The dynamic polarization of the OP by the coupling between the elastic scattering and elastic
α
transfer channels can be effectively taken into account in the OM calculation by an angular-momentum (or parity) dependent potential added to the imaginary OP, as suggested by Frahn and Hussein 40 years ago. |
---|---|
AbstractList | Elastic 16O+12C scattering is known to exhibit the nuclear rainbow pattern at incident energies Elab≳200 MeV, with the Airy structure of the far-side scattering cross section clearly seen at medium and large angles. Such a rainbow pattern is well described by the deep real optical potential (OP) given by the double-folding model (DFM). At lower energies, the extensive elastic 16O+12C scattering data show consistently that the nuclear rainbow pattern at backward angles is deteriorated by an oscillating enhancement of elastic cross section that is difficult to describe in the conventional optical model (OM). Given a significant α spectroscopic factor predicted for the dissociation 16O→α+12C by the shell model and α-cluster models, the contribution of the elastic α transfer (or the core-core exchange) to the elastic 16O+12C scattering should not be negligible and is expected to account for the enhanced elastic cross section at backward angles. To reveal the impact of the elastic α transfer, a systematic coupled reaction channels analysis of the elastic 16O+12C scattering has been performed, with the coupling between the elastic scattering and elastic α transfer channels treated explicitly, using the real OP given by the DFM. We found that the elastic α transfer enhances the near-side scattering significantly at backward angles, giving rise to an oscillating distortion of the smooth Airy structure. The dynamic polarization of the OP by the coupling between the elastic scattering and elastic α transfer channels can be effectively taken into account in the OM calculation by an angular-momentum (or parity) dependent potential added to the imaginary OP, as suggested by Frahn and Hussein 40 years ago. Elastic 16 O + 12 C scattering is known to exhibit the nuclear rainbow pattern at incident energies E lab ≳ 200 MeV, with the Airy structure of the far-side scattering cross section clearly seen at medium and large angles. Such a rainbow pattern is well described by the deep real optical potential (OP) given by the double-folding model (DFM). At lower energies, the extensive elastic 16 O + 12 C scattering data show consistently that the nuclear rainbow pattern at backward angles is deteriorated by an oscillating enhancement of elastic cross section that is difficult to describe in the conventional optical model (OM). Given a significant α spectroscopic factor predicted for the dissociation 16 O → α + 12 C by the shell model and α -cluster models, the contribution of the elastic α transfer (or the core-core exchange) to the elastic 16 O + 12 C scattering should not be negligible and is expected to account for the enhanced elastic cross section at backward angles. To reveal the impact of the elastic α transfer, a systematic coupled reaction channels analysis of the elastic 16 O + 12 C scattering has been performed, with the coupling between the elastic scattering and elastic α transfer channels treated explicitly, using the real OP given by the DFM. We found that the elastic α transfer enhances the near-side scattering significantly at backward angles, giving rise to an oscillating distortion of the smooth Airy structure. The dynamic polarization of the OP by the coupling between the elastic scattering and elastic α transfer channels can be effectively taken into account in the OM calculation by an angular-momentum (or parity) dependent potential added to the imaginary OP, as suggested by Frahn and Hussein 40 years ago. |
Author | Khoa, Dao T. Phuc, Nguyen Hoang Phuc, Nguyen Tri Toan |
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References_xml | – reference: MoraisMCLichtenthälerRNucl. Phys. A201185712011NuPhA.857....1M – reference: KhoaDTvon OertzenWBohlenHGPhys. Rev. C19944916521994PhRvC..49.1652K – reference: FullerRCPhys. Rev. C19751215611975PhRvC..12.1561F – reference: VillariACCLépine-SzilyAFilhoRLFilhoOPObutiMMOliveiraJMJrAddedNNucl. Phys. A19895016051989NuPhA.501..605V – reference: BrandanMESatchlerGRPhys. Rep.19972851431997PhR...285..143B – reference: MichelFReidemeisterGOhkuboSPhys. Rev. C2001630346202001PhRvC..63c4620M – reference: FrahnWEHusseinMSPhys. Lett.198090B3581980PhLB...90..358F – reference: von OertzenWBohlenHGPhys. Rep.1975191 C1975PhR....19....1V – reference: FrickeSHBrandanMEMcVoyKWPhys. Rev. C1988386821988PhRvC..38..682F – reference: BrandanMEHusseinMSMcVoyKWSatchlerGRComments on Nuclear and Particle Physics1996New YorkGordon and Breach77 – reference: BrandanMESatchlerGRPhys. Lett. B19912563111991PhLB..256..311B – reference: SzilnerSvon OertzenWBasrakZHaasFMilinMEur. Phys. J. A2002132732002EPJA...13..273S – reference: KhoaDTSatchlerGRvon OertzenWPhys. Rev. C1997569541997PhRvC..56..954K – reference: Braun-MunzigerPBaretteJPhys. Rep.1982872091982PhR....87..209B – reference: FrahnWETreaties on Heavy-Ion Science1984New YorkPlenum Press135 – reference: RudchikATEur. Phys. J. A2010442212010EPJA...44..221R – reference: KhoaDTvon OertzenWBohlenHGNuofferFNucl. Phys. A20006723872000NuPhA.672..387K – reference: OgloblinAAKhoaDTKondōYGlukhovYADem’yanovaASRozhkovMVSatchlerGRGoncharovSAPhys. Rev. C19985717971998PhRvC..57.1797O – reference: YamadaTFunakiYMyoTHoriuchiHIkedaKRöpkeGSchuckPTohsakiAPhys. Rev. C2012850343152012PhRvC..85c4315Y – reference: SatchlerGRDirect Nuclear Reactions1983OxfordClarendon – reference: RousselPAlamanosNAugerFBarretteJBerthierBFernandezBPapineauLDoubreHMittigWPhys. Rev. Lett.19855417791985PhRvL..54.1779R – reference: SatchlerGRLoveWGPhys. Rep.1979551831979PhR....55..183S – reference: ThompsonIJNunesFMNuclear Reactions for Astrophysics2009CambridgeCambridge University Press – reference: BrandanMEMenchaca-RochaABuenerdMChauvinJDe SaintignonPDuhamelGLebrumDMartinPPerrinGHostachyJYPhys. Rev. C19863414841986PhRvC..34.1484B – reference: GlukhovYAGoncharovSADemyanovaASOgloblinAARozhkovMVRudakovVPTrashkaVIzv. Ross. Akad. Nauk, Ser. Fiz.200165647 – reference: VolyaATchuvilskyYMPhys. Rev. C2015910443192015PhRvC..91d4319V – reference: MackintoshRSEur. Phys. J. A2019551472019EPJA...55..147M – reference: HamadaSBurtebayevNGridnevKAAmangeldiNNucl. Phys. A2011859292011NuPhA.859...29H – reference: RowleyNDoubreHMartyCPhys. Lett. B1977691471977PhLB...69..147R – reference: J. Raynal, Computing as a Language of Physics (IAEA, Vienna, 1972) p. 75; coupled-channel code ECIS97 (unpublished) – reference: BrinkDMTakigawaNNucl. Phys. A19772791591977NuPhA.279..159B – reference: BrandanMEMenchaca-RochaATracheLClarkHLAzhariAGagliardiCALuiY-WTribbleREVarnerRLBeeneJRSatchlerGRNucl. Phys. A20016886592001NuPhA.688..659B – reference: NicoliMPHaasFFreemanRMSzilnerSBasrakZMorsadASatchlerGRBrandanMEPhys. Rev. C2000610346092000PhRvC..61c4609N – reference: KhoaDTPhucNHLoanDTLocBMPhys. Rev. C2016940346122016PhRvC..94c4612K – reference: ThompsonIJComput. Phys. Rep.198871671988CoPhR...7..167T – reference: OgloblinAAGlukhovYATrzaskaWHDemyanovaASGoncharovSAJulinRKlebnikovSVMuttererMRozhkovMVRudakovVPTiorinGPKhoaDTSatchlerGRPhys. Rev. C2000620446012000PhRvC..62d4601O – reference: GlukhovYARudakovVPArtemovKPDemyanovaASOgloblinAAGoncharovSAIzadpanakhAPhys. At. Nucl.2007701 – reference: HusseinMSMcVoyKWProg. Part. Nucl. Phys.1984121031984PrPNP..12..103H – reference: StiliarisEBohlenHGFröbrichPGebauerBKolbertDvon OertzenWWilpertMWilpertThPhys. Lett. B19892232911989PhLB..223..291S – reference: KhoaDTvon OertzenWBohlenHGOhkuboSJ. Phys. G200734R111 – reference: BrandanMESatchlerGRNucl. Phys. A19884874771988NuPhA.487..477B – reference: PhucNTTPhucNHKhoaDTPhys. Rev. C2018980246132018PhRvC..98b4613P – reference: FrahnWEHusseinMSNucl. Phys. A19803462371980NuPhA.346..237F – reference: OhkuboSHirabayashiYPhys. Rev. C201489051601(R)2014PhRvC..89e1601O – reference: PhucNTTMackintoshRSPhucNHKhoaDTPhys. Rev. C20191000546152019PhRvC.100e4615P |
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Snippet | Elastic
16
O
+
12
C
scattering is known to exhibit the nuclear rainbow pattern at incident energies
E
lab
≳
200
MeV, with the Airy structure of the far-side... Elastic 16O+12C scattering is known to exhibit the nuclear rainbow pattern at incident energies Elab≳200 MeV, with the Airy structure of the far-side... |
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SubjectTerms | Angular momentum Channels Cluster Structure and Dynamics of Nuclei - A Tribute to Mahir Hussein Coupling Elastic scattering Hadrons Heavy Ions Nuclear Fusion Nuclear Physics Particle and Nuclear Physics Physics Physics and Astronomy Rainbows Regular Article – Theoretical Physics Scattering cross sections |
Title | Elastic α transfer in the 16O+12C scattering and its impact on the nuclear rainbow |
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