High-angular-momentum structures in 64Zn

D. Karlgren; R. M. Clark; I. Ragnarsson; C. E. Svensson; D. Ward; R. Wyss; C. Andreoiu; R. A.E. Austin; M. P. Carpenter; M. Cromaz; M. A. Deleplanque; R. M. Diamond; P. Fallon; A. Görgen; R. V.F. Janssens; T. L. Khoo; F. Kondev; G. J. Lane; T. Lauritsen; I. Y. Lee; A. O. Macchiavelli; T. Rodinger; D. Rudolph; D. G. Sarantites; D. Seweryniak; T. Steinhardt; F. S. Stephens; O. Thelen; K. Vetter; J. C. Waddington

doi:10.1103/PhysRevC.69.034330

High-angular-momentum structures in ⁶⁴Zn

D. Karlgren^*, R. M. Clark, I. Ragnarsson, C. E. Svensson, D. Ward, R. Wyss, C. Andreoiu, R. A.E. Austin, M. P. Carpenter, M. Cromaz, M. A. Deleplanque, R. M. Diamond, P. Fallon, A. Görgen, R. V.F. Janssens, T. L. Khoo, F. Kondev, G. J. Lane, T. Lauritsen, I. Y. LeeA. O. Macchiavelli, T. Rodinger, D. Rudolph, D. G. Sarantites, D. Seweryniak, T. Steinhardt, F. S. Stephens, O. Thelen, K. Vetter, J. C. Waddington

^*Corresponding author for this work

Research output: Contribution to journal › Article › peer-review

18 Citations (Scopus)

Abstract

High-angular-momentum states in ⁶⁴Zn were populated in the ⁴⁰Ca( ²⁸Si,4p) reaction at a beam energy of 122 MeV. Evaporated, light, charged particles were identified by the Microball, while γ rays were detected using the Gammasphere array. The main focus of this paper is on two strongly coupled, collective bands. The yrast band, which was previously known, has been linked to lower-lying states establishing the excitation energies and angular momenta of in-band states for the first time. The newly identified excited band decays to the yrast band but firm angular-momentum assignments could not be made. In order to interpret these structures cranked-Nilsson-Strutinsky calculations have been performed. The calculations have been extended to account for the distribution of nucleons within a configuration. The yrast collective band is interpreted as based on the π(f _7/2) ^-1(p _3/2f _5/2) ²(g _9/2) ¹ ^ν(p _3/2f _5/2) ⁴(g _9/2) ² configuration. There are several possible interpretations of the second band but it is difficult to distinguish between the different possibilities.

Original language	English
Article number	034330
Pages (from-to)	034330-1-034330-13
Journal	Physical Review C - Nuclear Physics
Volume	69
Issue number	3
DOIs	https://doi.org/10.1103/PhysRevC.69.034330
Publication status	Published - Mar 2004

Access to Document

10.1103/PhysRevC.69.034330

Cite this

Karlgren, D., Clark, R. M., Ragnarsson, I., Svensson, C. E., Ward, D., Wyss, R., Andreoiu, C., Austin, R. A. E., Carpenter, M. P., Cromaz, M., Deleplanque, M. A., Diamond, R. M., Fallon, P., Görgen, A., Janssens, R. V. F., Khoo, T. L., Kondev, F., Lane, G. J., Lauritsen, T., ... Waddington, J. C. (2004). High-angular-momentum structures in ⁶⁴Zn. Physical Review C - Nuclear Physics, 69(3), 034330-1-034330-13. Article 034330. https://doi.org/10.1103/PhysRevC.69.034330

@article{d8ed2bc929c542cbaae0971b02a20be2,

title = "High-angular-momentum structures in 64Zn",

abstract = "High-angular-momentum states in 64Zn were populated in the 40Ca( 28Si,4p) reaction at a beam energy of 122 MeV. Evaporated, light, charged particles were identified by the Microball, while γ rays were detected using the Gammasphere array. The main focus of this paper is on two strongly coupled, collective bands. The yrast band, which was previously known, has been linked to lower-lying states establishing the excitation energies and angular momenta of in-band states for the first time. The newly identified excited band decays to the yrast band but firm angular-momentum assignments could not be made. In order to interpret these structures cranked-Nilsson-Strutinsky calculations have been performed. The calculations have been extended to account for the distribution of nucleons within a configuration. The yrast collective band is interpreted as based on the π(f 7/2) -1(p 3/2f 5/2) 2(g 9/2) 1 ν(p 3/2f 5/2) 4(g 9/2) 2 configuration. There are several possible interpretations of the second band but it is difficult to distinguish between the different possibilities.",

author = "D. Karlgren and Clark, {R. M.} and I. Ragnarsson and Svensson, {C. E.} and D. Ward and R. Wyss and C. Andreoiu and Austin, {R. A.E.} and Carpenter, {M. P.} and M. Cromaz and Deleplanque, {M. A.} and Diamond, {R. M.} and P. Fallon and A. G{\"o}rgen and Janssens, {R. V.F.} and Khoo, {T. L.} and F. Kondev and Lane, {G. J.} and T. Lauritsen and Lee, {I. Y.} and Macchiavelli, {A. O.} and T. Rodinger and D. Rudolph and Sarantites, {D. G.} and D. Seweryniak and T. Steinhardt and Stephens, {F. S.} and O. Thelen and K. Vetter and Waddington, {J. C.}",

year = "2004",

month = mar,

doi = "10.1103/PhysRevC.69.034330",

language = "English",

volume = "69",

pages = "034330--1--034330--13",

journal = "Physical Review C - Nuclear Physics",

issn = "0556-2813",

publisher = "American Physical Society",

number = "3",

}

Karlgren, D, Clark, RM, Ragnarsson, I, Svensson, CE, Ward, D, Wyss, R, Andreoiu, C, Austin, RAE, Carpenter, MP, Cromaz, M, Deleplanque, MA, Diamond, RM, Fallon, P, Görgen, A, Janssens, RVF, Khoo, TL, Kondev, F, Lane, GJ, Lauritsen, T, Lee, IY, Macchiavelli, AO, Rodinger, T, Rudolph, D, Sarantites, DG, Seweryniak, D, Steinhardt, T, Stephens, FS, Thelen, O, Vetter, K & Waddington, JC 2004, 'High-angular-momentum structures in ⁶⁴Zn', Physical Review C - Nuclear Physics, vol. 69, no. 3, 034330, pp. 034330-1-034330-13. https://doi.org/10.1103/PhysRevC.69.034330

TY - JOUR

T1 - High-angular-momentum structures in 64Zn

AU - Karlgren, D.

AU - Clark, R. M.

AU - Ragnarsson, I.

AU - Svensson, C. E.

AU - Ward, D.

AU - Wyss, R.

AU - Andreoiu, C.

AU - Austin, R. A.E.

AU - Carpenter, M. P.

AU - Cromaz, M.

AU - Deleplanque, M. A.

AU - Diamond, R. M.

AU - Fallon, P.

AU - Görgen, A.

AU - Janssens, R. V.F.

AU - Khoo, T. L.

AU - Kondev, F.

AU - Lane, G. J.

AU - Lauritsen, T.

AU - Lee, I. Y.

AU - Macchiavelli, A. O.

AU - Rodinger, T.

AU - Rudolph, D.

AU - Sarantites, D. G.

AU - Seweryniak, D.

AU - Steinhardt, T.

AU - Stephens, F. S.

AU - Thelen, O.

AU - Vetter, K.

AU - Waddington, J. C.

PY - 2004/3

Y1 - 2004/3

N2 - High-angular-momentum states in 64Zn were populated in the 40Ca( 28Si,4p) reaction at a beam energy of 122 MeV. Evaporated, light, charged particles were identified by the Microball, while γ rays were detected using the Gammasphere array. The main focus of this paper is on two strongly coupled, collective bands. The yrast band, which was previously known, has been linked to lower-lying states establishing the excitation energies and angular momenta of in-band states for the first time. The newly identified excited band decays to the yrast band but firm angular-momentum assignments could not be made. In order to interpret these structures cranked-Nilsson-Strutinsky calculations have been performed. The calculations have been extended to account for the distribution of nucleons within a configuration. The yrast collective band is interpreted as based on the π(f 7/2) -1(p 3/2f 5/2) 2(g 9/2) 1 ν(p 3/2f 5/2) 4(g 9/2) 2 configuration. There are several possible interpretations of the second band but it is difficult to distinguish between the different possibilities.

AB - High-angular-momentum states in 64Zn were populated in the 40Ca( 28Si,4p) reaction at a beam energy of 122 MeV. Evaporated, light, charged particles were identified by the Microball, while γ rays were detected using the Gammasphere array. The main focus of this paper is on two strongly coupled, collective bands. The yrast band, which was previously known, has been linked to lower-lying states establishing the excitation energies and angular momenta of in-band states for the first time. The newly identified excited band decays to the yrast band but firm angular-momentum assignments could not be made. In order to interpret these structures cranked-Nilsson-Strutinsky calculations have been performed. The calculations have been extended to account for the distribution of nucleons within a configuration. The yrast collective band is interpreted as based on the π(f 7/2) -1(p 3/2f 5/2) 2(g 9/2) 1 ν(p 3/2f 5/2) 4(g 9/2) 2 configuration. There are several possible interpretations of the second band but it is difficult to distinguish between the different possibilities.

UR - http://www.scopus.com/inward/record.url?scp=84862371396&partnerID=8YFLogxK

U2 - 10.1103/PhysRevC.69.034330

DO - 10.1103/PhysRevC.69.034330

M3 - Article

SN - 0556-2813

VL - 69

SP - 034330-1-034330-13

JO - Physical Review C - Nuclear Physics

JF - Physical Review C - Nuclear Physics

IS - 3

M1 - 034330

ER -

High-angular-momentum structures in ⁶⁴Zn

Abstract

Access to Document

Other files and links

Fingerprint

Cite this