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Simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopes
Background: The mercury isotopes around <math><mrow><mi>N</mi><mo>=</mo><mn>104</mn></mrow></math> are a well-known example of nuclei exhibiting shape coexistence. Mixing of configurations can be studied by measuring the monopole strength &...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2023
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevC.108.014308 http://cds.cern.ch/record/2866156 |
_version_ | 1780978081992802304 |
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author | Stryjczyk, M. Andel, B. Cubiss, J.G. Rezynkina, K. Rodríguez, T.R. García-Ramos, J.E. Andreyev, A.N. Pakarinen, J. Van Duppen, P. Antalic, S. Berry, T. Borge, M.J.G. Clisu, C. Cox, D.M. De Witte, H. Fraile, L.M. Fynbo, H.O.U. Gaffney, L.P. Harkness-Brennan, L.J. Huyse, M. Illana, A. Judson, D.S. Konki, J. Kurcewicz, J. Lazarus, I. Lica, R. Madurga, M. Marginean, N. Marginean, R. Mihai, C. Mosat, P. Nacher, E. Negret, A. Ojala, J. Ovejas, J.D. Page, R.D. Papadakis, P. Pascu, S. Perea, A. Podolyák, Zs. Próchniak, L. Pucknell, V. Rapisarda, E. Rotaru, F. Sotty, C. Tengblad, O. Vedia, V. Viñals, S. Wadsworth, R. Warr, N. Wrzosek-Lipska, K. |
author_facet | Stryjczyk, M. Andel, B. Cubiss, J.G. Rezynkina, K. Rodríguez, T.R. García-Ramos, J.E. Andreyev, A.N. Pakarinen, J. Van Duppen, P. Antalic, S. Berry, T. Borge, M.J.G. Clisu, C. Cox, D.M. De Witte, H. Fraile, L.M. Fynbo, H.O.U. Gaffney, L.P. Harkness-Brennan, L.J. Huyse, M. Illana, A. Judson, D.S. Konki, J. Kurcewicz, J. Lazarus, I. Lica, R. Madurga, M. Marginean, N. Marginean, R. Mihai, C. Mosat, P. Nacher, E. Negret, A. Ojala, J. Ovejas, J.D. Page, R.D. Papadakis, P. Pascu, S. Perea, A. Podolyák, Zs. Próchniak, L. Pucknell, V. Rapisarda, E. Rotaru, F. Sotty, C. Tengblad, O. Vedia, V. Viñals, S. Wadsworth, R. Warr, N. Wrzosek-Lipska, K. |
author_sort | Stryjczyk, M. |
collection | CERN |
description | Background: The mercury isotopes around <math><mrow><mi>N</mi><mo>=</mo><mn>104</mn></mrow></math> are a well-known example of nuclei exhibiting shape coexistence. Mixing of configurations can be studied by measuring the monopole strength <math><mrow><msup><mi>ρ</mi><mn>2</mn></msup><mrow><mo>(</mo><mi>E</mi><mn>0</mn><mo>)</mo></mrow></mrow></math>, however, currently the experimental information is scarce and lacks precision, especially for the <math><mrow><msup><mi>I</mi><mi>π</mi></msup><mo>→</mo><msup><mi>I</mi><mi>π</mi></msup></mrow></math> (<math><mrow><mi>I</mi><mo>≠</mo><mn>0</mn></mrow></math>) transitions.
Purpose: The goals of this study were to increase the precision of the known branching ratios and internal conversion coefficients, to increase the amount of available information regarding excited states in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math>, and to interpret the results in the framework of shape coexistence using different models.
Method: The low-energy structures in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> were populated in the <math><mi>β</mi></math> decay of <math><mmultiscripts><mi>Tl</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math>, produced at ISOLDE, CERN and purified by laser ionization and mass separation. The <math><mi>γ</mi></math>-ray and internal conversion electron events were detected by five germanium clover detectors and a segmented silicon detector, respectively, and correlated in time to build decay schemes.
Results: In total, 193, 178, and 156 transitions, including 144, 140, and 108 observed for the first time in a <math><mi>β</mi></math>-decay experiment, were assigned to <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math>, respectively. Internal conversion coefficients were determined for 23 transitions, out of which 12 had an <math><mrow><mi>E</mi><mn>0</mn></mrow></math> component. Extracted branching ratios allowed the sign of the interference term in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mn>182</mn></mmultiscripts></math> as well as <math><mrow><msup><mi>ρ</mi><mn>2</mn></msup><mrow><mo>(</mo><mi>E</mi><mn>0</mn><mo>;</mo><msubsup><mn>0</mn><mn>2</mn><mo>+</mo></msubsup><mo>→</mo><msubsup><mn>0</mn><mn>1</mn><mo>+</mo></msubsup><mo>)</mo></mrow></mrow></math> and <math><mrow><mi>B</mi><mo>(</mo><mi>E</mi><mn>2</mn><mo>;</mo><msubsup><mn>0</mn><mn>2</mn><mo>+</mo></msubsup><mo>→</mo><msubsup><mn>2</mn><mn>1</mn><mo>+</mo></msubsup><mo>)</mo></mrow></math> in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mn>184</mn></mmultiscripts></math> to be determined. By means of electron-electron coincidences, the <math><msubsup><mn>0</mn><mn>3</mn><mo>+</mo></msubsup></math> state was identified in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mn>184</mn></mmultiscripts></math>. The experimental results were qualitatively reproduced by five theoretical approaches, the interacting boson model with configuration mixing with two different parametrizations, the general Bohr Hamiltonian, the beyond mean-field model, and the symmetry-conserving configuration-mixing model. However, a quantitative description is lacking.
Conclusions: The presence of shape coexistence in neutron-deficient mercury isotopes was confirmed and evidence for the phenomenon existing at higher energies was found. The new experimental results provide important spectroscopic input for future Coulomb excitation studies. |
id | cern-2866156 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2023 |
record_format | invenio |
spelling | cern-28661562023-10-18T09:20:10Zdoi:10.1103/PhysRevC.108.014308http://cds.cern.ch/record/2866156engStryjczyk, M.Andel, B.Cubiss, J.G.Rezynkina, K.Rodríguez, T.R.García-Ramos, J.E.Andreyev, A.N.Pakarinen, J.Van Duppen, P.Antalic, S.Berry, T.Borge, M.J.G.Clisu, C.Cox, D.M.De Witte, H.Fraile, L.M.Fynbo, H.O.U.Gaffney, L.P.Harkness-Brennan, L.J.Huyse, M.Illana, A.Judson, D.S.Konki, J.Kurcewicz, J.Lazarus, I.Lica, R.Madurga, M.Marginean, N.Marginean, R.Mihai, C.Mosat, P.Nacher, E.Negret, A.Ojala, J.Ovejas, J.D.Page, R.D.Papadakis, P.Pascu, S.Perea, A.Podolyák, Zs.Próchniak, L.Pucknell, V.Rapisarda, E.Rotaru, F.Sotty, C.Tengblad, O.Vedia, V.Viñals, S.Wadsworth, R.Warr, N.Wrzosek-Lipska, K.Simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopesnucl-thNuclear Physics - Theorynucl-exNuclear Physics - ExperimentBackground: The mercury isotopes around <math><mrow><mi>N</mi><mo>=</mo><mn>104</mn></mrow></math> are a well-known example of nuclei exhibiting shape coexistence. Mixing of configurations can be studied by measuring the monopole strength <math><mrow><msup><mi>ρ</mi><mn>2</mn></msup><mrow><mo>(</mo><mi>E</mi><mn>0</mn><mo>)</mo></mrow></mrow></math>, however, currently the experimental information is scarce and lacks precision, especially for the <math><mrow><msup><mi>I</mi><mi>π</mi></msup><mo>→</mo><msup><mi>I</mi><mi>π</mi></msup></mrow></math> (<math><mrow><mi>I</mi><mo>≠</mo><mn>0</mn></mrow></math>) transitions. Purpose: The goals of this study were to increase the precision of the known branching ratios and internal conversion coefficients, to increase the amount of available information regarding excited states in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math>, and to interpret the results in the framework of shape coexistence using different models. Method: The low-energy structures in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> were populated in the <math><mi>β</mi></math> decay of <math><mmultiscripts><mi>Tl</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math>, produced at ISOLDE, CERN and purified by laser ionization and mass separation. The <math><mi>γ</mi></math>-ray and internal conversion electron events were detected by five germanium clover detectors and a segmented silicon detector, respectively, and correlated in time to build decay schemes. Results: In total, 193, 178, and 156 transitions, including 144, 140, and 108 observed for the first time in a <math><mi>β</mi></math>-decay experiment, were assigned to <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math>, respectively. Internal conversion coefficients were determined for 23 transitions, out of which 12 had an <math><mrow><mi>E</mi><mn>0</mn></mrow></math> component. Extracted branching ratios allowed the sign of the interference term in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mn>182</mn></mmultiscripts></math> as well as <math><mrow><msup><mi>ρ</mi><mn>2</mn></msup><mrow><mo>(</mo><mi>E</mi><mn>0</mn><mo>;</mo><msubsup><mn>0</mn><mn>2</mn><mo>+</mo></msubsup><mo>→</mo><msubsup><mn>0</mn><mn>1</mn><mo>+</mo></msubsup><mo>)</mo></mrow></mrow></math> and <math><mrow><mi>B</mi><mo>(</mo><mi>E</mi><mn>2</mn><mo>;</mo><msubsup><mn>0</mn><mn>2</mn><mo>+</mo></msubsup><mo>→</mo><msubsup><mn>2</mn><mn>1</mn><mo>+</mo></msubsup><mo>)</mo></mrow></math> in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mn>184</mn></mmultiscripts></math> to be determined. By means of electron-electron coincidences, the <math><msubsup><mn>0</mn><mn>3</mn><mo>+</mo></msubsup></math> state was identified in <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mn>184</mn></mmultiscripts></math>. The experimental results were qualitatively reproduced by five theoretical approaches, the interacting boson model with configuration mixing with two different parametrizations, the general Bohr Hamiltonian, the beyond mean-field model, and the symmetry-conserving configuration-mixing model. However, a quantitative description is lacking. Conclusions: The presence of shape coexistence in neutron-deficient mercury isotopes was confirmed and evidence for the phenomenon existing at higher energies was found. The new experimental results provide important spectroscopic input for future Coulomb excitation studies.Background: The mercury isotopes around $N=104$ are a well-known example of nuclei exhibiting shape coexistence. Mixing of configurations can be studied by measuring the monopole strength $\rho^2(E0)$, however, currently the experimental information is scarce and lacks precision, especially for the $I^\pi \rightarrow I^\pi$ ($I \neq 0$) transitions. Purpose: The goals of this study were to increase the precision of the known branching ratios and internal conversion coefficients, to increase the amount of available information regarding excited states in $^{182,184,186}$Hg and to interpret the results in the framework of shape coexistence using different models. Method: The low-energy structures in $^{182,184,186}$Hg were populated in the $\beta$ decay of $^{182,184,186}$Tl, produced at ISOLDE and purified by laser ionization and mass separation. The $\gamma$-ray and internal conversion electron events were detected by five germanium clover detectors and a segmented silicon detector, respectively, and correlated in time to build decay schemes. Results: In total, 193, 178 and 156 transitions, including 144, 140 and 108 observed for the first time in a $\beta$-decay experiment, were assigned to $^{182,184,186}$Hg, respectively. Internal conversion coefficients were determined for 23 transitions, out of which 12 had an $E0$ component. Extracted branching ratios allowed the sign of the interference term in $^{182}$Hg as well as $\rho^2(E0;0^+_2\rightarrow 0^+_1)$ and $B(E2;0^+_2\rightarrow 2^+_1)$ in $^{184}$Hg to be determined. By means of electron-electron coincidences, the $0^+_3$ state was identified in $^{184}$Hg. The experimental results were qualitatively reproduced by five theoretical approaches, the IBM with configuration mixing with two different parametrizations, the General Bohr Hamiltonian, the BMF model and the SCCM model. However, a quantitative description is lacking.arXiv:2305.16442oai:cds.cern.ch:28661562023-05-25 |
spellingShingle | nucl-th Nuclear Physics - Theory nucl-ex Nuclear Physics - Experiment Stryjczyk, M. Andel, B. Cubiss, J.G. Rezynkina, K. Rodríguez, T.R. García-Ramos, J.E. Andreyev, A.N. Pakarinen, J. Van Duppen, P. Antalic, S. Berry, T. Borge, M.J.G. Clisu, C. Cox, D.M. De Witte, H. Fraile, L.M. Fynbo, H.O.U. Gaffney, L.P. Harkness-Brennan, L.J. Huyse, M. Illana, A. Judson, D.S. Konki, J. Kurcewicz, J. Lazarus, I. Lica, R. Madurga, M. Marginean, N. Marginean, R. Mihai, C. Mosat, P. Nacher, E. Negret, A. Ojala, J. Ovejas, J.D. Page, R.D. Papadakis, P. Pascu, S. Perea, A. Podolyák, Zs. Próchniak, L. Pucknell, V. Rapisarda, E. Rotaru, F. Sotty, C. Tengblad, O. Vedia, V. Viñals, S. Wadsworth, R. Warr, N. Wrzosek-Lipska, K. Simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopes |
title | Simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopes |
title_full | Simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopes |
title_fullStr | Simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopes |
title_full_unstemmed | Simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopes |
title_short | Simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>Hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopes |
title_sort | simultaneous <math><mi>γ</mi></math>-ray and electron spectroscopy of <math><mmultiscripts><mi>hg</mi><mprescripts/><none/><mrow><mn>182</mn><mo>,</mo><mn>184</mn><mo>,</mo><mn>186</mn></mrow></mmultiscripts></math> isotopes |
topic | nucl-th Nuclear Physics - Theory nucl-ex Nuclear Physics - Experiment |
url | https://dx.doi.org/10.1103/PhysRevC.108.014308 http://cds.cern.ch/record/2866156 |
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simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT rapisardae simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT rotaruf simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT sottyc simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT tengblado simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT vediav simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT vinalss simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT wadsworthr simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT warrn simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes AT wrzoseklipskak simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes |