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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 &...

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Autores principales: 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.
Lenguaje:eng
Publicado: 2023
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevC.108.014308
http://cds.cern.ch/record/2866156
_version_ 1780978081992802304
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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AT ojalaj simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes
AT ovejasjd simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes
AT pagerd simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes
AT papadakisp simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes
AT pascus simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes
AT pereaa simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes
AT podolyakzs simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes
AT prochniakl simultaneousmathmigmimathrayandelectronspectroscopyofmathmmultiscriptsmihgmimprescriptsnonemrowmn182mnmomomn184mnmomomn186mnmrowmmultiscriptsmathisotopes
AT pucknellv 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