159Dy Electron-Capture: A New Candidate for Neutrino Mass Determination
The ground state to ground state electron-capture Q value of ^{159}Dy (3/2^{-}) has been measured directly using the double Penning trap mass spectrometer JYFLTRAP. A value of 364.73(19) keV was obtained from a measurement of the cyclotron frequency ratio of the decay parent ^{159}Dy and the decay d...
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creator | Ge, Z Eronen, T Tyrin, K.S Kotila, J Kostensalo, J Nesterenko, D.A Beliuskina, O de Groote, R de Roubin, A Geldhof, S Gins, W Hukkanen, M Jokinen, A Kankainen, A Koszorus, A Krivoruchenko, M Kujanpaa, S Moore, I.D Raggio, A Rinta-Antila, S Suhonen, J Virtanen, V Weaver, A.P Zadvornaya, A |
description | The ground state to ground state electron-capture Q value of ^{159}Dy (3/2^{-}) has been measured directly using the double Penning trap mass spectrometer JYFLTRAP. A value of 364.73(19) keV was obtained from a measurement of the cyclotron frequency ratio of the decay parent ^{159}Dy and the decay daughter ^{159}Tb ions using the novel phase-imaging ion-cyclotron resonance technique. The Q values for allowed Gamow-Teller transition to 5/2^{-} and the third-forbidden unique transition to 11/2^{+} state with excitation energies of 363.5449(14) keV and 362.050(40) keV in ^{159}Tb were determined to be 1.18(19) keV and 2.68(19) keV, respectively. The high-precision Q value of transition 3/2^{-}→5/2^{-} from this work, revealing itself as the lowest electron-capture Q value, is used to unambiguously characterize all the possible lines that are present in its electron-capture spectrum. We performed atomic many-body calculations for both transitions to determine electron-capture probabilities from various atomic orbitals and found an order of magnitude enhancement in the event rates near the end point of energy spectrum in the transition to the 5/2^{-} nuclear excited state, which can become very interesting once the experimental challenges of identifying decays into excited states are overcome. The transition to the 11/2^{+} state is strongly suppressed and found unsuitable for measuring the neutrino mass. These results show that the electron-capture in the ^{159}Dy atom, going to the 5/2^{-} state of the ^{159}Tb nucleus, is a new candidate that may open the way to determine the electron-neutrino mass in the sub-eV region by studying electron-capture. Further experimental feasibility studies, including coincidence measurements with realistic detectors, will be of great interest. |
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A value of 364.73(19) keV was obtained from a measurement of the cyclotron frequency ratio of the decay parent ^{159}Dy and the decay daughter ^{159}Tb ions using the novel phase-imaging ion-cyclotron resonance technique. The Q values for allowed Gamow-Teller transition to 5/2^{-} and the third-forbidden unique transition to 11/2^{+} state with excitation energies of 363.5449(14) keV and 362.050(40) keV in ^{159}Tb were determined to be 1.18(19) keV and 2.68(19) keV, respectively. The high-precision Q value of transition 3/2^{-}→5/2^{-} from this work, revealing itself as the lowest electron-capture Q value, is used to unambiguously characterize all the possible lines that are present in its electron-capture spectrum. We performed atomic many-body calculations for both transitions to determine electron-capture probabilities from various atomic orbitals and found an order of magnitude enhancement in the event rates near the end point of energy spectrum in the transition to the 5/2^{-} nuclear excited state, which can become very interesting once the experimental challenges of identifying decays into excited states are overcome. The transition to the 11/2^{+} state is strongly suppressed and found unsuitable for measuring the neutrino mass. These results show that the electron-capture in the ^{159}Dy atom, going to the 5/2^{-} state of the ^{159}Tb nucleus, is a new candidate that may open the way to determine the electron-neutrino mass in the sub-eV region by studying electron-capture. Further experimental feasibility studies, including coincidence measurements with realistic detectors, will be of great interest.</description><identifier>ISSN: 0031-9007</identifier><language>eng</language><publisher>AMER PHYSICAL SOC</publisher><ispartof>PHYSICAL REVIEW LETTERS, 2021-12, Vol.127 (27)</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,315,776,780,27837</link.rule.ids></links><search><creatorcontrib>Ge, Z</creatorcontrib><creatorcontrib>Eronen, T</creatorcontrib><creatorcontrib>Tyrin, K.S</creatorcontrib><creatorcontrib>Kotila, J</creatorcontrib><creatorcontrib>Kostensalo, J</creatorcontrib><creatorcontrib>Nesterenko, D.A</creatorcontrib><creatorcontrib>Beliuskina, O</creatorcontrib><creatorcontrib>de Groote, R</creatorcontrib><creatorcontrib>de Roubin, A</creatorcontrib><creatorcontrib>Geldhof, S</creatorcontrib><creatorcontrib>Gins, W</creatorcontrib><creatorcontrib>Hukkanen, M</creatorcontrib><creatorcontrib>Jokinen, A</creatorcontrib><creatorcontrib>Kankainen, A</creatorcontrib><creatorcontrib>Koszorus, A</creatorcontrib><creatorcontrib>Krivoruchenko, M</creatorcontrib><creatorcontrib>Kujanpaa, S</creatorcontrib><creatorcontrib>Moore, I.D</creatorcontrib><creatorcontrib>Raggio, A</creatorcontrib><creatorcontrib>Rinta-Antila, S</creatorcontrib><creatorcontrib>Suhonen, J</creatorcontrib><creatorcontrib>Virtanen, V</creatorcontrib><creatorcontrib>Weaver, A.P</creatorcontrib><creatorcontrib>Zadvornaya, A</creatorcontrib><title>159Dy Electron-Capture: A New Candidate for Neutrino Mass Determination</title><title>PHYSICAL REVIEW LETTERS</title><description>The ground state to ground state electron-capture Q value of ^{159}Dy (3/2^{-}) has been measured directly using the double Penning trap mass spectrometer JYFLTRAP. A value of 364.73(19) keV was obtained from a measurement of the cyclotron frequency ratio of the decay parent ^{159}Dy and the decay daughter ^{159}Tb ions using the novel phase-imaging ion-cyclotron resonance technique. The Q values for allowed Gamow-Teller transition to 5/2^{-} and the third-forbidden unique transition to 11/2^{+} state with excitation energies of 363.5449(14) keV and 362.050(40) keV in ^{159}Tb were determined to be 1.18(19) keV and 2.68(19) keV, respectively. The high-precision Q value of transition 3/2^{-}→5/2^{-} from this work, revealing itself as the lowest electron-capture Q value, is used to unambiguously characterize all the possible lines that are present in its electron-capture spectrum. We performed atomic many-body calculations for both transitions to determine electron-capture probabilities from various atomic orbitals and found an order of magnitude enhancement in the event rates near the end point of energy spectrum in the transition to the 5/2^{-} nuclear excited state, which can become very interesting once the experimental challenges of identifying decays into excited states are overcome. The transition to the 11/2^{+} state is strongly suppressed and found unsuitable for measuring the neutrino mass. These results show that the electron-capture in the ^{159}Dy atom, going to the 5/2^{-} state of the ^{159}Tb nucleus, is a new candidate that may open the way to determine the electron-neutrino mass in the sub-eV region by studying electron-capture. Further experimental feasibility studies, including coincidence measurements with realistic detectors, will be of great interest.</description><issn>0031-9007</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>FZOIL</sourceid><recordid>eNqVjL0OgjAYADtoIqLv0NkE87UFETcDqItO7k0DHwmKLWmLP2-vgw-g0yWXy41IACBYlAGkEzJ17gIAjK_WAdmzJCtetOyw8tboKFe9Hyxu6Jae8EFzpeu2Vh5pY-zHDN622tCjco4W6NHeWq18a_SMjBvVOZx_GZLFrjznh-g6dDjcUcva9apCyUEmAJLxLOYy5ULEQoRk-XMs_dOLv-5v1JNK0w</recordid><startdate>20211231</startdate><enddate>20211231</enddate><creator>Ge, Z</creator><creator>Eronen, T</creator><creator>Tyrin, K.S</creator><creator>Kotila, J</creator><creator>Kostensalo, J</creator><creator>Nesterenko, D.A</creator><creator>Beliuskina, O</creator><creator>de Groote, R</creator><creator>de Roubin, A</creator><creator>Geldhof, S</creator><creator>Gins, W</creator><creator>Hukkanen, M</creator><creator>Jokinen, A</creator><creator>Kankainen, A</creator><creator>Koszorus, A</creator><creator>Krivoruchenko, M</creator><creator>Kujanpaa, S</creator><creator>Moore, I.D</creator><creator>Raggio, A</creator><creator>Rinta-Antila, S</creator><creator>Suhonen, J</creator><creator>Virtanen, V</creator><creator>Weaver, A.P</creator><creator>Zadvornaya, A</creator><general>AMER PHYSICAL SOC</general><scope>FZOIL</scope></search><sort><creationdate>20211231</creationdate><title>159Dy Electron-Capture: A New Candidate for Neutrino Mass Determination</title><author>Ge, Z ; Eronen, T ; Tyrin, K.S ; Kotila, J ; Kostensalo, J ; Nesterenko, D.A ; Beliuskina, O ; de Groote, R ; de Roubin, A ; Geldhof, S ; Gins, W ; Hukkanen, M ; Jokinen, A ; Kankainen, A ; Koszorus, A ; Krivoruchenko, M ; Kujanpaa, S ; Moore, I.D ; Raggio, A ; Rinta-Antila, S ; Suhonen, J ; Virtanen, V ; Weaver, A.P ; Zadvornaya, A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-kuleuven_dspace_20_500_12942_7233433</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ge, Z</creatorcontrib><creatorcontrib>Eronen, T</creatorcontrib><creatorcontrib>Tyrin, K.S</creatorcontrib><creatorcontrib>Kotila, J</creatorcontrib><creatorcontrib>Kostensalo, J</creatorcontrib><creatorcontrib>Nesterenko, D.A</creatorcontrib><creatorcontrib>Beliuskina, O</creatorcontrib><creatorcontrib>de Groote, R</creatorcontrib><creatorcontrib>de Roubin, A</creatorcontrib><creatorcontrib>Geldhof, S</creatorcontrib><creatorcontrib>Gins, W</creatorcontrib><creatorcontrib>Hukkanen, M</creatorcontrib><creatorcontrib>Jokinen, A</creatorcontrib><creatorcontrib>Kankainen, A</creatorcontrib><creatorcontrib>Koszorus, A</creatorcontrib><creatorcontrib>Krivoruchenko, M</creatorcontrib><creatorcontrib>Kujanpaa, S</creatorcontrib><creatorcontrib>Moore, I.D</creatorcontrib><creatorcontrib>Raggio, A</creatorcontrib><creatorcontrib>Rinta-Antila, S</creatorcontrib><creatorcontrib>Suhonen, J</creatorcontrib><creatorcontrib>Virtanen, V</creatorcontrib><creatorcontrib>Weaver, A.P</creatorcontrib><creatorcontrib>Zadvornaya, A</creatorcontrib><collection>Lirias (KU Leuven Association)</collection><jtitle>PHYSICAL REVIEW LETTERS</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ge, Z</au><au>Eronen, T</au><au>Tyrin, K.S</au><au>Kotila, J</au><au>Kostensalo, J</au><au>Nesterenko, D.A</au><au>Beliuskina, O</au><au>de Groote, R</au><au>de Roubin, A</au><au>Geldhof, S</au><au>Gins, W</au><au>Hukkanen, M</au><au>Jokinen, A</au><au>Kankainen, A</au><au>Koszorus, A</au><au>Krivoruchenko, M</au><au>Kujanpaa, S</au><au>Moore, I.D</au><au>Raggio, A</au><au>Rinta-Antila, S</au><au>Suhonen, J</au><au>Virtanen, V</au><au>Weaver, A.P</au><au>Zadvornaya, A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>159Dy Electron-Capture: A New Candidate for Neutrino Mass Determination</atitle><jtitle>PHYSICAL REVIEW LETTERS</jtitle><date>2021-12-31</date><risdate>2021</risdate><volume>127</volume><issue>27</issue><issn>0031-9007</issn><abstract>The ground state to ground state electron-capture Q value of ^{159}Dy (3/2^{-}) has been measured directly using the double Penning trap mass spectrometer JYFLTRAP. A value of 364.73(19) keV was obtained from a measurement of the cyclotron frequency ratio of the decay parent ^{159}Dy and the decay daughter ^{159}Tb ions using the novel phase-imaging ion-cyclotron resonance technique. The Q values for allowed Gamow-Teller transition to 5/2^{-} and the third-forbidden unique transition to 11/2^{+} state with excitation energies of 363.5449(14) keV and 362.050(40) keV in ^{159}Tb were determined to be 1.18(19) keV and 2.68(19) keV, respectively. The high-precision Q value of transition 3/2^{-}→5/2^{-} from this work, revealing itself as the lowest electron-capture Q value, is used to unambiguously characterize all the possible lines that are present in its electron-capture spectrum. We performed atomic many-body calculations for both transitions to determine electron-capture probabilities from various atomic orbitals and found an order of magnitude enhancement in the event rates near the end point of energy spectrum in the transition to the 5/2^{-} nuclear excited state, which can become very interesting once the experimental challenges of identifying decays into excited states are overcome. The transition to the 11/2^{+} state is strongly suppressed and found unsuitable for measuring the neutrino mass. These results show that the electron-capture in the ^{159}Dy atom, going to the 5/2^{-} state of the ^{159}Tb nucleus, is a new candidate that may open the way to determine the electron-neutrino mass in the sub-eV region by studying electron-capture. Further experimental feasibility studies, including coincidence measurements with realistic detectors, will be of great interest.</abstract><pub>AMER PHYSICAL SOC</pub></addata></record> |
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title | 159Dy Electron-Capture: A New Candidate for Neutrino Mass Determination |
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