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Electromagnetic moments of the antimony isotopes $^{112−133}$Sb - CERN Document Server

<!DOCTYPE html PUBLIC "-//W3C//DTD XHTML 1.0 Transitional//EN" "http://www.w3.org/TR/xhtml1/DTD/xhtml1-transitional.dtd"> <!--[if IEMobile 7]><html class="iem7" xmlns="http://www.w3.org/1999/xhtml" lang="en" xml:lang="en" xmlns:og="http://ogp.me/ns#" xmlns:fb="http://ogp.me/ns/fb#"><![endif]--> <!--[if lte IE 6]><html class="ie6 ie6-7 ie6-8" xmlns="http://www.w3.org/1999/xhtml" lang="en" xml:lang="en" xmlns:og="http://ogp.me/ns#" xmlns:fb="http://ogp.me/ns/fb#"><![endif]--> <!--[if (IE 7)&(!IEMobile)]><html class="ie7 ie6-7 ie6-8" xmlns="http://www.w3.org/1999/xhtml" lang="en" xml:lang="en" xmlns:og="http://ogp.me/ns#" xmlns:fb="http://ogp.me/ns/fb#"><![endif]--> <!--[if IE 8]><html class="ie8 ie6-8" xmlns="http://www.w3.org/1999/xhtml" lang="en" xml:lang="en" xmlns:og="http://ogp.me/ns#" xmlns:fb="http://ogp.me/ns/fb#"><![endif]--> <!--[if (gte IE 9)|(gt IEMobile 7)]><!--><html xmlns="http://www.w3.org/1999/xhtml" lang="en" xml:lang="en" xmlns:og="http://ogp.me/ns#" xmlns:fb="http://ogp.me/ns/fb#"><!--<![endif]--> <head> <title>Electromagnetic moments of the antimony isotopes $^{112−133}$Sb - CERN Document Server</title> <link href='https://framework.web.cern.ch/framework/2.0/fonts/PTSansWeb/PTSansWeb.css' rel='stylesheet' type='text/css' /> <link rel="stylesheet" href="https://cds.cern.ch/img/invenio.css?v=20141127" type="text/css" /> <link rel="stylesheet" href="https://cds.cern.ch/img/cern_theme/css/cern_theme.css?v=20141127" type="text/css" /> <link rel="stylesheet"href="/css/font-awesome.min.css"> <meta http-equiv="X-UA-Compatible" content="IE=Edge"/> <link rel="stylesheet" href="https://cds.cern.ch/img/cern_toolbar/css/toolbar.css" type="text/css" /> <!--[if lt IE 8]> <link href="https://cds.cern.ch/img/cern_toolbar/css/toolbar-ie.css" rel="stylesheet" type="text/css"> <![endif]--> <!--[if lt IE 8]> <link rel="stylesheet" type="text/css" href="https://cds.cern.ch/img/invenio-ie7.css" /> <![endif]--> <!--[if gt IE 8]> <style type="text/css">div.restrictedflag {filter:none;}</style> <![endif]--> <link rel="canonical" href="https://cds.cern.ch/record/2882324" /> <link rel="alternate" hreflang="el" href="https://cds.cern.ch/record/2882324?ln=el" /> <link rel="alternate" hreflang="fr" href="https://cds.cern.ch/record/2882324?ln=fr" /> <link rel="alternate" hreflang="bg" href="https://cds.cern.ch/record/2882324?ln=bg" /> <link rel="alternate" hreflang="zh-TW" href="https://cds.cern.ch/record/2882324?ln=zh_TW" /> <link rel="alternate" hreflang="pt" href="https://cds.cern.ch/record/2882324?ln=pt" /> <link rel="alternate" hreflang="no" href="https://cds.cern.ch/record/2882324?ln=no" /> <link rel="alternate" hreflang="hr" href="https://cds.cern.ch/record/2882324?ln=hr" /> <link rel="alternate" hreflang="ca" href="https://cds.cern.ch/record/2882324?ln=ca" /> <link rel="alternate" hreflang="de" href="https://cds.cern.ch/record/2882324?ln=de" /> <link rel="alternate" hreflang="it" href="https://cds.cern.ch/record/2882324?ln=it" /> <link rel="alternate" hreflang="zh-CN" href="https://cds.cern.ch/record/2882324?ln=zh_CN" /> <link rel="alternate" hreflang="sv" href="https://cds.cern.ch/record/2882324?ln=sv" /> <link rel="alternate" hreflang="sk" href="https://cds.cern.ch/record/2882324?ln=sk" /> <link rel="alternate" hreflang="en" href="https://cds.cern.ch/record/2882324?ln=en" /> <link rel="alternate" hreflang="pl" href="https://cds.cern.ch/record/2882324?ln=pl" /> <link rel="alternate" hreflang="ru" href="https://cds.cern.ch/record/2882324?ln=ru" /> <link rel="alternate" hreflang="ka" href="https://cds.cern.ch/record/2882324?ln=ka" /> <link rel="alternate" hreflang="ja" href="https://cds.cern.ch/record/2882324?ln=ja" /> <link rel="alternate" hreflang="es" href="https://cds.cern.ch/record/2882324?ln=es" /> <link rel="alternate" type="application/rss+xml" title="CERN Document Server RSS" href="/rss?ln=en" /> <link rel="search" type="application/opensearchdescription+xml" href="https://cds.cern.ch/opensearchdescription" title="CERN Document Server" /> <link rel="unapi-server" type="application/xml" title="unAPI" href="https://cds.cern.ch/unapi" /> <link rel="apple-touch-icon" href="/apple-touch-icon.png"/> <link rel="apple-touch-icon-precomposed" href="/apple-touch-icon-precomposed.png"/> <meta http-equiv="Content-Type" content="text/html; charset=utf-8" /> <meta http-equiv="Content-Language" content="en" /> <meta name="description" content="Nuclear moments of the antimony isotopes &lt;sup loc=&quot;post&quot;&gt;113−133&lt;/sup&gt;Sb are measured by collinear laser spectroscopy and used to benchmark phenomenological shell-model and ab initio calculations in the valence-space in-medium similarity renormalization group (VS-IMSRG). The shell-model calculations reproduce the electromagnetic moments over all Sb isotopes when suitable effective g-factors and charges are employed. Good agreement is achieved by VS-IMSRG for magnetic moments on the neutron-deficient side for both odd-even and odd-odd Sb isotopes while its results deviate from experiment on the neutron-rich side. When the same effective g-factors are used, VS-IMSRG agrees with experiment nearly as well as the shell model. Hence, the wave functions are very similar in both approaches and missing contributions to the M1 operator are identified as the cause of the discrepancy of VS-IMSRG with experiment. Electric quadrupole moments remain more challenging for VS-IMSRG. Nuclear moments of the antimony isotopes $^{113-133}$Sb are measured by collinear laser spectroscopy and used to benchmark phenomenological shell-model and \textit{ab initio} calculations in the valence-space in-medium similarity renormalization group (VS-IMSRG). The shell-model calculations reproduce the electromagnetic moments over all Sb isotopes when suitable effective $g$-factors and charges are employed. Good agreement is achieved by VS-IMSRG for magnetic moments on the neutron-deficient side for both odd-even and odd-odd Sb isotopes while its results deviate from experiment on the neutron-rich side. When the same effective $g$-factors are used, VS-IMSRG agrees with experiment nearly as well as the shell model. Hence, the wave functions are very similar in both approaches and missing contributions to the M1 operator are identified as the cause of the discrepancy of VS-IMSRG with experiment. Electric quadrupole moments remain more challenging for VS-IMSRG. Lechner, S.; Miyagi, T.; Xu, Z.Y.; Bissell, M.L.; Blaum, K.; Cheal, B.; Devlin, C.S.; Garcia Ruiz, R.F.; Ginges, J.S.M.; Heylen, H.; Holt, J.D.; Imgram, P.; Kanellakopoulos, A.; Koszorús, Á.; Malbrunot-Ettenauer, S.; Neugart, R.; Neyens, G.; Nörtershäuser, W.; Plattner, P.; Rodríguez, L.V.; Sanamyan, G.; Stroberg, S.R.; Utsuno, Y.; Yang, X.F.; Yordanov, D.T." /> <meta name="keywords" content="CERN Document Server, WebSearch, CERN Document Server" /> <script type="text/javascript" src="https://cds.cern.ch/js/jquery.min.js"></script> <!-- WebNews CSS library --> <link rel="stylesheet" href="https://cds.cern.ch/img/webnews.css" type="text/css" /> <!-- WebNews JS library --> <script type="text/javascript" src="https://cds.cern.ch/js/webnews.js?v=20131009"></script> <meta property="fb:app_id" content="137353533001720"/> <script type="text/x-mathjax-config"> MathJax.Hub.Config({ tex2jax: {inlineMath: [['$','$']], processEscapes: true}, showProcessingMessages: false, messageStyle: "none" }); </script> <script src="/MathJax/MathJax.js?config=TeX-AMS_CHTML" type="text/javascript"> </script> <!-- GoogleScholar --> <meta content="Elsevier B.V. : Electromagnetic moments of the antimony isotopes $^{112−133}$Sb" name="citation_title" /> <meta content="Lechner, S." name="citation_author" /> <meta content="Garcia Ruiz, R.F." name="citation_author" /> <meta content="Stroberg, S.R." name="citation_author" /> <meta content="Sanamyan, G." name="citation_author" /> <meta content="Yang, X.F." name="citation_author" /> <meta content="Ginges, J.S.M." name="citation_author" /> <meta content="Blaum, K." name="citation_author" /> <meta content="Heylen, H." name="citation_author" /> <meta content="Holt, J.D." name="citation_author" /> <meta content="Nörtershäuser, W." name="citation_author" /> <meta content="Rodríguez, L.V." name="citation_author" /> <meta content="Utsuno, Y." name="citation_author" /> <meta content="Plattner, P." name="citation_author" /> <meta content="Devlin, C.S." name="citation_author" /> <meta content="Bissell, M.L." name="citation_author" /> <meta content="Malbrunot-Ettenauer, S." name="citation_author" /> <meta content="Cheal, B." name="citation_author" /> <meta content="Neugart, R." name="citation_author" /> <meta content="Yordanov, D.T." name="citation_author" /> <meta content="Kanellakopoulos, A." name="citation_author" /> <meta content="Koszorús, Á." name="citation_author" /> <meta content="Imgram, P." name="citation_author" /> <meta content="Xu, Z.Y." name="citation_author" /> <meta content="Miyagi, T." name="citation_author" /> <meta content="Neyens, G." name="citation_author" /> <meta content="10.1016/j.physletb.2023.138278" name="citation_doi" /> <meta content="Phys. 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Electromagnetic moments of the antimony isotopes $^{112−133}$Sb </td> </tr> </table> </div> <div class="pagebody"><div class="pagebodystripemiddle"> <div class="detailedrecordbox"> <div class="detailedrecordtabs"> <div> <ul class="detailedrecordtabs"><li class="on first"><a href="/record/2882324/?ln=en">Information </a></li><li class=""><a href="/record/2882324/files?ln=en">Files </a></li></ul> <div id="tabsSpacer" style="clear:both;height:0px">&nbsp;</div></div> </div> <div class="detailedrecordboxcontent"> <div class="top-left-folded"></div> <div class="top-right-folded"></div> <div class="inside"> <!--<div style="height:0.1em;">&nbsp;</div> <p class="notopgap">&nbsp;</p>--> <abbr class="unapi-id" title="2882324"></abbr> <style type="text/css"> <!-- ul.detailedrecordtabs li.on a{background-color:#4D94CC;color:#fff !important;border-bottom:1px solid #4D94CC!important;} div.detailedrecordboxcontent {padding-top:0px !important;} --> </style> <table class="formatRecordTableFullWidth" > <tr> <td class="formatRecordHeader" style="background-image: url('https://cds.cern.ch/img/journals.jpg');" colspan="2"> <!--YTD: record may have more than one 690C.a tag--> Article </td> </tr> <script type="text/javascript"> $( document ).ready(function() { $('.showAuthor').on('click', function() { var author = '<p>' + $(this).data('name') + '</p>'; var affiliation = $(this).data('affiliation') + '</br>'; var contribution = $(this).data('contribution') + '</br>'; $.magnificPopup.open({ items: { src: '<div id="ovelary-mathjax" class="overlay-white oc-content overlay-white-500">' + author + affiliation + contribution + '</div>', type: 'inline' }, callbacks: { open: function() { var div = document.getElementById("overlay-mathjax") MathJax.Hub.Queue(["Typeset", MathJax.Hub, div]); }, } }) }) }); </script> <tr><td class="formatRecordLabel"> Report number </td><td style="padding-left:5px;"><a href="http://arxiv.org/abs/arXiv:2311.01110">arXiv:2311.01110</a></td></tr> <tr><td class="formatRecordLabel"> Title </td><td style="padding-left:5px;"><b>Electromagnetic moments of the antimony isotopes $^{112−133}$Sb</b></td></tr> <tr><td class="formatRecordLabel" style="vertical-align:top;">Related title</td><td style="padding-left:5px; ">Electromagnetic moments of the antimony isotopes 112−133Sb<br/></td></tr> <tr><td class="formatRecordLabel"><span style="white-space:nowrap;"> Author(s) </span> </td><td style="padding-left:5px;"> <script type="text/javascript"> function toggle_authors_visibility(){ var more = document.getElementById('more'); var link = document.getElementById('link'); var extension = document.getElementById('extension'); if (more.style.display=='none'){ more.style.display = ''; extension.style.display = 'none'; link.innerHTML = "Hide" } else { more.style.display = 'none'; extension.style.display = ''; link.innerHTML = "Show all 25 authors" } link.style.color = "rgb(204,0,0);" } function set_up(){ var extension = document.getElementById('extension'); extension.innerHTML = ""; toggle_authors_visibility(); } </script> <a name="show_hide" /><a href="https://cds.cern.ch/search?f=author&amp;p=Lechner%2C%20S.&amp;ln=en">Lechner, S.</a> (CERN ; Vienna, Tech. U., Atominst.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Miyagi%2C%20T.&amp;ln=en">Miyagi, T.</a> (Darmstadt, EMMI ; Heidelberg, Max Planck Inst. ; TRIUMF) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Xu%2C%20Z.Y.&amp;ln=en">Xu, Z.Y.</a> (Leuven U. ; Tennessee U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Bissell%2C%20M.L.&amp;ln=en">Bissell, M.L.</a> (Manchester U. ; CERN) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Blaum%2C%20K.&amp;ln=en">Blaum, K.</a> (Heidelberg, Max Planck Inst.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Cheal%2C%20B.&amp;ln=en">Cheal, B.</a> (Liverpool U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Devlin%2C%20C.S.&amp;ln=en">Devlin, C.S.</a> (Liverpool U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Garcia%20Ruiz%2C%20R.F.&amp;ln=en">Garcia Ruiz, R.F.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Ginges%2C%20J.S.M.&amp;ln=en">Ginges, J.S.M.</a> (Queensland U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Heylen%2C%20H.&amp;ln=en">Heylen, H.</a> (CERN ; Heidelberg, Max Planck Inst.)<span id="more" style=""> ; <a href="https://cds.cern.ch/search?f=author&amp;p=Holt%2C%20J.D.&amp;ln=en">Holt, J.D.</a> (TRIUMF) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Imgram%2C%20P.&amp;ln=en">Imgram, P.</a> (Darmstadt, EMMI ; Leuven U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Kanellakopoulos%2C%20A.&amp;ln=en">Kanellakopoulos, A.</a> (Leuven U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Koszor%C3%BAs%2C%20%C3%81.&amp;ln=en">Koszorús, Á.</a> (CERN ; Leuven U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Malbrunot-Ettenauer%2C%20S.&amp;ln=en">Malbrunot-Ettenauer, S.</a> (CERN ; TRIUMF ; Toronto U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Neugart%2C%20R.&amp;ln=en">Neugart, R.</a> (Heidelberg, Max Planck Inst. ; Mainz U., Inst. Kernphys.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Neyens%2C%20G.&amp;ln=en">Neyens, G.</a> (CERN ; Leuven U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=N%C3%B6rtersh%C3%A4user%2C%20W.&amp;ln=en">Nörtershäuser, W.</a> (Darmstadt, EMMI) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Plattner%2C%20P.&amp;ln=en">Plattner, P.</a> (CERN ; Innsbruck U. ; Heidelberg, Max Planck Inst.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Rodr%C3%ADguez%2C%20L.V.&amp;ln=en">Rodríguez, L.V.</a> (Heidelberg, Max Planck Inst. ; IJCLab, Orsay) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Sanamyan%2C%20G.&amp;ln=en">Sanamyan, G.</a> (Queensland U.) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Stroberg%2C%20S.R.&amp;ln=en">Stroberg, S.R.</a> (Washington U., Seattle ; NIST, Boulder) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Utsuno%2C%20Y.&amp;ln=en">Utsuno, Y.</a> (Tokyo U. ; JAEA, Ibaraki) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Yang%2C%20X.F.&amp;ln=en">Yang, X.F.</a> (Peking U., SKLNPT) ; <a href="https://cds.cern.ch/search?f=author&amp;p=Yordanov%2C%20D.T.&amp;ln=en">Yordanov, D.T.</a> (IJCLab, Orsay)</span> <span id="extension"></span> <small><i><a id="link" href="#" onclick="toggle_authors_visibility()" style="color:rgb(204,0,0);"></a></i></small><script type="text/javascript">set_up()</script></td></tr> <tr><td class="formatRecordLabel"> Publication </td><td style="padding-left:5px;">2023-10-26</td></tr> <tr><td class="formatRecordLabel"> Imprint </td><td style="padding-left:5px;">2023-11-02</td></tr> <tr><td class="formatRecordLabel"> Number of pages </td><td style="padding-left:5px;">9</td></tr> <tr><td class="formatRecordLabel"> In: </td><td style="padding-left:5px;"><i>Phys. Lett. B</i> 847 (2023) pp.138278</td></tr> <tr><td class="formatRecordLabel"> DOI </td><td style="padding-left:5px;"><a href="http://dx.doi.org/10.1016/j.physletb.2023.138278" title="DOI" target="_blank">10.1016/j.physletb.2023.138278</a> (publication)<br/> <a href="http://dx.doi.org/10.1016/j.physletb.2023.138278" title="DOI" target="_blank">10.1016/j.physletb.2023.138278</a> (publication) <tr><td class="formatRecordLabel"> Subject category </td><td style="padding-left:5px;">nucl-th ; Nuclear Physics - Theory ; nucl-ex ; Nuclear Physics - Experiment</td></tr> <tr><td class="formatRecordLabel"> Abstract </td><td style="padding-left:5px;">Nuclear moments of the antimony isotopes $^{113-133}$Sb are measured by collinear laser spectroscopy and used to benchmark phenomenological shell-model and \textit{ab initio} calculations in the valence-space in-medium similarity renormalization group (VS-IMSRG). The shell-model calculations reproduce the electromagnetic moments over all Sb isotopes when suitable effective $g$-factors and charges are employed. Good agreement is achieved by VS-IMSRG for magnetic moments on the neutron-deficient side for both odd-even and odd-odd Sb isotopes while its results deviate from experiment on the neutron-rich side. When the same effective $g$-factors are used, VS-IMSRG agrees with experiment nearly as well as the shell model. Hence, the wave functions are very similar in both approaches and missing contributions to the M1 operator are identified as the cause of the discrepancy of VS-IMSRG with experiment. Electric quadrupole moments remain more challenging for VS-IMSRG.</td></tr> <tr><td class="formatRecordLabel"> Copyright/License </td><td style="padding-left:5px;">preprint: (License: <a href="http://creativecommons.org/licenses/by-nc-nd/4.0/">CC BY-NC-ND 4.0</a>)<br/>publication: &copy; 2023-2025 The Authors (License: <a href="http://creativecommons.org/licenses/by/4.0/">CC BY 4.0</a>), sponsored by <a href="http://scoap3.org">SCOAP&#179;</a></td></tr> </table> <br /><div style="max-width:1024px;margin:auto"><div style="overflow-x:auto;display:inline;width:100%;"><a href="/record/2882324/plots#0"><img style="vertical-align:middle;" src="https://cds.cern.ch/record/2882324/files/113Sb.png" title=" Hyperfine spectrum of $^{113}$Sb in the $5s^25p^3\ ^4\text{S}_{3/2} \rightarrow 5s^25p^26s\ ^4\text{P}_{3/2}$ transition including a scheme of the hyperfine splitting. The frequency is given as an offset from the transition frequency (45945.340(5)\,cm$^{-1}$ \cite{NIST_ASD})." width="200px"/></a> <a href="/record/2882324/plots#1"><img style="vertical-align:middle;" src="https://cds.cern.ch/record/2882324/files/orbitals.png" title=" Relevant orbitals for the Sb isotopic chain. All calculation methods include the full neutron $N=50-82$ valence space. For the shell-model calculations also the full proton $Z=50-82$ valence space (dashed) is used, while for the \textit{ab initio} calculations either the sdg7 (dash-dot) or sdg (full line) valence space is employed." width="200px"/></a> <a href="/record/2882324/plots#2"><img style="vertical-align:middle;" src="https://cds.cern.ch/record/2882324/files/prl_mu.png" title=" Magnetic moments of (a) odd-even and (b) odd-odd $^{112-133}$Sb isotopes in comparison to shell-model and \textit{ab initio} calculations within the VS-IMSRG framework and the EM1.8/2.0 nuclear interaction. $\mu_\text{sp}$ indicates the single-particle value for the respective orbital. (sdg) includes the proton orbitals $\{0g_{9/2}, 0g_{7/2}, 1d_{5/2}, 2s_{1/2}, 1d_{3/2}\}$ and (sdg7) the same except $0g_{9/2}$, see \figref{fig:orbitals}. ``eff'' means that the effective $g$-factors $g_{\text{s,eff}}=0.6g_{\text{s}}$, $g_{\text{l,}\pi}=1.11$ and $g_{\text{l},\nu}=-0.02$ from the shell-model calculations were used instead of the renormalization of the operator. Literature values are taken from Refs.~\cite{Proctor1951,Fernando1960,Jackson1968,Krane1972,EKSTROM1974,CALLAGHAN1974,Ketel1976,Langouche1976,Booth1993,Lindroos1996,Stone1997,Stone2019}. Note that the second literature value of $^{121}$Sb is the first excited $7/2^+$ state (not observed in this work due to its short half-life)." width="200px"/></a> <a href='/record/2882324/plots'>Show more plots</a></div></div><br /> <br/>Corresponding record in: <a href="http://inspirehep.net/record/2716131">Inspire</a> <small> </small> <br/> <br/><br/><div align="right"><div style="padding-bottom:2px;padding-top:30px;"><span class="moreinfo" style="margin-right:10px;"> <a href="" class="moreinfo">Back to search</a> </span></div></div> <div class="bottom-left-folded"><div class="recordlastmodifiedbox" style="position:relative;margin-left:1px">&nbsp;Record created 2023-11-28, last modified 2024-05-08</div></div> <div class="bottom-right-folded" style="text-align:right;padding-bottom:2px;"> <span class="moreinfo" style="margin-right:10px;"></span></div> </div> </div> </div> <br/> <br /> <div class="detailedrecordminipanel"> <div class="top-left"></div><div class="top-right"></div> <div class="inside"> <div id="detailedrecordminipanelfile" style="width:33%;float:left;text-align:center;margin-top:0"> <div><small class="detailedRecordActions">Fulltext:</small> <br /><em>2311.01110</em> - <a href="/record/2882324/files/2311.01110.pdf"><img style="border:none" src="/img/file-icon-text-12x16.gif" alt="Download fulltext"/>PDF</a><br /><em>Publication</em> - <a href="/record/2882324/files/Publication.pdf"><img style="border:none" src="/img/file-icon-text-12x16.gif" alt="Download fulltext"/>PDF</a><br /></div> </div> <div id="detailedrecordminipanelreview" style="width:30%;float:left;text-align:center"> </div> <div id="detailedrecordminipanelactions" style="width:36%;float:right;text-align:right;"> <ul class="detailedrecordactions"> <li><a href="/yourbaskets/add?ln=en&amp;recid=2882324">Add to personal basket</a></li> <li>Export as <a style="text-decoration:underline;font-weight:normal" href="/record/2882324/export/hx?ln=en">BibTeX</a>, <a style="text-decoration:underline;font-weight:normal" href="/record/2882324/export/hm?ln=en">MARC</a>, <a style="text-decoration:underline;font-weight:normal" href="/record/2882324/export/xm?ln=en">MARCXML</a>, <a style="text-decoration:underline;font-weight:normal" href="/record/2882324/export/xd?ln=en">DC</a>, <a style="text-decoration:underline;font-weight:normal" href="/record/2882324/export/xe?ln=en">EndNote</a>, <!-- <a style="text-decoration:underline;font-weight:normal" href="/record/2882324/export/xe8x?ln=en">EndNote (8-X)</a>,--> <a style="text-decoration:underline;font-weight:normal" href="/record/2882324/export/xn?ln=en">NLM</a>, <a style="text-decoration:underline;font-weight:normal" href="/record/2882324/export/xw?ln=en">RefWorks</a> </li> </ul> <div style='padding-left: 13px;'> <!-- JQuery Bookmark Button BEGIN --> <div id="bookmark"></div> <div id="bookmark_sciencewise"></div> <style type="text/css"> #bookmark_sciencewise, #bookmark {float: left;} #bookmark_sciencewise li {padding: 2px; width: 25px;} #bookmark_sciencewise ul, #bookmark ul {list-style-image: none;} </style> <script type="text/javascript" src="/js/jquery.bookmark.min.js"></script> <style type="text/css">@import "/css/jquery.bookmark.css";</style> <script type="text/javascript">// <![CDATA[ $.bookmark.addSite('sciencewise', 'ScienceWise.info', 'https://cds.cern.ch/img/sciencewise.png', 'en', 'bookmark', 'http://sciencewise.info/bookmarks/2311.0111/add'); $('#bookmark_sciencewise').bookmark({sites: ['sciencewise']}); $('#bookmark').bookmark({ sites: ['facebook', 'twitter', 'linkedin', 'google_plusone'], icons: '/img/bookmarks.png', url: 'https://cds.cern.ch/record/2882324', addEmail: true, title: "Electromagnetic moments of the antimony isotopes $^{112\u2212133}$Sb", description: "Nuclear moments of the antimony isotopes <sup loc=\"post\">113\u2212133</sup>Sb are measured by collinear laser spectroscopy and used to benchmark phenomenological shell-model and ab initio calculations in the valence-space in-medium similarity renormalization group (VS-IMSRG). The shell-model calculations reproduce the electromagnetic moments over all Sb isotopes when suitable effective g-factors and charges are employed. Good agreement is achieved by VS-IMSRG for magnetic moments on the neutron-deficient side for both odd-even and odd-odd Sb isotopes while its results deviate from experiment on the neutron-rich side. When the same effective g-factors are used, VS-IMSRG agrees with experiment nearly as well as the shell model. Hence, the wave functions are very similar in both approaches and missing contributions to the M1 operator are identified as the cause of the discrepancy of VS-IMSRG with experiment. 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