{"id":73,"date":"2011-07-07T18:44:00","date_gmt":"2011-07-07T16:44:00","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=73"},"modified":"2012-01-08T19:44:31","modified_gmt":"2012-01-08T17:44:31","slug":"paper-g-factor-of-hydrogenlike-28si13","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=73","title":{"rendered":"[paper] g Factor of Hydrogenlike <sup>28<\/sup>Si<sup>13+<\/sup>"},"content":{"rendered":"<p><em>g Factor of Hydrogenlike <sup>28<\/sup>Si<sup>13+<\/sup><\/em><\/p>\n<p>S. Sturm <em>et al.<\/em><\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevLett.107.023002\">10.1103\/PhysRevLett.107.023002<\/a><\/p>\n<p>We determined the experimental value of the g factor of the electron bound in hydrogenlike <sup>28<\/sup>Si<sup>13+<\/sup> by using a single ion confined in a cylindrical Penning trap. From the ratio of the ion\u2019s cyclotron frequency and the induced spin flip frequency, we obtain g=1.995\u2009348\u2009958\u20097(5)(3)(8). It is in excellent agreement with the state-of-the-art theoretical value of 1.995\u2009348\u2009958\u20090(17), which includes QED contributions up to the two-loop level of the order of (Z\u03b1)2 and (Z\u03b1)4 and represents a stringent test of bound-state quantum electrodynamics calculations.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>g Factor of Hydrogenlike 28Si13+ S. Sturm et al. doi: 10.1103\/PhysRevLett.107.023002 We determined the experimental value of the g factor of the electron bound in hydrogenlike 28Si13+ by using a single ion confined in a cylindrical Penning trap. From the&#46;&#46;&#46;<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"jetpack_post_was_ever_published":false,"jetpack_publicize_message":"","jetpack_is_tweetstorm":false,"jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":false,"jetpack_social_options":{"image_generator_settings":{"template":"highway","enabled":false}}},"categories":[3,1],"tags":[111,39,113,5,114,104,112],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-1b","jetpack-related-posts":[{"id":95,"url":"https:\/\/magneticmoments.info\/wp\/?p=95","url_meta":{"origin":73,"position":0},"title":"[paper] First g-factor measurements of the 21+ and the 41+ states of radioactive 100Pd","date":"Oct 25, 2011","format":false,"excerpt":"First g-factor measurements of the 21+ and the 41+ states of radioactive 100Pd D.A. Torres et al. doi: 10.1103\/PhysRevC.84.044327 The g factors of the first 2+ and 4+ states of the radioactive 100Pd nucleus have been investigated for the first time, using an \u03b1-particle transfer reaction from 12C to 96Ru.\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":105,"url":"https:\/\/magneticmoments.info\/wp\/?p=105","url_meta":{"origin":73,"position":1},"title":"[paper] Direct Measurement of the Proton Magnetic Moment","date":"Apr 10, 2012","format":false,"excerpt":"Direct Measurement of the Proton Magnetic Moment J. DiSciacca and G. Gabrielse doi: 10.1103\/PhysRevLett.108.153001 The proton magnetic moment in nuclear magnetons is measured to be \u03bcp\/\u03bcN\u2261g\/2=2.792\u2009846\u00b10.000\u2009007, a 2.5 parts per million uncertainty. The direct determination, using a single proton in a Penning trap, demonstrates the first method that should work\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":36,"url":"https:\/\/magneticmoments.info\/wp\/?p=36","url_meta":{"origin":73,"position":2},"title":"[paper] g factor of the 44Cl ground state: Probing the reduced Z=16 and N=28 gaps","date":"Mar 19, 2010","format":false,"excerpt":"g factor of the 44Cl ground state: Probing the reduced Z=16 and N=28 gaps M. De Rydt et al. doi: 10.1103\/PhysRevC.81.034308 The g factor of the 44Cl ground state is measured at the LISE fragment separator at the Grand Accl\u00e9rateur National d\u2019Ions Lourds (GANIL) using the \u03b2 nuclear magnetic resonance\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":110,"url":"https:\/\/magneticmoments.info\/wp\/?p=110","url_meta":{"origin":73,"position":3},"title":"[paper] First g(2+) measurement on neutron-rich 72Zn, and the high-velocity transient field technique for radioactive heavy-ion beams","date":"Mar 29, 2012","format":false,"excerpt":"First g(2+) measurement on neutron-rich 72Zn, and the high-velocity transient field technique for radioactive heavy-ion beams E. Fiori et al. doi: 10.1103\/PhysRevC.85.034334 The high-velocity transient-field (HVTF) technique was used to measure the g factor of the 2+ state of 72Zn produced as a radioactive beam. The transient-field strength was probed\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":115,"url":"https:\/\/magneticmoments.info\/wp\/?p=115","url_meta":{"origin":73,"position":4},"title":"[paper] Structure of the Sr-Zr isotopes near and at the magic N=50 shell from g-factor and lifetime measurements in8840Zr and 84,86,8838Sr","date":"Apr 30, 2012","format":false,"excerpt":"Structure of the Sr-Zr isotopes near and at the magic N=50 shell from g-factor and lifetime measurements in8840Zr and 84,86,8838Sr G. Kumbartzki et al. doi: 10.1103\/PhysRevC.85.044322 Background: The evolution of and interplay between single-particle and collective excitations in the 40 \u2a7dN\u2a7d 50 range for 38Sr and 40Zr isotopes have been\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":144,"url":"https:\/\/magneticmoments.info\/wp\/?p=144","url_meta":{"origin":73,"position":5},"title":"[paper] g factor of the exotic N=21 isotope 34Al: probing the N=20 and N=28 shell gaps at the border of the &quot;island of inversion&quot;","date":"Jan 10, 2008","format":false,"excerpt":"g factor of the exotic N=21 isotope 34Al: probing the N=20 and N=28 shell gaps at the border of the \"island of inversion\" P. Himpe et al. doi: 10.1016\/j.physletb.2007.11.017 For the first time the g factor of an isotope beyond N=20 near the \"island of inversion\" has been measured. A\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/73"}],"collection":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=73"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/73\/revisions"}],"predecessor-version":[{"id":74,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/73\/revisions\/74"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=73"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=73"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=73"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}