{"id":134,"date":"2013-06-04T11:42:10","date_gmt":"2013-06-04T08:42:10","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=134"},"modified":"2013-06-04T11:42:45","modified_gmt":"2013-06-04T08:42:45","slug":"paper-demonstration-of-the-double-penning-trap-technique-with-a-single-proton","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=134","title":{"rendered":"[paper] Demonstration of the double Penning Trap technique with a single proton"},"content":{"rendered":"<p><em>Demonstration of the double Penning Trap technique with a single proton<\/em><\/p>\n<p>A. Mooser et al.<\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1016\/j.physletb.2013.05.012\">10.1016\/j.physletb.2013.05.012<\/a><\/p>\n<p>Spin flips of a single proton were driven in a Penning trap with a homogeneous magnetic field.<br \/>\nFor the spin-state analysis the proton was transported into a second Penning trap with<br \/>\na superimposed magnetic bottle, and the continuous Stern\u2013Gerlach effect was applied.<br \/>\nThis first demonstration of the double Penning trap technique with a single proton suggests<br \/>\nthat the antiproton magnetic moment measurement can potentially be improved by three<br \/>\norders of magnitude or more.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Demonstration of the double Penning Trap technique with a single proton A. Mooser et al. doi: 10.1016\/j.physletb.2013.05.012 Spin flips of a single proton were driven in a Penning trap with a homogeneous magnetic field. For the spin-state analysis the proton&#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],"tags":[149,191,8,114,148],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-2a","jetpack-related-posts":[{"id":105,"url":"https:\/\/magneticmoments.info\/wp\/?p=105","url_meta":{"origin":134,"position":0},"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":216,"url":"https:\/\/magneticmoments.info\/wp\/?p=216","url_meta":{"origin":134,"position":1},"title":"[paper] Sixfold improved single particle measurement of the magnetic moment of the antiproton","date":"Jan 19, 2017","format":false,"excerpt":"Sixfold improved single particle measurement of the magnetic moment of the antiproton H. Nagahama et al. doi: 10.1038\/ncomms14084 Our current understanding of the Universe comes, among others, from particle physics and cosmology. In particle physics an almost perfect symmetry between matter and antimatter exists. On cosmological scales, however, a striking\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":73,"url":"https:\/\/magneticmoments.info\/wp\/?p=73","url_meta":{"origin":134,"position":2},"title":"[paper] g Factor of Hydrogenlike 28Si13+","date":"Jul 7, 2011","format":false,"excerpt":"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 ratio of the ion\u2019s cyclotron frequency and the induced spin\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":170,"url":"https:\/\/magneticmoments.info\/wp\/?p=170","url_meta":{"origin":134,"position":3},"title":"[Paper] The ASACUSA CUSP: an antihydrogen experiment","date":"Nov 10, 2015","format":false,"excerpt":"The ASACUSA CUSP: an anti hydrogen experiment N. Kuroda et al. doi: 10.1007\/s10751-015-1205-1 In order to test CPT symmetry between antihydrogen and its counterpart hydrogen, the ASACUSA collaboration plans to perform high precision microwave spectroscopy of ground-state hyperfine splitting of antihydrogen atom in-flight. We have developed an apparatus (\u201ccusp trap\u201d)\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":36,"url":"https:\/\/magneticmoments.info\/wp\/?p=36","url_meta":{"origin":134,"position":4},"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":303,"url":"https:\/\/magneticmoments.info\/wp\/?p=303","url_meta":{"origin":134,"position":5},"title":"Probing Sizes and Shapes of Nobelium Isotopes by Laser Spectroscopy","date":"Jun 10, 2018","format":false,"excerpt":"Until recently, ground-state nuclear moments of the heaviest nuclei could only be inferred from nuclear spectroscopy, where model assumptions are required. Laser spectroscopy in combination with modern atomic structure calculations is now able to probe these moments directly, in a comprehensive and nuclear-model-independent way. Here we report on unique access\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/134"}],"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=134"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/134\/revisions"}],"predecessor-version":[{"id":135,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/134\/revisions\/135"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=134"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=134"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=134"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}