{"id":281,"date":"2013-11-17T14:41:46","date_gmt":"2013-11-17T12:41:46","guid":{"rendered":"https:\/\/wissen.science-and-fun.de\/chemistry\/?p=281"},"modified":"2013-12-01T22:36:57","modified_gmt":"2013-12-01T20:36:57","slug":"lanthanum","status":"publish","type":"post","link":"https:\/\/wissen.science-and-fun.de\/chemistry\/2013\/11\/17\/lanthanum\/","title":{"rendered":"Lanthanum"},"content":{"rendered":"

NMR- Data<\/h2>\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n
Isotope<\/td>\n\u00a0138<\/sup>La<\/td>\nSpin<\/td>\n\u00a05<\/td>\n<\/tr>\n
Natural abundance (%)<\/td>\n\u00a00.090<\/td>\nMagnetic moment \u03bc\/\u03bcN<\/sub><\/td>\n\u00a04.068095<\/td>\n<\/tr>\n
Magnetogyric ratio
\n\u03b3\/107<\/sup>rad s-1<\/sup>T-1<\/sup><\/td>\n		\u00a03.557239<\/td>\nQuadrupole moment
\nQ\/fm2<\/sup><\/td>\n		\u00a045.0<\/td>\n<\/tr>\n
Frequency ratio
\n\u039e\/%<\/td>\n		\u00a013.194300<\/td>\nReference Sample<\/td>\n\u00a0LaCl3<\/sub><\/td>\n<\/tr>\n
Sample conditions<\/td>\n\u00a0D2<\/sub>O\/H2<\/sub>O<\/td>\nLine-width factor
\nl\/fm4<\/sup><\/td>\n		\u00a0120<\/td>\n<\/tr>\n
receptivity relative to 1<\/sup>H<\/td>\n\u00a08.46*10-5<\/sup><\/td>\nreceptivity relative to 13<\/sup>C<\/td>\n\u00a00.497<\/td>\n<\/tr>\n
Larmor Frequenzies (MHz) vs. Bruker Field Strengths (Tesla<\/span>)<\/th>\n<\/tr>\n
7.04925<\/td>\n9.39798<\/td>\n11.7467<\/td>\n14.0954<\/td>\n<\/tr>\n
\u00a039.600<\/td>\n\u00a052.794<\/td>\n\u00a065.989<\/td>\n\u00a079.183<\/td>\n<\/tr>\n
16.4442<\/td>\n17.6185<\/td>\n18.7929<\/td>\n19.9673<\/td>\n<\/tr>\n
\u00a092.377<\/td>\n\u00a098.974<\/td>\n\u00a0105.572<\/td>\n\u00a0112.169<\/td>\n<\/tr>\n
21.1416<\/td>\n22.3160<\/td>\n23.4904<\/td>\n<\/td>\n<\/tr>\n
\u00a0118.766<\/td>\n\u00a0125.363<\/td>\n\u00a0131.960<\/td>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n
\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n
Isotope<\/td>\n139<\/sup>La<\/td>\nSpin<\/td>\n\u00a07\/2<\/td>\n<\/tr>\n
Natural abundance (%)<\/td>\n\u00a099.910<\/td>\nMagnetic moment \u03bc\/\u03bcN<\/sub><\/td>\n\u00a03.1556770<\/td>\n<\/tr>\n
Magnetogyric ratio
\n\u03b3\/107<\/sup>rad s-1<\/sup>T-1<\/sup><\/td>\n		\u00a03.8083318<\/td>\nQuadrupole moment
\nQ\/fm2<\/sup><\/td>\n		\u00a020.0<\/td>\n<\/tr>\n
Frequency ratio
\n\u039e\/%<\/td>\n		\u00a014.125641<\/td>\nReference Sample<\/td>\n\u00a0LaCl3<\/sub><\/td>\n<\/tr>\n
Sample conditions<\/td>\n\u00a0D2<\/sub>O, 0.01M<\/td>\nLine-width factor
\nl\/fm4<\/sup><\/td>\n		\u00a054<\/td>\n<\/tr>\n
receptivity relative to 1<\/sup>H<\/td>\n\u00a06.05*10-2<\/sup><\/td>\nreceptivity relative to 13<\/sup>C<\/td>\n\u00a03.56*102<\/sup><\/td>\n<\/tr>\n
Larmor Frequenzies (MHz) vs. Bruker Field Strengths (Tesla<\/span>)<\/th>\n<\/tr>\n
7.04925<\/td>\n9.39798<\/td>\n11.7467<\/td>\n14.0954<\/td>\n<\/tr>\n
\u00a042.395<\/td>\n\u00a056.521<\/td>\n\u00a070.647<\/td>\n\u00a084.772<\/td>\n<\/tr>\n
16.4442<\/td>\n17.6185<\/td>\n18.7929<\/td>\n19.9673<\/td>\n<\/tr>\n
\u00a098.898<\/td>\n\u00a0105.961<\/td>\n\u00a0113.023<\/td>\n\u00a0120.086<\/td>\n<\/tr>\n
21.1416<\/td>\n22.3160<\/td>\n23.4904<\/td>\n<\/td>\n<\/tr>\n
\u00a0127.149<\/td>\n\u00a0134.212<\/td>\n\u00a0141.275<\/td>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n","protected":false},"excerpt":{"rendered":"

NMR- Data Isotope \u00a0138La Spin \u00a05 Natural abundance (%) \u00a00.090 Magnetic moment \u03bc\/\u03bcN \u00a04.068095 Magnetogyric ratio \u03b3\/107rad s-1T-1 \u00a03.557239 Quadrupole moment Q\/fm2 \u00a045.0 Frequency ratio \u039e\/% \u00a013.194300 Reference Sample \u00a0LaCl3 Sample conditions \u00a0D2O\/H2O Line-width factor l\/fm4 \u00a0120 receptivity relative to 1H \u00a08.46*10-5 receptivity relative to 13C \u00a00.497 Larmor Frequenzies (MHz) vs. Bruker Field Strengths (Tesla) … <\/p>\n

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