文摘
In this paper we present tabulated data for magnetic-dipole-to-electric-quadrupole cross-susceptibilities (class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0092640X16300110&_mathId=si1.gif&_user=111111111&_pii=S0092640X16300110&_rdoc=1&_issn=0092640X&md5=038d8ac5e35c6c7b0308b1bd6a610a6e" title="Click to view the MathML source">χM1→E2class="mathContainer hidden">class="mathCode">) for Dirac one-electron atoms with a pointlike, spinless and motionless nucleus of charge class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0092640X16300110&_mathId=si326.gif&_user=111111111&_pii=S0092640X16300110&_rdoc=1&_issn=0092640X&md5=e26f23291228842087088201ef84048c" title="Click to view the MathML source">Zeclass="mathContainer hidden">class="mathCode">. Numerical values of this susceptibility for the hydrogen atom (class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0092640X16300110&_mathId=si327.gif&_user=111111111&_pii=S0092640X16300110&_rdoc=1&_issn=0092640X&md5=6baaf1bfce88246b25fe7a9e795d416d" title="Click to view the MathML source">Z=1class="mathContainer hidden">class="mathCode">) and for hydrogenic ions with class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0092640X16300110&_mathId=si328.gif&_user=111111111&_pii=S0092640X16300110&_rdoc=1&_issn=0092640X&md5=30226b17c12246766462c6fd501938a4" title="Click to view the MathML source">2⩽Z⩽137class="mathContainer hidden">class="mathCode"> are computed from the general analytical formula, recently derived by us (Stefanska, 2016), valid for an arbitrary discrete energy eigenstate. In this work we provide 30 tables with the values of class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0092640X16300110&_mathId=si1.gif&_user=111111111&_pii=S0092640X16300110&_rdoc=1&_issn=0092640X&md5=038d8ac5e35c6c7b0308b1bd6a610a6e" title="Click to view the MathML source">χM1→E2class="mathContainer hidden">class="mathCode"> for the ground state, and also for the first, the second and the third set of excited states (i.e.: 2s1/2, 2p1/2, 2p3/2, 3s1/2, 3p1/2, 3p3/2, 3d3/2, 3d5/2, 4s1/2, 4p1/2, 4p3/2, 4d3/2, 4d5/2, 4f5/2 and 4f7/2) of the relativistic hydrogenlike atoms. The value of the inverse of the fine-structure constant used in the calculations is class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0092640X16300110&_mathId=si4.gif&_user=111111111&_pii=S0092640X16300110&_rdoc=1&_issn=0092640X&md5=709aaadd10bbf5e27edac9241baf8149" title="Click to view the MathML source">α−1=137.035999139class="mathContainer hidden">class="mathCode">, and was taken from CODATA 2014.