文摘
In this paper we present tabulated data for magnetic-dipole-to-electric-quadrupole cross-susceptibilities (mmlsi1" class="mathmlsrc">mulatext 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→E2mathContainer hidden">mathCode"><math altimg="si1.gif" overflow="scroll"><msub><mrow><mi>χmi>mrow><mrow><mtext>Mmtext><mn>1mn><mo>→mo><mtext>Emtext><mn>2mn>mrow>msub>math>) for Dirac one-electron atoms with a pointlike, spinless and motionless nucleus of charge mmlsi326" class="mathmlsrc">mulatext 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">ZemathContainer hidden">mathCode"><math altimg="si326.gif" overflow="scroll"><mi>Zmi><mi>emi>math>. Numerical values of this susceptibility for the hydrogen atom (mmlsi327" class="mathmlsrc">mulatext 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=1mathContainer hidden">mathCode"><math altimg="si327.gif" overflow="scroll"><mi>Zmi><mo>=mo><mn>1mn>math>) and for hydrogenic ions with mmlsi328" class="mathmlsrc">mulatext 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⩽137mathContainer hidden">mathCode"><math altimg="si328.gif" overflow="scroll"><mn>2mn><mo>⩽mo><mi>Zmi><mo>⩽mo><mn>137mn>math> 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 mmlsi1" class="mathmlsrc">mulatext 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→E2mathContainer hidden">mathCode"><math altimg="si1.gif" overflow="scroll"><msub><mrow><mi>χmi>mrow><mrow><mtext>Mmtext><mn>1mn><mo>→mo><mtext>Emtext><mn>2mn>mrow>msub>math> 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 mmlsi4" class="mathmlsrc">mulatext 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=137.035999139mathContainer hidden">mathCode"><math altimg="si4.gif" overflow="scroll"><msup><mrow><mi>αmi>mrow><mrow><mo>−mo><mn>1mn>mrow>msup><mo>=mo><mn>137.035999139mn>math>, and was taken from CODATA 2014.