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Show 75 The Table 15. of the eigenvectors filled molecular orbital highest and lowest vacant molecular orbital calculated from the simple LeAO-MO method foY' structures X and XIV, Eienvectors Atom ch_( X) cjk(; ) c .I.. ( -'.TV) . ( 'X r! ) - ]1\. Nl -.4453 02620 -04636 00084 C2 -,0688 -<11105 -111755. "'05552 N3 -110627 1)1833 02114 113401 C4 111005 -113169 ,,1003 '""01436 C5 07247 -113682 06487 "".4644 C6 (12941 117214 1)3406 .5379 °7 02099 tl0961 IIll96 01754 Os '""113067 ,,2757 \13854 .1401 °9 --.1819 "'02095 The observed rot.tional the recorded .... I strenst,hs, oan be roughly estimated from amplitude values56 by use of Equation 47 and the 1"e- lationship Amp [eo J ,A _= - 122 which arises as a corollary of the KronigKramers theorem.59 "observed" rotational strengths and the caloulated in terms of 1040 cgs.units are given belows The rotatioal strengths |