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ÀûÓøß˹ÖеÄtd¼ÆË㼤·¢Ì¬£¬ÎÒÄܹ»µÃµ½¸ß˹¹Ø¼ü´Ê½éÉÜÖеÄÕâЩÄÚÈÝ£º ======================================================== Here is the key part of the output from a TD excited states calculation: Excitation energies and oscillator strengths: Excited State 1: Singlet-A2 4.0147 eV 308.83 nm f=0.0000 <S**2>=0.000 8 -> 9 0.70701 This state for optimization and/or second-order correction. Copying the excited state density for this state as the 1-particle RhoCI density. Excited State 2: Singlet-B1 9.1612 eV 135.34 nm f=0.0017 <S**2>=0.000 6 -> 9 0.70617 Excited State 3: Singlet-B2 9.5662 eV 129.61 nm f=0.1563 <S**2>=0.000 8 -> 10 0.70616 The results on each state are summarized, including the spin and spatial symmetry, the excitation energy, the oscillator strength, the S2, and (on the second line for each state) the largest coefficients in the CI expansion. The ECD results appear slightly earlier in the output as follows: 1/2[<0|r|b>*<b|rxdel|0> + (<0|rxdel|b> *<b|r|0> ) *] Rotatory Strengths (R) in cgs (10**-40 erg-esu-cm/Gauss) state XX YY ZZ R(length) R(au) 1 0.0000 0.0000 0.0000 0.0000 0.0000 2 0.0000 0.0000 0.0000 0.0000 0.0000 3 0.0000 0.0000 0.0000 0.0000 0.0000 1/2[<0|del|b>*<b|r|0> + (<0|r|b>*<b|del|0> )*] (Au) state X Y Z Dip. S. Osc.(frdel) 1 0.0000 0.0000 0.0000 0.0000 0.0000 2 -0.0050 0.0000 0.0000 0.0050 0.0033 3 0.0000 -0.2099 0.0000 0.2099 0.1399 ================================================================ ÏÖÔÚÓÐÁ½¸öÎÊÌâ²»Ã÷°×£¬Âé·³¸÷λ¸ßÊÖ¸øÖ¸µãһϣ¬Ð»Ð»£¡ 1. ÉÏÃæµÄÄÚÈÝÖ»¸ø³öÁË»ù̬µ½¼¤·¢Ì¬µÄԾǨÄÜÁ¿ºÍÕñ×ÓÇ¿¶È£¬¼¤·¢Ì¬µÄ²¨º¯ÊýÊÇÔõôÃèÊöµÄÄØ£¿ÎÒÔõôÄÜ¿´µ½£¿ 2. ×îºóÃæµÄ1/2[<0|r|b>*<b|rxdel|0> + (<0|rxdel|b> *<b|r|0> ) *] ºÍ 1/2[<0|del|b>*<b|r|0> + (<0|r|b>*<b|del|0> )*] (Au) ¶ÔÓ¦µÄ¹«Ê½Ó¦¸ÃÊÇÄÄÁ½¸ö£¬ÀïÃæµÄ¸÷Ïî·Ö±ðÊÇʲôÎïÀíÒâÒåÄØ£¿ |
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