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СµÜÎÒÏë×öÒ»¸öÀàËÆÏÂÃæÕâÑùµÄ¹ìµÀͼ1£ºÕâÊÇÒ»¸ö´ß»¯¼Á»î»¯ÇâÆøµÄ¹ý¶É̬£¬Í¨¹ý°Ñ¹ý¶É̬·Ö³É´ß»¯¼ÁµÄÒ»²¿·ÖºÍÇâÆøÁíÒ»²¿·Ö£¬×ܹ²Á½¸ö²¿·Ö£¬È»ºó×ö³ö·Ö±ð×÷³öÕâÁ½¸ö²¿·ÖµÄHOMOºÍLUMO¹ìµÀͼ£¬ÕâЩÎÒÖªµÀÓøß˹×öµ¥µã¾Í¿ÉÒԵõ½£¬µ«ÊÇËû»¹¿ÉÒÔËã³öÕâÁ½¸ö¶ÀÁ¢²¿·ÖµÄHOMOºÍHOMOÔÚ¹ý¶É̬Öеĵç×Ó·Ö²¼£¬±ÈÈçH2µÄHOMOÖеç×ÓΪ1.393×ªÒÆÁË0.683eµ½´ß»¯¼ÁµÄLUMO£¬¶ø´ß»¯¼ÁµÄHOMOµç×ÓΪ1.714e×ªÒÆ0.284µ½ÇâÆøµÄ·´¼ü¹ìµÀ£¬ÎÒÏëÖªµÀÕâÑùµÄ·ÖÎöÊÇÔõô×öµÄ£¬ÎÒ³¢ÊÔ¹ýÓÃMultiwfnµÄCDA·Ö½â¹¦ÄÜ£¬µ«ÊÇÕâ¸ö¹¦ÄÜÊÇ´ÓÅäºÏÎï¹ìµÀµÄ½Ç¶ÈÈ¥Ëãÿ¸öÿ¸öÅäºÏÎï¹ìµÀµÄdonationºÍback donation£¬ÎÒÏë´ÓÕâÁ½¸öƬ¶Î³ö·¢£¬¶øÇÒÖ»ÒªÖªµÀƬ¶ÎµÄHOMOºÍLUMOµç×Ó·Ö²¼¾Í¿ÉÒÔÁË£¬¾ÍºÍͼ1ÊÇÒ»ÑùµÄ£¬²éÁ˸÷ÖÖ×ÊÁÏ£¬»¹ÊDz»»á×ö£¬Çë½Ì´ó¼Ò£¬Ï×ÉÏÎҵĽð±Ò£¬»Ø¸´µÄÕýÈ·µÄÎÒ»¹¸øÄã×·¼Ó½ð±Ò¡£ÏÂÃæÎÒ°ÑÕâ¸öÎÄÕµÄÕⲿ·ÖÄÚÈÝÌùÉÏ£¬ÎÒÔÙ·ÅÉÏÕâ¸öÎÄÕµÄÔ­ÎÄ£¬ÕæµÄºÜÏëÖªµÀÔõô×öµÄ£¬Ð»Ð»Ð»Ð»£¡
MO Analysis of TS2/3. To clarify the reason why H−H ¦Ò-
bond cleavage leads to the formation of two positively charged
hydrogen atoms, we performed MO analysis of TS2/3.
Generally, MOs of a total system AB can be represented by a
linear combination of MOs of fragments A and B; see eq 1,28
¦Õi = ¦²C ¦Õ + ¦²C ϕ
m
im m
n
in n
AB A A B B
(1)
where ¦Õi
AB represents the ith MO of complex AB and ¦Õm A and
¦Õn
B are the mth and nth MOs of fragments A and B, respectively.
Cim
A and Cin
B are expansion coefficients of ¦Õm A and ¦Õn
B,
respectively. Electron populations of ¦Õm A and ¦Õn
B can be
obtained from these coefficients.29 Here, TS2/3 is divided into
such two moieties as H2 and 1Mes. Electron populations of
important MOs and MO pictures of the H2 and 1Mes moieties
are shown in Scheme 4. The population on the LUMO of 1Mes
considerably increases to 0.683 e, where the LUMO mainly
consists of a boron empty p orbital into which the nickel dz2
orbital moderately mixes in an antibonding way; see Scheme 4
for x, y, and z axes. In line with this increase, the population on
the ¦Ò-bonding MO of H2 considerably decreases to 1.393 e.These results clearly indicate that CT substantially occurs from
the ¦Ò-bonding MO of H2 to the LUMO of 1Mes. Furthermore,
the population of the ¦Ò*-antibonding MO of H2 somewhat
increases to 0.284 e. Accordingly, the electron population on
the highest occupied molecular orbital (HOMO) of 1Mes
somewhat decreases to 1.714 e, where the HOMO mainly
consists of the nickel dx2−y2 orbital. These population changes
indicate that CT occurs from the doubly occupied nickel dx2−y2
orbital to the H2 ¦Ò*-antibonding MO. Both of these CTs
contribute to a weakening of the strong H−H ¦Ò-bond.
However, it is noted that the former CT is much larger than
the latter one, indicating that CT from H2 to 1Mes plays a
dominant role in the H−H ¦Ò-bond cleavage process. This is
consistent with natural bond order analysis along the IRC that
H−H ¦Ò-bond cleavage leads to the formation of two positively
charged hydrogen atoms. When the boron atom is replaced by
the CH group, the former CT becomes much weaker, which
leads to the formation of two much less negatively charged
hydrogen atoms (−0.06 and −0.07 e, respectively). The higher
¦¤G¡ã⧧ value of the H2 activation reaction mediated by 1−CH
also confirms the importance of CT from H2 to 1Mes. These
results indicate that the borane ligand facilitates H−H ¦Ò-bond
cleavage by inducing large CT from H2 to 1Mes.ÇóÖúÕâ¸ö¹ìµÀµÄµç×ÓÕ¼¾ÝÊý·ÖÎö·½·¨
1.png


ÇóÖúÕâ¸ö¹ìµÀµÄµç×ÓÕ¼¾ÝÊý·ÖÎö·½·¨-1
2.png


ÇóÖúÕâ¸ö¹ìµÀµÄµç×ÓÕ¼¾ÝÊý·ÖÎö·½·¨-2
3.png
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  • ¸½¼þ 1 : MO.pdf
  • 2017-09-21 19:30:15, 3.58 M

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