1977
DOI: 10.1016/s0040-4039(01)83513-9
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Enantiomere pentatetraene und deren barriere der thermischen razemisierung

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Cited by 9 publications
(6 citation statements)
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“…It is interesting to note that the corresponding DE a 0 with triplet spin multiplicity (using the unrestricted B3LYP/6-31G Ã method for the transition state structures) were also closer to the reported experimental data. [9][10] Therefore, this fact is in accordance with Hund's rule which would predict that the triplet transition state structure energy is below the correspond-ing rotated singlet state, as shown below:…”
Section: Computational Detailssupporting
confidence: 82%
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“…It is interesting to note that the corresponding DE a 0 with triplet spin multiplicity (using the unrestricted B3LYP/6-31G Ã method for the transition state structures) were also closer to the reported experimental data. [9][10] Therefore, this fact is in accordance with Hund's rule which would predict that the triplet transition state structure energy is below the correspond-ing rotated singlet state, as shown below:…”
Section: Computational Detailssupporting
confidence: 82%
“…8 The DH # values between the diastereoisomers is relatively low: 129.64 kJ mol À1 for CH 3 CH --C --C --CHCH 3 and only 112.91 kJ mol À1 for t-Bu(C 6 H 5 )C --C --C --C(C 6 H 5 )t-Bu. 9,10 The values of DG # for the two cases, 132.15 and 125.26 kJ mol À1 , 11 are in agreement with the values for RR 0 C --C --C --CRR 0 (R¼C 6 H 5 , R'¼C(CH 3 ) 2 CH 2 C 6 H 5 ), for example, 125.04 kJ mol À1 . 10 The t-Bu/ C 6 H 5 compound has a remarkably negative activation entropy for isomerization (DS # ¼ À31.99 J mol À1 K À1 ).…”
Section: Introductionsupporting
confidence: 78%
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