采用AM1和Ab Initio DFT方法,对3-(吡啶-2)-4-(喹啉-4)-吡唑(PQP) 进行了量子化学计算,给出了分子的几何构型、前沿分子轨道组成与能级、前沿轨道电子密度、原子的净电荷、键级等参数.结果表明PQP分子的稳定构型呈蝴蝶状,分子中的所有N...采用AM1和Ab Initio DFT方法,对3-(吡啶-2)-4-(喹啉-4)-吡唑(PQP) 进行了量子化学计算,给出了分子的几何构型、前沿分子轨道组成与能级、前沿轨道电子密度、原子的净电荷、键级等参数.结果表明PQP分子的稳定构型呈蝴蝶状,分子中的所有N原子和C18、C21等原子很可能是它与TβR-I作用时的活性位点.展开更多
AM1 method is employed to calculate the barriers against intramolecular proton transfer (IPT) of perylenequinone (PQ). The results obtained are as follows: (i) Barriers against the IPT reaction of ground state, single...AM1 method is employed to calculate the barriers against intramolecular proton transfer (IPT) of perylenequinone (PQ). The results obtained are as follows: (i) Barriers against the IPT reaction of ground state, singlet excited state and triplet excited state of PQ are 89.75, 55.40 and 83.97 kJ/mol, respectively. (ii) Barriers a-gainst the IPT process of anion of PQ in ground state and singlet excited state are 80.12 and 79. 91 kJ/mol, respectively, (iii) Barriers against the IPT of cation and anion radical of PQ (PQ,+ and PC,-) are 65. 94 and 59.29 kJ/ mol. (iv) The barrier against double proton transfer of PQ is 172.13 kJ/mol. (v) Two barriers against IPT of a type of perylenequinonoid photosensitizer (PQP), hypocrellin A (HA), are 89. 24 and 88. 07 kJ/mol. From these data conclusions can be drawn as follows: (i) IPT processes in ground state and excited state of PQ exist, but the transfer rate of excited state is much higher than that of ground state. (ii) It is almost impossible for PQ to transfer two protons simultaneously. (iii) IPT processes in anion, anion radical and cation radical of PQ still exist. (iv) The seven-membered side ring of HA has no marked influence on its barrier against IPT.展开更多
文摘采用AM1和Ab Initio DFT方法,对3-(吡啶-2)-4-(喹啉-4)-吡唑(PQP) 进行了量子化学计算,给出了分子的几何构型、前沿分子轨道组成与能级、前沿轨道电子密度、原子的净电荷、键级等参数.结果表明PQP分子的稳定构型呈蝴蝶状,分子中的所有N原子和C18、C21等原子很可能是它与TβR-I作用时的活性位点.
文摘AM1 method is employed to calculate the barriers against intramolecular proton transfer (IPT) of perylenequinone (PQ). The results obtained are as follows: (i) Barriers against the IPT reaction of ground state, singlet excited state and triplet excited state of PQ are 89.75, 55.40 and 83.97 kJ/mol, respectively. (ii) Barriers a-gainst the IPT process of anion of PQ in ground state and singlet excited state are 80.12 and 79. 91 kJ/mol, respectively, (iii) Barriers against the IPT of cation and anion radical of PQ (PQ,+ and PC,-) are 65. 94 and 59.29 kJ/ mol. (iv) The barrier against double proton transfer of PQ is 172.13 kJ/mol. (v) Two barriers against IPT of a type of perylenequinonoid photosensitizer (PQP), hypocrellin A (HA), are 89. 24 and 88. 07 kJ/mol. From these data conclusions can be drawn as follows: (i) IPT processes in ground state and excited state of PQ exist, but the transfer rate of excited state is much higher than that of ground state. (ii) It is almost impossible for PQ to transfer two protons simultaneously. (iii) IPT processes in anion, anion radical and cation radical of PQ still exist. (iv) The seven-membered side ring of HA has no marked influence on its barrier against IPT.
