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J. D. Petke Gerald M. Maggiora Lester L. Shipman† Ralph E. Christoffersen 《Photochemistry and photobiology》1980,32(5):661-667
Ab initio configuration interaction wavefunctions and energies are reported for 16 doublet states of the anion radical of ethyl bacteriopheophorbide a (Et-BPheo a-˙), and are employed in an analysis of the electronic absorption spectrum. The lowest excited doublet state D1 is predicted to lie 8601 cm-1 above the ground state D0; the D1← D0 transition is nearly forbidden, with a computed oscillator strength f= 0.002. The visible absorption spectrum is shown to consist of transitions to three 2(π, π*) states, D2, D3, and D4. The D4← D0 transition (y-polarized, f= 0.91) appears to account for observed intense absorption at 15 800 cm-1. The Soret band of Et-BPheo a-˙ is shown to consist of transitions to several 2(π,π*) states, D7-D15. Transitions of particularly high intensity include D7← D0 (y-polarized, f= 0.72), D10← D0 (y-polarized, f= 1.1), D12← D0 (xy-polarized, f= 0.86) and D15← D0 (y-polarized, f= 0.83). Spin density data and plots are used to describe and compare the general features of the unpaired spin distributions in D0 and D1, which are in reasonable agreement with other reported calculated values and available experimental data for D0. 相似文献
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J. D. Petke Gerald M. Maggiora Lester L. Shipman Ralph E. Christoffersen 《Photochemistry and photobiology》1980,31(3):243-257
Abstract— Ab initio configuration interaction wavefunctions and energies are reported for 29 doublet states and three quartet states of the cation radicals of ethyl chlorophyllide a (Et-Chl a+) and ethyl bacteriochlorophyllide a (Et-BChl a+). In Et-Chl a.+ I the lowest excited doublet state D1 is estimated to lie 5220 cm-1 above the ground state D0, with a negligibly small D1← D0 transition probability. The lowest quartet state, Q1, is estimated to lie 7980 cm-1 above D1. The absorption spectrum up to 20,000cm-1 is shown to consist primarily of numerous low-intensity ‘background’ transitions, with transitions to D5 and D11 accounting for the observed peaks at 12,200cm-1 and 17,500cm-1, respectively. The large intense band at 25,000cm-1 is due primarily to transitions to D22 and D23, with numerous lower-intensity transitions to neighboring states. In Et-BChl a.+ D1 is estimated to lie 7112 cm-1 above D0, and Q, is approximately 5725 cm-1 above D. A pair of states, D3 and D5, account for the absorption at 11,000 cm-1, while another pair of states, D13 and D14, are associated with the broad, weak absorption near 20,000 cm-1. The two prominent intense peaks at 23,700 cm-1 and 27,700 cm-1 are assigned to D23 and D28, respectively, while the shoulder located at 25,500cm-1 is attributed to transitions to D24 and D26. As in Et-Chl at, numerous background transitions are found throughout the spectrum. The π spin density distribution in D0 of both molecules is similar, with spin density found predominantly on the α-carbon atoms. In both systems, approximately 65% of the π spin density in D1 is found on the methine carbon atoms, with the remainder found largely on the nitrogen atoms. 相似文献
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J. D. Petke G. M. Maggiora Lester L. Shipman†Ralph E. Christoffersen‡ 《Photochemistry and photobiology》1982,36(4):383-393
Ab initio configuration interaction wavefunctions and energies are reported for the ground and low-lying excited doublet states of the anion radicals of ethyl chlorophyllide a (Et-Chl a - ) and ethyl pheophorbide a (Et-Pheo a - ), and are employed in a comparative analysis of their respective electronic absorption spectra.
Strong similarities exist between the first five computed excited states of both molecules, providing no distinguishing features in the electronic absorption spectra below 20000 cm- . Their ground state charge and spin density distributions are also very similar, and there is negligible spin density predicted on the magnesium atom in Et-Chl a- .
The Soret bands of both molecules are predicted to arise from intense transitions to several closely-spaced higher excited states, and the calculations indicate that there are significant differences in the number and composition of these states in the two molecules. It is suggested that these differences may provide a means of distinguishing between the two molecules using resonance Raman spectroscopy. 相似文献
Strong similarities exist between the first five computed excited states of both molecules, providing no distinguishing features in the electronic absorption spectra below 20000 cm
The Soret bands of both molecules are predicted to arise from intense transitions to several closely-spaced higher excited states, and the calculations indicate that there are significant differences in the number and composition of these states in the two molecules. It is suggested that these differences may provide a means of distinguishing between the two molecules using resonance Raman spectroscopy. 相似文献
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J. D. Petke Gerald M. Maggiora‡ Lester Shipman‡ Ralph E. CHRISTOFFERSEN‡ 《Photochemistry and photobiology》1979,30(2):203-223
Abstract— Ab initio configuration interaction wavefunctions and energies are reported for the ground state and many low-lying excited singlet and triplet states of ethyl pheophorbide a (Et-Pheo a) and ethyl chlorophyllide a (Et-Chl a), and are employed in an analysis of the electronic absorption spectra of these systems. In both molecules the visible spectrum is found to consist of transitions to the two lowest-lying 1(π, π*) states, S1 and S2. The configurational compositions of S1 and S2 in both molecules are similar, and are described qualitatively in terms of a four-orbital model. The S1← S0 transition in each case is predicted to be intense, and is largely in-plane y-polarized, while the S2← S0 transition is predicted to be extremely weak and in-plane polarized. The orientation of the S2← S0 transition dipole is not conclusively established in the present calculations. The Soret band in both molecules is composed of transitions to no less than ten states (S3-S12 in Et-Chl a and S3-S7S9-S12. and S14 in Et-Pheo a), which exhibit primarily (π, π*) character. The configurational compositions of these states are generally a complex mixture of excitations from both occupied macrocyclic π molecular orbitals and occupied orbitals with electron density in the cyclopen-tanone ring and the carbomethoxy chain. No clear correspondences are evident between respective Soret states of the two systems. Transitions to these states are generally intense and display a variety of in-plane polarizations. Two additional Soret states of Et-Pheo a, S8 and S13, exhibit primarily (n. π*) character. S8 is characterized by excitations from u and non-bonding regions of the carbomethoxy chain, while S13 is described by n →π* excitations involving the nitrogen atom of ring II. No corresponding (n, π*) states were found for Et-Chl a. In both molecules the lowest two triplet states, T1 and T2, are found to lie lower in energy than S1. while T, and S1 are approximately degenerate. The configurational compositions of T1-T4 of both molecules are nearly identical, and may be described by a four-orbital model. However, the compositions of T1-T4 differ sharply from those of S1 and S2. A number of higher-lying 3(π, π*) states of both molecules (T5-T13 in Et-Chi a and T8-T9, T11-T13 in Et-Pheo a) are found to have energies similar to the singlet Soret states, relative to S0. They are characterized by a complex mixture of configurations which do not include significant contributions involving the four-orbital model. In addition, two 3(n, π*) states of Et-Pheo a, T10 and T14, are found, which are somewhat analogous to S8 and S13. Additional data presented include the charge distributions and molecular dipole moments of the S0. S1, and T1 states of both molecules, as well as energies and oscillator strengths of computed Sn←S1 and Tn←1 transitions. 相似文献
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J. D. Petke Gerald M. Maggiora Lester L. Shipman Ralph E. Christoffersen 《Photochemistry and photobiology》1980,32(3):399-414
Abstract— Ab initio quantum mechanical calculations on ethyl bacteriochlorophyllide-a (Et-BChl-a) and ethyl bacteriopheophorbide-a (Et-BPheo-a) are presented, including self-consistent-field (SCF) molecular orbital studies on the ground states using the molecular fragment procedure, and configuration interaction (CI) calculations on the low-lying singlet and triplet states and absorption spectra. A characterization and comparison of many of the higher-lying molecular orbitals obtained from the SCF studies is presented. The estimated first ionization potentials are 5.66 and 5.97 eV for Et-BChl-a and Et-BPheo-a, respectively. Excited state calculations show that the visible spectrum of both molecules consists of an intense, y-polarized S1← S0 transition and a weakly-allowed, x-polarized S2← S0 transition. Both S1 and S2 states are 1(π, π*) in character, and are described by a four-orbital model. Transitions to the remaining calculated states, S3-S12, appear in the Soret region of the spectrum of both molecules. However, only transitions to S9(‘x’), S10(‘x’) and S11(‘y’) of Et-BChl-a, and S7(‘x’) and S10(‘y’) of Et-BPheo-a are of high intensity. The composition of the high intensity Soret states is 1(π, π*) and strongly “four-orbital” in nature. The lowest triplet state, T1, is predicted to lie 9752 cm-1 and 7880 cm-1 above S0 for Et-BPheo-a and Et-BChl-a, respectively. In each molecule T2 and S1 are nearly degenerate, suggesting a favorable pathway for intersystem crossing. Calculated Tn← T1 transitions indicate that the y-polarized T12← T1 transition in Et-BChl-a corresponds to the observed intense 24,400 cm-1 absorption in the triplet-triplet spectrum of BChl-a. A similar type spectrum is also predicted for BPheo-a. 相似文献
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本文根据Flory的溶胀理论和橡胶弹性理论,考察了顺-1 4-聚丁二烯辐射交联产物的化学网络和物理缠结网络结构特性及其对固体力学性能的影响。结果表明,交联产物的物理缠结网络密度远远大于化学交联网络密度。随着辐照剂量的增大,化学交联密度增高,物理缠结数下降。探讨了交联、缠结密度与Mooney-Rivlin方程的常数项C_1和C_2的关系。C_1来自化学交联网络的贡献;C_2来自物理缠结的贡献。物理缠结网络主要贡献于交联物体在小形变下的起始弹性模量G_0;化学交联网络则主要贡献于交联物体在大形变下的非线性弹性,即断裂强度(?)_B。 相似文献
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用X-射线衍射、动态力学测定等手段研究了不同拉伸倍数的超高分子量聚丙烯薄膜的力学性能的变化.以X-射线衍射法并基于串联力学模型的假设得到的各样品的表观晶区模量E_c~(app)约为34-38GPa.样品模量E_b随拉伸倍数增加而逐渐增大,其变化趋势与非晶区取向因子的变化相类似,说明非晶区取向是左右样品模量的重要因素.室温下,69倍拉伸样品的模量为27GPa,约为表观结晶模量的3/4,且其值在-150-160℃的温度范围内没有急剧变化,说明超拉伸明显改善了材料的力学性能及热稳定性.在各拉伸样品中,考虑伸直链结晶生成的可能性,利用并串联力学模型对伸直链结晶的体积分数做了估算,并对X-射线衍射法所得表观结晶模量进行了修正,认为室温下聚丙烯的真正晶区模量约为47GPa. 相似文献
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用X-射线衍射、动态力学测定等手段研究了不同拉伸倍数的超高分子量聚丙烯薄膜的力学性能的变化.以X-射线衍射法并基于串联力学模型的假设得到的各样品的表观晶区模量Ecapp约为34-38GPa.样品模量E_b随拉伸倍数增加而逐渐增大,其变化趋势与非晶区取向因子的变化相类似,说明非晶区取向是左右样品模量的重要因素.室温下,69倍拉伸样品的模量为27GPa,约为表观结晶模量的3/4,且其值在-150-160℃的温度范围内没有急剧变化,说明超拉伸明显改善了材料的力学性能及热稳定性.在各拉伸样品中,考虑伸直链结晶生成的可能性,利用并串联力学模型对伸直链结晶的体积分数做了估算,并对X-射线衍射法所得表观结晶模量进行了修正,认为室温下聚丙烯的真正晶区模量约为47GPa. 相似文献