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1.
采用量子化学计算方法和跃迁密度及电荷差分密度分析方法对含芴酮的低聚物激发态性质进行理论研究。计算得到的跃迁能和振子强度与实验数据一致。跃迁密度分析显示跃迁偶极矩的大小和方向,电荷差分密度分析揭示了分子间电荷转移的方向和结果。研究表明含芴酮的低聚物在光诱导下产生的第一激发态为分子内电荷转移激发态,而第五激发态为局域激发态。跃迁密度矩阵分析和电荷差分密度的理论分析结果易于理解含芴酮低聚物的激发态特性。  相似文献   

2.
采用量子化学计算方法和跃迁密度及电荷差分密度分析方法对含芴酮的低聚物激发态性质进行理论研究。计算得到的跃迁能和振子强度与实验数据一致。跃迁密度分析显示跃迁偶极矩的大小和方向,电荷差分密度分析揭示了分子间电荷转移的方向和结果。研究表明含芴酮的低聚物在光诱导下产生的第一激发态为分子内电荷转移激发态,而第五激发态为局域激发态。跃迁密度矩阵分析和电荷差分密度的理论分析结果易于理解含芴酮低聚物的激发态特性。  相似文献   

3.
研究了N ,N 二甲基苯胺和苯醌间光诱导电荷转移的溶剂效应 .首先在B3LYP/ 6 31G 水平上对给体和受体进行构型优化 ,然后采用优化的给受体构型在Cs 对称性下计算得到两种相对稳定的复合物构象P和T .在CIS/ 6 31+G 水平上计算复合物气相激发态 ,结果发现 ,构象P的第三单重激发态发生分子间的完全电荷分离 ,构象T的第三激发单重态发生分子间的部分电荷分离 .在上述同样水平上计算复合物溶剂条件下的激发态性质 ,与气相结果相比表明 ,溶剂中两种构象的第三单重激发态均发生完全电荷分离 ,吸收光谱均发生较大红移 .  相似文献   

4.
光系统Ⅱ反应中心包含有2个去镁叶绿素分子(Pheo),2个β胡萝卜素分子(β-Car)和6个叶绿素a分子(Chla).对反应中心的时间分辨荧光光谱表明,两个β-Car具有不同的吸收光谱,吸收峰分别为489 nm(Car489)和507 nm(Car507),Car489靠近吸收峰为667 nm和675 nm的叶绿素a(Chl a),它的主要功能是保护反应中心免受单态氧的破坏,而不能将激发能传递给光化学反应活性的色素分子P680;Car507靠近吸收峰为669 nm的Chl a分子;能够将激发能传递给P680,进行电荷分离.采用全局优化拟合的方法对荧光光谱进行处理,Car489在61 ps时间内将能量传递给Chl a672, 随后传给Chl a677,处于激发态的Chl a677在3 ns衰减到基态;Car507在274 ps时间内将能量传递给P680,P680+Pheo-的电荷重组发生在3.8 ns和16 ns.  相似文献   

5.
本文用密度泛函理论研究了一种给体-受体型低聚物(2,6-二(4-甲基-1-苯并噻二唑基)-4,4-二(2-乙基己基)-二噻吩并环戊二烯)中电荷转移态的光产生机制.研究表明,当CPDTBT单体的BT基团(苯并噻二唑)偏离共轭平面大于20°时,CPDTBT二聚体在光照时可以有效地产生分子间电荷转移态.计算表明,530 nm波长的光激发只能产生分子内的电荷转移态,而370 nm短波长的光激发才能产生分子间的电荷转移态,这和实验结果是比较一致的.本文还讨论了CPDTBT低聚物中光生电荷的分离机制.  相似文献   

6.
通过稳态光谱实验和量子化学计算相结合,研究了黄芩素激发态质子转移耦合电荷转移的反应. 实验和计算中S1态吸收峰的缺失表明S1态是暗态. S1暗态导致在实验中观察不到黄芩素在乙醇溶液中的荧光峰,且固体的荧光峰很弱. 黄芩素分子的前线分子轨道和电荷差异密度表明S1态是电荷转移态,然而S2态是局域激发态. 计算的黄芩素分子的势能曲线在激发态只有一个稳定点,这表明了黄芩素激发态分子内质子转移的过程是一个无  相似文献   

7.
蔡霞  王水才  贺俊芳  刘晓  彭菊芳 《光子学报》2008,37(7):1441-1445
采用稳态及飞秒荧光光谱技术研究了光系统Ⅱ中核心复合物在83 K、160 K和273 K低温下的能量传递途径.激发波长为507 nm.随着温度的升高,稳态荧光光谱逐渐发生蓝移.通过对不同温度下稳态光谱进行高斯解析,获得5个特征叶绿素a分子, 分别为Chl a670.4670, Chl a681.9680, Chl a683.9683, Chl a687.5,687.8,689687和Chl a698.0690,其中仅有Chl a687.5,687.8,689687在3个温度下的光谱中都解析获得,并且其谱宽以及荧光比例都随着温度升高而增加,因此推断温度对CP47中易裂解的叶绿素a分子有较大的影响.在680 nm以及690 nm波长处对不同温度下的时间曲线利用F900时间处理系统进行拟合,获得73 ps、 110 ps、 186 ps、 246~972 ps和1~3.7 ns 5个时间组分.其中, 73 ps是电荷分离的时间;110 ps和186 ps是β-Car分子受激发后,将激发能最终传递给反应中心所需要的时间;246~972 ps是电荷重组的时间过程;而1~3.7 ns是激发态分子发生电荷重组后又衰退回到基态的时间.73 ps的时间组分只在83 K温度下得到,因此,随着温度降低,可以探测到快的时间组分. 此外,对光谱随温度升高而发生蓝移进行了分析.  相似文献   

8.
在fullerene-PBTDP-TPA三体体系中的光诱导的分子内电荷转移的实验基础上,分别利用密度泛函理论和含时密度泛函理论以及结合二维、三维实空分析方法对fullerene、PBTDP-TPA二体以及fullerene-PBTDP-TPA三体的基态和激发态的性质进行了理论研究.二维定点表象揭示了激发情况下电子和空穴的相干情况.三维跃迁矩阵展示了跃迁偶极矩的方向和强度,而且三维电荷差密度给出了光诱导的分子内电荷转移的方向和结果.同时,用二维和三维表象的方法对fullerene-PBTDP-TPA三体中光诱导的分子内电荷转移过程进行了验证,揭示了在给予者-桥-接收者三体分子体系中分子内激发时电荷转移的机制.除此之外,还发现直接从给予者到接收者超交换的分子内电荷转移极大地促进了给予者-桥-接收者三体分子体系内的电荷转移.  相似文献   

9.
戚继发  修光宇  郭础 《光子学报》1991,20(1):114-119
本文采用时间分辨荧光光谱方法,考查了两种7-胺基香豆类素衍生物分子在不同溶剂中的荧光辐射弛豫过程,研究了环境因素对伴随着分子内电荷转移的分子内转动激发态(TICT)弛豫过程的影响。结果说明TICT态是非刚性香豆素分子激发态无辐射弛豫路径之一,这一过程受到环境介质的极性、粘度和温度的影响。并指出了在考虑粘度影响时,须对DSE理论进行修正,同时提出了TICT态存在位垒的观点。  相似文献   

10.
本文基于密度泛函理论,采用B3LYP方法,在6-31G(d,p)基组上对麻醉剂氯普鲁卡因的分子结构进行几何优化,在此基础上以乙醇为溶剂计算分子的前20个激发态,所有计算在Gaussian 09W-D01中进行。利用Multiwfn3.7软件绘制红外光谱图,并对其分子振动进行分析;利用Origin 2018 64Bit软件和Multiwfn3.7软件相结合绘制紫外光谱图,并计算空穴-电子来分析分子的激发态性质;通过计算前线轨道来预测氯普鲁卡因分子的活性位点。结果表明,在所计算得到的激发态中,由基态到第2、3、6、10激发态为局域激发,由基态到第19激发态为电荷转移激发。氯普鲁卡因乙氨基上的N22为亲电反应位点,苯环上的碳原子和脂基上的氧原子为亲核反应位点。本研究对更好的了解氯普鲁卡因分子的反应机理和在医学上的麻醉活性提供理论参考。  相似文献   

11.
The excitation wavelength dependence of the steady-state and time-resolved emission spectra of ethyl 5-(4-aminophenyl)-3-amino-2,4-dicyanobenzoate (EAADCy) in tetrahydrofuran (THF) at room temperature has been examined. It is found that the ratio of the fluorescence intensity of the long-wavelength and short-wavelength fluorescence bands strongly depends on the excitation wavelength, whereas the wavelengths of the fluorescence excitation and fluorescence bands maxima are independent on the observation/excitation wavelengths. The dynamic Stokes shift of fluorophore in locally excited (LE) and intramolecular charge transfer (ICT) states has been studied with a time resolution about 30 ps. The difference between Stokes shift in the LE and ICT states was attributed to the solvent response to the large photoinduced dipole moment of EAADCy in the fluorescent charge transfer state. On this base we can state that, the relaxation of the polar solvent molecules around the fluorophore was observed.  相似文献   

12.
We perform density functional theory calculations to investigate the polaron pair (charge transfer state) photo-generation in donor-acceptor oligomer methyl-capped (4,7-benzo[2,1,3]thiadiazole-2,6-(4,4-bis (2-ethylhexyl)-4H-cyclopenta[1,2-b;3,4-b'']dithiophene-4,7-benzo[2,1,3]thiadiazole)(CPDTBT).Results show that effective photo-generation of charge transfer state can happen in CPDTBT dimer when the group 4,7-benzo[2,1,3]thiadiazole (BT) in one monomer deviates against the conjugated plane (onset torsion angle is about 20°).The lower excitation energy (530 nm) can only generate the intramolecular excitonic state,while the higher excitation energy (370 nm) can generate the intermolecular charge transfer state,in good agreement with the experiment.Moreover,the mechanism of charge separation in CPDTBT oligomers is discussed.  相似文献   

13.
CF_3I由于其良好的绝缘性能和较低的液化温度而作为SF_6替代性气体被广泛研究.本文采用量子化学从头计算法在3-21g基组下优化了CF_3I基态分子结构,得到了基态CF_3I分子的键长、分子前线轨道、Mulliken电荷布居数、红外光谱等.并且在此基础上采用杂化CIS/3-21g方法计算了分子的激发态,得到了分子的激发能、波长和振子强度.结果显示基态CF_3I分子在外电场作用下分子结构发生形变,分子能隙减小,分子活性变强;分子前9个激发态变化明显,随着外电场强度增加,第1、2、9激发能先增大后减小,第3、4、5、6、7与8激发能逐渐减小;第1、2、9激发波长先减小后增大,3、4、5、6、7与8激发波长逐渐增大;在0~0.009 a.u.外电场作用下,第1、2、4、5、6激发态振子强度为零,属于禁阻跃迁,第3、9激发态振子强度随着电场强度的增加而减小,第7、8激发态振子强度随着外电场强度的增加而增加.  相似文献   

14.
Ultrafast relaxation kinetics of fucoxanthin in polar and non-polar solvents have been studied by femtosecond pump-probe spectroscopy. Transient absorption associated with S1 or intramolecular charge transfer (ICT) excited state has been observed following either one-photon excitation to the optically allowed S2 state or two-photon excitation to the symmetry-forbidden S1 state. The results suggest that the ICT state formed after excitation of fucoxanthin in a polar solvent is a distinct excited state from S1.  相似文献   

15.
找出了合成Eu3+激活的硼钒酸钇铕发光粉的适宜条件和发光最佳化学组分,它是(Y0.94Eu0.06)(V0.69B0.31)O3.7.对其发光光谱的温度依赖关系的研究指出,发光最佳温度在350℃左右.发光的这种温度依赖关系与基质和Eu3+对能量的吸收,以及基质向Eu3+能量传递效率的提高有关.此外,试验结果还表明,在365nm激发下,少显Gd2O3、Zn2GeO4·GeO2:Mn2+等添加剂的加入提高了样品的发光亮度.  相似文献   

16.
唐久超 《发光学报》2020,(3):288-295
染料敏化剂是染料敏化太阳能电池中关键的光电转换材料,其受光激发后,电子由低能级基态跃迁到高能级激发态从而产生有效的电势差。设计和筛选优异性能的染料敏化剂有利于提升其光电转化效率。本文以相关实验研究为背景,设计了一系列具有不同桥位基团的四硫富瓦烯(TTF)类纯有机染料敏化剂,利用密度泛函理论(DFT)和含时密度泛函理论(TD-DFT)对其光电转化及分子内电子转移特性进行了系统研究,通过比较筛选出了高性能的四硫富瓦烯类染料敏化剂。研究结果表明,以环戊联噻吩及其衍生物作为桥位基团的四硫富瓦类染料敏化剂的整体性能更佳,主要表现在较好的电荷分离态、拓宽的光谱吸收范围、提升的光捕获效率以及增强的分子内电子转移(IET)性能等。  相似文献   

17.
吴永刚  李世雄  郝进欣  徐梅  孙光宇  令狐荣锋 《物理学报》2015,64(15):153102-153102
采用密度泛函(DFT)B3PW91方法在Lanl2dz基组下优化得到CdSe分子的基态稳定构型, 并研究了外电场对CdSe基态分子的总能量、HOMO能级、LUMO能级、能隙、电偶极矩μ、电荷布居、红外光谱的影响. 在相同的基组下用TD-DFT 方法计算了外电场下CdSe分子的前9个激发态的激发能、激发波长和振子强度. 结果表明: 无电场时CdSe分子的激发波长与实验结果符合较好, 相应的激发能也很接近. 随着电场增加, CdSe基态分子键长、偶极矩、红外谱强度先减小后增大; HOMO能级、LUMO能级、能隙随电场增加而减小; 总能量、谐振频率则是先增大后减小. 此外, 外电场对CdSe分子的激发能, 激发波长和振子强度均有较大影响.  相似文献   

18.
A novel intramolecular donor–acceptor system of hydroquinone–benzonitrile was synthesized. Its photo-induced intramolecular charge-transfer (ICT) transition was confirmed by (1) shift of its emission maximum with increasing solvent polarity, (2) high dipole moment for the ICT excited state calculated from the Lippert equation, and (3) its HOMO and LUMO. According to the extent of separation between HOMO and LUMO, it is suggested that substituent position (ortho, meta, or para) in the donor–acceptor biphenyls is not a key point for the photo-induced intramolecular charge transfer and the donor with two alkoxy or hydroxy groups has more photo-induced charge transfer transitions than the one with one alkoxy or hydroxy group. In other words, the hydroquinone–benzonitrile system displays more photo-induced charge transfer transitions than 4COB (4-cyano-4′-butyloxybiphenyl).  相似文献   

19.
The intramolecular photoinduced charge separation within an oligo(p-phenylene vinylene)–fulleropyrrolidine dyad with four phenyl rings (OPV4-C60) has been investigated with femtosecond pump-probe spectroscopy in solvents of different polarity and in the solid state. In solution, photoexcitation of the OPV4 moiety of OPV4-C60 results in an ultrafast (<190 fs) singlet energy transfer reaction, creating the fullerene singlet excited state. In polar solvents, the ultrafast energy transfer is followed in the picosecond time domain by an intramolecular electron transfer. In accordance with Marcus theory, the rates for forward and backward intramolecular electron transfer in OPV4-C60 are influenced by the polarity of the solvent. In the solid state the photophysics of OPV4-C60 is dramatically different. In thin films, the forward electron transfer proceeds within 500 fs, irrespective of which chromophore is photoexcited. The increased rate for charge separation in the solid state is attributed to a more favorable orientation of the donor and acceptor that results in an intermolecular electron transfer. In the films, energy and electron transfer processes compete at the earliest moments after photoexcitation. In the solid state, the photogenerated electrons and holes have long lifetimes as a result of migration of these charges to thermodynamically more favorable sites in the film. PACS 78.47.1+p; 34.30.+h; 33.50.-j  相似文献   

20.
By utilizing the density functional theory(DFT) and the time-dependent density functional theory(TDDFT), the excited state intramolecular proton transfer(ESIPT) mechanism of o-hydroxynaphthyl phenanthroimidazole(HNPI) is studied in detail. Upon photo is excited, the intramolecular hydrogen bond is obviously enhanced in the S_1 state, which thus promotes the ESIPT process. Hydrogen bond is shown to be strengthened via comparing the molecular structures and the infrared vibration spectra of the S_0 and S_1 states. Through analyzing the frontier molecular orbitals, we can conclude that the excitation is a type of the intramolecular charge transfer excitation, which also indicates the trend of proton transfer in S_1 state. The vertical excitation based on TDDFT calculation can effectively repeat the absorption and fluorescence spectra of the experiment. However, the fluorescence spectrum of normal structure, which is similar to the spectrum of isomer structure is not detected in the experiment. It can be concluded that the fluorescence measured in the experiment is attributed to both structures. In addition, by analyzing the potential energy curves(PECs) calculated by the B3 LYP functional method, it can be derived that since the molecule to cross the potential barrier in the S_1 state is smaller than in the S_0 state and the reverse proton transfer process in the S_1 state is more difficult than in the S_0 state, the ESIPT occurs in the S_1 state.  相似文献   

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