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×î½üͶÁËÒ»¸öÀ¬»øÎÄÕ£¬Ö®Ç°±»¾Ü7´ÎºóÕâ´ÎÒâÍâÈôóÐÞ£¬ÀïÃæÓÐÒ»¸ö¼ÆËãµÄÎÊÌâ¶Ô±¾ÈËÀ´Ëµ·Ç³£¼¬ÊÖ£¬±¾È˶ԼÆËãȷʵ²»Ì«¶®£¬¶øÇÒ¼ÆËãÕâ¿éÔÀ´ÊÇʦÐÖËãµÄ£¬ÏÖÔÚʦÐÖ±ÏÒµ£¬ÎÒ¶ÔÕâÎÊÌâ¸üÎÞ½âÁË£¬Éó¸åÈËÆÀÂÛºÍÎÊÌâ¼ò½éÈçÏ£º This manuscript reports on the synthesis and characterization using usual spectroscopic techniques of two novel cationic cyclopentadienyl-iron-arene complexes containing triphenyl butene substituent as well as their nucleophilic hydroxyl organic precursors. In addition, the optical properties of the mixed sandwich compounds were studied both experimentally and theoretically (DFT/B3LYP and TD-DFT) methods). ÎÊÌ⣺7) the authors should be aware that the dipole moment of an ion is not invariant with respect to a change of the origin. Have they tried to calculate the hyperpolarizabilities with different choices of origin? ÏÂÃæÊDz¿·Ö¼ÆËãÔ´³ÌÐòÄÚÈÝ£º ÀïÃæÒ»ÖÖÎïÖʵÄZ¹¹Ð͵IJ¿·ÖÄÚÈÝ£º %nosave %chk=D:\calculation(Junru Han)\2.chk %mem=1GB # opt freq=savenormalmodes b3pw91/lanl2dz guess=(mix,local,save) pop=npa geom=connectivity scfcon=8 Title Card Required 1 1 C -0.29761905 0.00000000 0.00000000 C -1.00186977 -0.10291912 1.19379033 C -0.36969614 0.18339069 2.40414775 C 0.95935295 0.57603500 2.41930512 C 1.67668178 0.68083245 1.22976466 C 1.04456758 0.39048709 0.01315648 ¡¡ ÁíÒ»¸öEÐͲ¿·ÖÄÚÈÝ£º %nosave %chk=D:\try2\mo\1.chk # rb3lyp/genecp pop=full Title Card Required 1 1 C -0.50477747 0.14851485 -0.01321806 C -1.87921347 0.43661585 0.14665494 C -2.27681547 1.37158985 1.13107394 C -1.30983147 2.02649885 1.92557894 C 0.07722353 1.81381085 1.69965394 ¡¡ C Cl O H 0 6-31g** **** Fe 0 lanl2dz **** Fe 0 lanl2dz Á½¸öÎļþ¼ÆËãÒªÇó²î±ð´ó£¬Õâ¸öÎÒÒ²²»ÖªµÀʦÐÖµ±Ê±Ôõô۵쬲»¹ý´óÖµIJÎÊý¿ÉÒÔ¿´³öÁË¡£½á¹¹ÓÅ»¯ÊÇÓõÄÑ§Ð£ÔÆ¼ÆËãÆ½Ì¨ËãµÄ£¬ÔÙÓÃʵÑéÊÒµçÄÔ×öµÄµ¥µãÄܼÆËã~~ºÃÏñÊÇÕâÑù~~ ÏÂÃæÊÇÎÄÕµIJ¿·ÖÄÚÈÝ£¬Ï£Íû¶ÔÓ¦ÖúÓаïÖú~~ The positive solvatochromism of the UV-Vis absorption of TPE-Fcs upon the increase in solvent polarity was found from the experiment. Quantum chemical calculations of the orbital energy, geometrical structure, absorption spectra, and first hyperpolarizability (¦Â) values of the TPE-Fcs were carried out using density functional (DFT/B3LYP and TD-DFT) methods. The experimental results showed that the observed spectra were in good agreement with the calculated values. The calculated HOMO and LUMO energies showed that the compounds exhibit charge transfer that mediated by the metal center. ¡¡ In the present work, we have used density functional theory (DFT) at the Becke 3-Lee-Yang-Parr (B3LYP)/Genecp (Fe with Lanl2dz basis set and C, H, N, and O with 6-31G** basic set) basis set level for the computation of molecular structure and energies of the optimized structures in the ground state. The entire calculations were performed by using Gaussian09 program package. The absorption spectra of TPE-Fcs were calculated using the time-dependent density functional theory (TD-DFT) method from the gas phase optimized geometries. ¡¡ The enhancement of charge separation is known to favor large NLO responses. The electrostatic first hyperpolarizability (¦Â) was calculated using the Gaussian 09 package. Based on the calculated electronic properties and geometries, the electrostatic first hyperpolarizability ¦Â¦Ì were calculated using the DFT/B3LYP method. The ¦Â¦Ì of the title compounds are shown in Table 4. The second-order optical susceptibility of the target compounds followed the order: ¦Â¦Ì (TPE) < ¦Â¦Ì (TPE-Fc) and ¦Â¦Ì (Z) < ¦Â¦Ì (E). This trend is attributed to the intermolecular charge-transfer of the TPE-Fc compounds. In the presence of the electron-rich diphenyl ether and diphenyl sulfide moiety as a strong donor-group and the cationic cyclopentadienyliron fragment as a strong acceptor-group led to a larger value of ¦Â¦Ì (TPE-Fcs) than our previous study. This switching of electron delocalization directly affected the NLO coefficient, which could generate push¨Cpull systems. Such systems favor the generation of large NLO responses. Sample Text |
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jiqiang
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The dipole moment (¦Ì), mean polarizability (¦Á), and total first static hyperpolarizability (¦Â) of TPE-Fcs were calculated in terms of x, y, z components, which are given by the following equations: ¦Ì=(¦Ìx2+¦Ìy2+¦Ìz2)1/2 (1) ¦Á=(¦Áxx+¦Áyy+¦Ázz)/3 (2) ¦Â=(¦Âx2+¦Ây2+¦Âz2)1/2 (3) ¦Âj=¦Âjjj+¡Æ(¦Âjii+2¦Âijj)/3 (i¡Ùj; i, j=x, y, z) The ¦Â components of Gaussian output are reported on atomic units and therefore the calculated ¦Â components have been converted into electrostatic units ¦Âtot(esu) (1 a.u.=8.6393¡Á10-33esu)[31]. ÉÏ´ÎÍü¼Ç¸ø³öÕâЩÄÚÈÝÁË£¬ÎÊÌâÓ¦¸ÃÊÇÀ´×ÔÕâ¶ùµÄ£¡£¡£¡ |
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jiqiang
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- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 2907.5
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- ³æºÅ: 616592
- ×¢²á: 2008-10-04
- רҵ: Óлú·Ö×Ó¹¦ÄܲÄÁÏ»¯Ñ§
2Â¥2014-02-22 11:35:24













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