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The experimental work is supported by by theoretical DFT calculation using Gaussian software.Calculations confirmed stability of determined structure. Authors also calculated UV-Vis spectra by means of TDDFT and conclude that experimentally observed spectrum is in good agreement with calculated one. At this point I do not agree with the claim that calculation agrees well with experiment, but, understandably, more precise calculation (e.g. by means of GW and Bethe Salpeter equation) is too demanding for such large system. Experimentally unobserved peaks in calculated spectra are of the same intensity as observed one, thus natural question is if the calculated oscillator strength is overestimated for the peaks at 449nm and 374nm or the problem is more deep due to some TDDFT deficiency (e.g. HOMO-LUMO gap underestimate) and both peaks positions and also intensities are in question. I would welcome if the authors can comment this point. [ Last edited by brilliant on 2010-3-10 at 06:52 ] |
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brilliant(½ð±Ò+5):лл 2010-03-08 13:48
mingdong(½ð±Ò+1):¸Ðл½»Á÷£¡ 2010-03-08 23:14
brilliant(½ð±Ò+5):лл 2010-03-08 13:48
mingdong(½ð±Ò+1):¸Ðл½»Á÷£¡ 2010-03-08 23:14
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2Â¥2010-03-08 13:27:31
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fegg7502(½ð±Ò+1):¹ÄÀø½»Á÷ 2010-03-09 16:25
fegg7502(½ð±Ò+1):¹ÄÀø½»Á÷ 2010-03-09 16:25
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The gas phase geometry of the Í complex was optimized without any symmetry restriction in the doublet state with the DFT method using the hybrid B3LYP functional of GAUSSIAN-03. The calculation was performed by using the standard 6-31G* basis set for C, H, N, and O atoms, and effective core potentials basis set of LanL2DZ for Cu atom ÍÅäºÏÎï [ Last edited by brilliant on 2010-3-8 at 13:49 ] |
3Â¥2010-03-08 13:47:35
c111999
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dongdong3881(½ð±Ò+1):¶àл½»Á÷ 2010-03-09 13:33
brilliant(½ð±Ò+15):thanks 2010-03-09 13:40
dongdong3881(½ð±Ò+1):¶àл½»Á÷ 2010-03-09 13:33
brilliant(½ð±Ò+15):thanks 2010-03-09 13:40
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ÕâÊÇʵÑéÎÊÌ⣬Ϊʲô704µÄ·æÄÜʶ±ð£¬±ðµÄ£¨628~374£©Ê¶±ð²»ÁË£¿ Ï£ÍûÄã¸øµÄ±íÊÇÓÃ×÷supporting material ¼ÆËãÖµºÜÄÑÍêÈ«¸úʵÑéÖµÖØºÏ£ºÈÝ»ýЧӦ£¨Î¶ȣ¬ìØ£¬µç×ÓÉþ×ÓñîºÏ¡¡£©£¬DFT±¾ÉíµÄÎÊÌâ¡£ÄãÖ»ÄÜÇ¿µ÷×îÇ¿µÄÁ½¸ö·æËã³öÀ´ÁË¡£ We appreciate the reviewer's comments on some calculated but experimentally unresolved peaks (449 and 374). Oscillator strength may be overstimated in the gas phase than in the solution, i.e. we calculated gas phase molecule, which approximately represents solution result. It is known solution will reduce transition intensity. However, the calculations do capture the major transition peaks, which are also oberved experimentally. In this sense we say the calculations agree with experiments well. |
4Â¥2010-03-09 11:25:23
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fegg7502(½ð±Ò+1):thank you very much! 2010-03-09 16:26
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fegg7502(½ð±Ò+1):thank you very much! 2010-03-09 16:26
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5Â¥2010-03-09 13:50:56
brilliant
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·Ç³£¸ÐлbeeflyÀÏʦºÍc111999 TD-DFT is a formally exact theory that relies on the analysis of the time-dependent linear response of the formally exact ground-state density to a time-dependent external perturbation, which after Fourier transformation yields exact excited-state energies and oscillator strengths. The derivation of the famous Runge-Gross theorem and the subsequent formulation of a time-dependent Kohn-Sham equation were the cornerstones in the development of the TD-DFT formalism. However, since the exact xc functional is not known, approximate xc functionals need to be employed in a practical calculation. Usually the adiabatic local density approximation (ALDA) is employed, and standard time-independent xc functionals derived for ground-state DFT are used. Concomitantly, errors in the excitation energies and oscillator strengths are introduced. [ Last edited by brilliant on 2010-3-10 at 06:56 ] |
6Â¥2010-03-10 06:55:11
c111999
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luoqiquan(½ð±Ò+1):ths 2010-03-10 16:43
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luoqiquan(½ð±Ò+1):ths 2010-03-10 16:43
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ÄãÕâЩ¶¼ÊÇ·Ï»°,ǧÍò±ð˵ÕâÊÇÄã¸ø±à¼µÄ»ØÐÅÀïµÄÄÚÈÝ ¹Ø¼üÊÇÄãÃÇÉù³Æ¼ÆËã½á¹ûÓëʵÑé·ûºÏµÄºÜºÃ£¬ÊDz»×¼È·µÄ¡£ ±ØÐëÇ¿µ÷ÆøÏà¼ÆËãÄ£ÐÍÓëÈÜÒºÖеÄÊÔÑéÊDz»Ò»ÑùµÄ£¬ËùÒÔ½á¹ûÒ²²»Ò»Ñù¡£ [ Last edited by c111999 on 2010-3-10 at 11:37 ] |
7Â¥2010-03-10 11:33:56
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luoqiquan(½ð±Ò+2):thank you 2010-03-11 18:19
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luoqiquan(½ð±Ò+2):thank you 2010-03-11 18:19
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