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Illusionist

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# opt freq td=(nstates=6,root=1) b3lyp/6-31+g(d,p)
scrf=(solvent=n,n-dimethylformamide) geom=connectivity
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tiaozaoququ

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Illusionist(½ð±Ò+1): 2011-12-04 13:52:08
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2Â¥2011-12-04 09:12:09
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Illusionist

Òø³æ (ÕýʽдÊÖ)

ÒýÓûØÌû:
2Â¥: Originally posted by tiaozaoququ at 2011-12-04 09:12:09:
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3Â¥2011-12-04 10:52:20
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Illusionist

Òø³æ (ÕýʽдÊÖ)

Illusionist: »ØÌûÖö¥ 2011-12-04 14:04:30
=================================
Model                : PCM.
Atomic radii         : UFF (Universal Force Field).
Polarization charges : Total charges.
Charge compensation  : None.
Solution method      : Matrix inversion.
Cavity type          : Scaled VdW (van der Waals Surface) (Alpha=1.100).
Cavity algorithm     : GePol (No added spheres)
                        Default sphere list used, NSphG=   56.
                        Lebedev-Laikov grids with approx.  5.0 points / Ang**2.
                        Smoothing algorithm: Karplus/York (Gamma=1.0000).
                        Polarization charges: spherical gaussians, with
                                              point-specific exponents (IZeta= 3).
                        Self-potential: point-specific (ISelfS= 7).
                        Self-field    : sphere-specific E.n sum rule (ISelfD= 2).
1st derivatives      : Analytical E(r).r(x)/FMM algorithm (CHGder, D1EAlg=3).
                        Cavity 1st derivative terms included.
Solvent              : n,n-DiMethylFormamide, Eps=  37.219000 Eps(inf)=   2.046330
4Â¥2011-12-04 11:53:15
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

Jasminer

Ìú¸Ëľ³æ (ÖøÃûдÊÖ)

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Illusionist(½ð±Ò+2): лл 2011-12-04 13:51:59
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5Â¥2011-12-04 12:48:07
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Illusionist

Òø³æ (ÕýʽдÊÖ)

ÄÚÈÝÒÑɾ³ý
6Â¥2011-12-04 13:51:47
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

Illusionist

Òø³æ (ÕýʽдÊÖ)

°´ÕÕ˵Ã÷ÊéÉϼÆË㣬µ½µÚËIJ½µÄʱºò£¬Ã»ÓÐʹÓÃOPT=RCFC£¬¶øÖ±½ÓʹÓÃOPT¡£ÒòΪʹÓÃOPT=RCFCÎÞ·¨½øÐС£ÕâÒ»²½Ö®Ç°£¬¿´µÄHOMO£¬LUMO
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Step 1: Ground state geometry optimization and frequencies (equilibrium solvation). This is a standard Opt Freq calculation on the ground state including PCM equilibrium solvation.

%chk=01-ac
# B3LYP/6-31+G(d,p) Opt Freq SCRF=(Solvent=Ethanol)

Acetaldehyde ground state

0 1
C
C,1,RA
X,2,1.,1,A
O,2,RB,3,A,1,180.,0
X,1,1.,2,90.,3,0.,0
H,1,R1,2,A1,5,0.,0
H,1,R23,2,A23,5,B23,0
H,1,R23,2,A23,5,-B23,0
H,2,R4,1,A4,3,180.,0

RA=1.53643
RB=1.21718
R1=1.08516
R23=1.08688
R4=1.10433
A=62.1511
A1=110.51212
A23=109.88119
A4=114.26114
B23=120.56468
Step 2: Vertical excitation with linear response solvation. This is a TD-DFT calculation of the vertical excitation, therefore at the ground state equilibrium geometry, with the default solvation: linear response, non-equilibrium. We perform a single-point TD-DFT calculation, which defaults to non-equilibrium solvation. The results of this job will be used to identify which state or states are of interest and their ordering. These results give a reasonable description of the solvation of the excited state, but not quite as good as that from a state-specific solvation calculation. In this case, we see that the n->¦Ð* state is the first excited state. Next, we will use the state-specific method to produce a better description of the vertical excitation step.

%chk=02-ac
# B3LYP/6-31+G(d,p) TD=NStates=6 SCRF=(Solvent=Ethanol)
  Geom=Check Guess=Read

Acetaldehyde: linear response vertical excited states

0 1
Step 3: State-specific solvation of the vertical excitation. This will require two job steps: first the ground state calculation is done, specifying NonEq=write in the PCM input section, in order to store the information about non-equilibrium solvation based on the ground state. Second, the actual state-specific calculation is done, reading in the necessary information for non-equilibrium solvation using NonEq=read.

%chk=03-ac
# B3LYP/6-31+G(d,p) SCRF=(Solvent=Ethanol,Read)
  Geom=Check Guess=Read

Acetaldehyde: prepare for state-specific non-eq solvation
by saving the solvent reaction field from the ground state

0 1

NonEq=write

--link1--
%chk=03-ac
# B3LYP/6-31+G(d,p) TD(NStates=6,Root=1)
  SCRF=(Solvent=Ethanol,ExternalIteration,Read)
  Geom=Check Guess=Read

Acetaldehyde: read non-eq solvation from ground state and
compute energy of the first excited with the state-specific method

0 1

NonEq=read
Step 4: Relaxation of the excited state geometry. Next, we perform a TD-DFT geometry optimization, with equilibrium, linear response solvation, in order to find the minimum energy point on the excited state potential energy surface. Since this is a TD-DFT optimization, the program defaults to equilibrium solvation. As is typical of such cases, the molecule has a plane of symmetry in the ground state but the symmetry is broken in the excited state, so the ground state geometry is perturbed slightly to break symmetry at the start of the optimization.

%chk=04-ac
# B3LYP/6-31+G(d,p) TD=(Read,NStates=6,Root=1) SCRF=(Solvent=Ethanol)
  Geom=Modify Guess=Read Opt=RCFC

Acetaldehyde: excited state opt
Modify geometry to break Cs symmetry
since first excited state is A"

0 1

4 1 2 3 10.0
5 1 2 7 -50.0
7Â¥2011-12-04 14:09:30
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

sjsznh

Òø³æ (³õÈëÎÄ̳)

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Illusionist(½ð±Ò+5): ±¾À´ÊÇ×óÓҶԳƵĽṹ£¬µ«ÊÇÏÖÔÚHOMOºÍLUMO¶¼²»¶Ô³Æ¡££È£Ï£Í£ÏÖ»ÔÚ×ó±ß£¬£Ì£Õ£Í£ÏÖ»ÔÚÓұߡ£¼´Ê¹ÊÇ·´×ªµÄÎÊÌ⣬£È£Ï£Í£Ï£¬£Ì£Õ£Í£Ï±¾ÉíÒ²Ó¦¸Ã¶Ô³Æ²Å¶Ô°¡¡¤ 2011-12-04 15:06:33
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http://www.gaussian.com/g_tech/rel_notes.pdf
8Â¥2011-12-04 14:25:56
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sjsznh

Òø³æ (³õÈëÎÄ̳)

¡¾´ð°¸¡¿Ó¦Öú»ØÌû

ÒýÓûØÌû:
8Â¥: Originally posted by sjsznh at 2011-12-04 14:25:56:
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9Â¥2011-12-04 14:31:58
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Jasminer

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Illusionist(½ð±Ò+5): ÎÒfreqÁËÁ½ÌìÁË£¬Ã»³öÀ´¡£Èç¹ûÊǽṹûÓÐÓÅ»¯ºÃ£¬ÄǸÃÔõô×ö£¬ÔÚÓÅ»¯Ò»±é£¬»á²»»áÓÖÊÇÕâ½á¹¹¡£¡¤¡¤¡¤ 2011-12-04 15:54:31
ben_ladeng(½ð±Ò+2): ר¼Ò¿¼ºË´æµµ 2011-12-04 16:45:31
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10Â¥2011-12-04 15:28:51
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