Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -685.906197 |
| Energy at 298.15K | |
| HF Energy | -685.906197 |
| Nuclear repulsion energy | 616.553821 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HF/LANL2DZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
2295 |
2066 |
395.10 |
|
|
|
| 2 |
A |
2230 |
2007 |
971.52 |
|
|
|
| 3 |
A |
2151 |
1936 |
0.49 |
|
|
|
| 4 |
A |
2098 |
1888 |
5154.62 |
|
|
|
| 5 |
A |
2092 |
1883 |
5281.64 |
|
|
|
| 6 |
A |
568 |
511 |
165.03 |
|
|
|
| 7 |
A |
551 |
496 |
22.71 |
|
|
|
| 8 |
A |
551 |
496 |
25.95 |
|
|
|
| 9 |
A |
541 |
487 |
0.01 |
|
|
|
| 10 |
A |
507 |
456 |
144.07 |
|
|
|
| 11 |
A |
507 |
456 |
142.92 |
|
|
|
| 12 |
A |
413 |
372 |
22.01 |
|
|
|
| 13 |
A |
397 |
357 |
131.38 |
|
|
|
| 14 |
A |
395 |
356 |
126.72 |
|
|
|
| 15 |
A |
389 |
350 |
0.03 |
|
|
|
| 16 |
A |
364 |
328 |
12.04 |
|
|
|
| 17 |
A |
363 |
326 |
13.24 |
|
|
|
| 18 |
A |
305 |
275 |
0.00 |
|
|
|
| 19 |
A |
286 |
258 |
22.47 |
|
|
|
| 20 |
A |
211 |
189 |
0.00 |
|
|
|
| 21 |
A |
110 |
99 |
8.47 |
|
|
|
| 22 |
A |
110 |
99 |
2.03 |
|
|
|
| 23 |
A |
110 |
99 |
8.65 |
|
|
|
| 24 |
A |
104 |
94 |
0.00 |
|
|
|
| 25 |
A |
82 |
74 |
6.83 |
|
|
|
| 26 |
A |
82 |
73 |
7.07 |
|
|
|
| 27 |
A |
48i |
43i |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8881.3 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 7992.3 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HF/LANL2DZ
Point Group is C1
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Fe |
-0.133 |
|
|
|
| 2 |
C |
0.338 |
|
|
|
| 3 |
C |
0.226 |
|
|
|
| 4 |
C |
0.225 |
|
|
|
| 5 |
C |
0.226 |
|
|
|
| 6 |
C |
0.224 |
|
|
|
| 7 |
O |
-0.207 |
|
|
|
| 8 |
O |
-0.224 |
|
|
|
| 9 |
O |
-0.225 |
|
|
|
| 10 |
O |
-0.224 |
|
|
|
| 11 |
O |
-0.225 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.004 |
-0.010 |
2.252 |
2.252 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-77.360 |
0.001 |
-0.006 |
| y |
0.001 |
-77.539 |
0.010 |
| z |
-0.006 |
0.010 |
-74.730 |
|
| Traceless |
| | x | y | z |
| x |
-1.225 |
0.001 |
-0.006 |
| y |
0.001 |
-1.494 |
0.010 |
| z |
-0.006 |
0.010 |
2.720 |
|
| Polar |
| 3z2-r2 | 5.439 |
| x2-y2 | 0.179 |
| xy | 0.001 |
| xz | -0.006 |
| yz | 0.010 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
22.676 |
0.001 |
0.002 |
| y |
0.001 |
22.905 |
-0.000 |
| z |
0.002 |
-0.000 |
12.597 |
<r2> (average value of r
2) Å
2
| <r2> |
539.406 |
| (<r2>)1/2 |
23.225 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -685.908326 |
| Energy at 298.15K | -685.906076 |
| HF Energy | -685.908326 |
| Nuclear repulsion energy | 618.221541 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HF/LANL2DZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1' |
2308 |
2077 |
0.00 |
|
|
|
| 2 |
A1' |
2212 |
1990 |
0.00 |
|
|
|
| 3 |
A1' |
378 |
340 |
0.00 |
|
|
|
| 4 |
A1' |
237 |
214 |
0.00 |
|
|
|
| 5 |
A2' |
397 |
357 |
0.00 |
|
|
|
| 6 |
A2" |
2274 |
2046 |
1450.50 |
|
|
|
| 7 |
A2" |
552 |
497 |
31.02 |
|
|
|
| 8 |
A2" |
333 |
299 |
34.76 |
|
|
|
| 9 |
A2" |
117 |
105 |
3.18 |
|
|
|
| 10 |
E' |
2041 |
1837 |
6196.56 |
|
|
|
| 10 |
E' |
2041 |
1837 |
6196.56 |
|
|
|
| 11 |
E' |
576 |
518 |
229.40 |
|
|
|
| 11 |
E' |
576 |
518 |
229.40 |
|
|
|
| 12 |
E' |
466 |
419 |
8.75 |
|
|
|
| 12 |
E' |
466 |
419 |
8.75 |
|
|
|
| 13 |
E' |
431 |
388 |
105.35 |
|
|
|
| 13 |
E' |
431 |
388 |
105.36 |
|
|
|
| 14 |
E' |
102 |
92 |
7.97 |
|
|
|
| 14 |
E' |
102 |
92 |
7.97 |
|
|
|
| 15 |
E' |
37 |
33 |
13.62 |
|
|
|
| 15 |
E' |
37 |
33 |
13.62 |
|
|
|
| 16 |
E" |
528 |
475 |
0.00 |
|
|
|
| 16 |
E" |
528 |
475 |
0.00 |
|
|
|
| 17 |
E" |
302 |
272 |
0.00 |
|
|
|
| 17 |
E" |
302 |
272 |
0.00 |
|
|
|
| 18 |
E" |
96 |
86 |
0.00 |
|
|
|
| 18 |
E" |
96 |
86 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8981.1 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 8082.1 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HF/LANL2DZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Fe1 |
0.000 |
0.000 |
0.000 |
| C2 |
0.000 |
0.000 |
2.023 |
| C3 |
0.000 |
1.867 |
0.000 |
| C4 |
1.617 |
-0.933 |
0.000 |
| C5 |
-1.617 |
-0.933 |
0.000 |
| C6 |
0.000 |
0.000 |
-2.023 |
| O7 |
0.000 |
0.000 |
3.155 |
| O8 |
0.000 |
3.011 |
0.000 |
| O9 |
2.608 |
-1.506 |
0.000 |
| O10 |
-2.608 |
-1.506 |
0.000 |
| O11 |
0.000 |
0.000 |
-3.155 |
Atom - Atom Distances (Å)
| |
Fe1 |
C2 |
C3 |
C4 |
C5 |
C6 |
O7 |
O8 |
O9 |
O10 |
O11 |
| Fe1 | | 2.0226 | 1.8667 | 1.8667 | 1.8667 | 2.0226 | 3.1550 | 3.0114 | 3.0114 | 3.0114 | 3.1550 |
C2 | 2.0226 | | 2.7523 | 2.7523 | 2.7523 | 4.0452 | 1.1324 | 3.6276 | 3.6276 | 3.6276 | 5.1776 | C3 | 1.8667 | 2.7523 | | 3.2331 | 3.2331 | 2.7523 | 3.6658 | 1.1448 | 4.2631 | 4.2631 | 3.6658 | C4 | 1.8667 | 2.7523 | 3.2331 | | 3.2331 | 2.7523 | 3.6658 | 4.2631 | 1.1448 | 4.2631 | 3.6658 | C5 | 1.8667 | 2.7523 | 3.2331 | 3.2331 | | 2.7523 | 3.6658 | 4.2631 | 4.2631 | 1.1448 | 3.6658 | C6 | 2.0226 | 4.0452 | 2.7523 | 2.7523 | 2.7523 | | 5.1776 | 3.6276 | 3.6276 | 3.6276 | 1.1324 | O7 | 3.1550 | 1.1324 | 3.6658 | 3.6658 | 3.6658 | 5.1776 | | 4.3615 | 4.3615 | 4.3615 | 6.3100 | O8 | 3.0114 | 3.6276 | 1.1448 | 4.2631 | 4.2631 | 3.6276 | 4.3615 | | 5.2159 | 5.2159 | 4.3615 | O9 | 3.0114 | 3.6276 | 4.2631 | 1.1448 | 4.2631 | 3.6276 | 4.3615 | 5.2159 | | 5.2159 | 4.3615 | O10 | 3.0114 | 3.6276 | 4.2631 | 4.2631 | 1.1448 | 3.6276 | 4.3615 | 5.2159 | 5.2159 | | 4.3615 | O11 | 3.1550 | 5.1776 | 3.6658 | 3.6658 | 3.6658 | 1.1324 | 6.3100 | 4.3615 | 4.3615 | 4.3615 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Fe1 |
C2 |
O7 |
180.000 |
|
Fe1 |
C3 |
O8 |
180.000 |
| Fe1 |
C4 |
O9 |
180.000 |
|
Fe1 |
C5 |
O10 |
180.000 |
| Fe1 |
C6 |
O11 |
180.000 |
|
C2 |
Fe1 |
C3 |
90.000 |
| C2 |
Fe1 |
C4 |
90.000 |
|
C2 |
Fe1 |
C5 |
90.000 |
| C2 |
Fe1 |
C6 |
180.000 |
|
C3 |
Fe1 |
C4 |
120.000 |
| C3 |
Fe1 |
C5 |
120.000 |
|
C3 |
Fe1 |
C6 |
90.000 |
| C4 |
Fe1 |
C5 |
120.000 |
|
C4 |
Fe1 |
C6 |
90.000 |
| C5 |
Fe1 |
C6 |
90.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Fe |
-0.178 |
|
|
|
| 2 |
C |
0.285 |
|
|
|
| 3 |
C |
0.249 |
|
|
|
| 4 |
C |
0.249 |
|
|
|
| 5 |
C |
0.249 |
|
|
|
| 6 |
C |
0.285 |
|
|
|
| 7 |
O |
-0.187 |
|
|
|
| 8 |
O |
-0.255 |
|
|
|
| 9 |
O |
-0.255 |
|
|
|
| 10 |
O |
-0.255 |
|
|
|
| 11 |
O |
-0.187 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-78.141 |
0.000 |
0.000 |
| y |
0.000 |
-78.141 |
0.000 |
| z |
0.000 |
0.000 |
-71.655 |
|
| Traceless |
| | x | y | z |
| x |
-3.243 |
0.000 |
0.000 |
| y |
0.000 |
-3.243 |
0.000 |
| z |
0.000 |
0.000 |
6.485 |
|
| Polar |
| 3z2-r2 | 12.971 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
24.174 |
0.000 |
0.000 |
| y |
0.000 |
24.174 |
0.000 |
| z |
0.000 |
0.000 |
13.140 |
<r2> (average value of r
2) Å
2
| <r2> |
536.175 |
| (<r2>)1/2 |
23.155 |