Jump to
S1C2
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -747.913981 |
Energy at 298.15K | |
HF Energy | -747.913981 |
Nuclear repulsion energy | 557.624349 |
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 |
Ag |
2035 |
1831 |
0.00 |
|
|
|
2 |
Ag |
1498 |
1348 |
0.00 |
|
|
|
3 |
Ag |
1372 |
1235 |
0.00 |
|
|
|
4 |
Ag |
1222 |
1100 |
0.00 |
|
|
|
5 |
Ag |
725 |
652 |
0.00 |
|
|
|
6 |
Ag |
601 |
541 |
0.00 |
|
|
|
7 |
Ag |
391 |
352 |
0.00 |
|
|
|
8 |
Ag |
359 |
323 |
0.00 |
|
|
|
9 |
Ag |
230 |
207 |
0.00 |
|
|
|
10 |
Au |
654 |
588 |
13.45 |
|
|
|
11 |
Au |
362 |
326 |
19.04 |
|
|
|
12 |
Au |
126 |
113 |
0.67 |
|
|
|
13 |
Au |
32i |
29i |
0.15 |
|
|
|
14 |
Bg |
755 |
679 |
0.00 |
|
|
|
15 |
Bg |
503 |
452 |
0.00 |
|
|
|
16 |
Bg |
194 |
175 |
0.00 |
|
|
|
17 |
Bu |
1958 |
1762 |
378.11 |
|
|
|
18 |
Bu |
1387 |
1248 |
376.78 |
|
|
|
19 |
Bu |
1248 |
1123 |
293.36 |
|
|
|
20 |
Bu |
980 |
882 |
284.16 |
|
|
|
21 |
Bu |
638 |
574 |
7.29 |
|
|
|
22 |
Bu |
498 |
448 |
12.68 |
|
|
|
23 |
Bu |
303 |
272 |
11.58 |
|
|
|
24 |
Bu |
141 |
127 |
2.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9071.3 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 8163.3 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 C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.156 |
1.852 |
0.000 |
C2 |
0.459 |
0.569 |
0.000 |
C3 |
-0.459 |
-0.569 |
0.000 |
C4 |
-0.156 |
-1.852 |
0.000 |
F5 |
1.080 |
2.820 |
0.000 |
F6 |
-1.080 |
2.362 |
0.000 |
F7 |
1.785 |
0.233 |
0.000 |
F8 |
-1.785 |
-0.233 |
0.000 |
F9 |
1.080 |
-2.362 |
0.000 |
F10 |
-1.080 |
-2.820 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
C4 |
F5 |
F6 |
F7 |
F8 |
F9 |
F10 |
C1 | | 1.3185 | 2.4972 | 3.7166 | 1.3387 | 1.3367 | 2.2970 | 2.8477 | 4.3140 | 4.8324 |
C2 | 1.3185 | | 1.4614 | 2.4972 | 2.3354 | 2.3631 | 1.3678 | 2.3824 | 2.9957 | 3.7217 | C3 | 2.4972 | 1.4614 | | 1.3185 | 3.7217 | 2.9957 | 2.3824 | 1.3678 | 2.3631 | 2.3354 | C4 | 3.7166 | 2.4972 | 1.3185 | | 4.8324 | 4.3140 | 2.8477 | 2.2970 | 1.3367 | 1.3387 | F5 | 1.3387 | 2.3354 | 3.7217 | 4.8324 | | 2.2080 | 2.6817 | 4.1863 | 5.1820 | 6.0394 | F6 | 1.3367 | 2.3631 | 2.9957 | 4.3140 | 2.2080 | | 3.5695 | 2.6886 | 5.1943 | 5.1820 | F7 | 2.2970 | 1.3678 | 2.3824 | 2.8477 | 2.6817 | 3.5695 | | 3.5997 | 2.6886 | 4.1863 | F8 | 2.8477 | 2.3824 | 1.3678 | 2.2970 | 4.1863 | 2.6886 | 3.5997 | | 3.5695 | 2.6817 | F9 | 4.3140 | 2.9957 | 2.3631 | 1.3367 | 5.1820 | 5.1943 | 2.6886 | 3.5695 | | 2.2080 | F10 | 4.8324 | 3.7217 | 2.3354 | 1.3387 | 6.0394 | 5.1820 | 4.1863 | 2.6817 | 2.2080 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
127.798 |
|
C1 |
C2 |
F7 |
117.524 |
C2 |
C1 |
F5 |
123.025 |
|
C2 |
C1 |
F6 |
125.739 |
C2 |
C3 |
C4 |
127.798 |
|
C2 |
C3 |
F8 |
114.677 |
C3 |
C2 |
F7 |
114.677 |
|
C3 |
C4 |
F9 |
125.739 |
C3 |
C4 |
F10 |
123.025 |
|
C4 |
C3 |
F8 |
117.524 |
F5 |
C1 |
F6 |
111.235 |
|
F9 |
C4 |
F10 |
111.235 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.592 |
|
|
|
2 |
C |
0.228 |
|
|
|
3 |
C |
0.228 |
|
|
|
4 |
C |
0.592 |
|
|
|
5 |
F |
-0.268 |
|
|
|
6 |
F |
-0.260 |
|
|
|
7 |
F |
-0.291 |
|
|
|
8 |
F |
-0.291 |
|
|
|
9 |
F |
-0.260 |
|
|
|
10 |
F |
-0.268 |
|
|
|
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 |
-63.070 |
-0.377 |
0.000 |
y |
-0.377 |
-60.361 |
0.000 |
z |
0.000 |
0.000 |
-49.738 |
|
Traceless |
| x | y | z |
x |
-8.020 |
-0.377 |
0.000 |
y |
-0.377 |
-3.957 |
0.000 |
z |
0.000 |
0.000 |
11.977 |
|
Polar |
3z2-r2 | 23.955 |
x2-y2 | -2.709 |
xy | -0.377 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.549 |
-0.577 |
0.000 |
y |
-0.577 |
11.094 |
0.000 |
z |
0.000 |
0.000 |
2.749 |
<r2> (average value of r
2) Å
2
<r2> |
427.760 |
(<r2>)1/2 |
20.682 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -747.915936 |
Energy at 298.15K | -747.917322 |
HF Energy | -747.915936 |
Nuclear repulsion energy | 560.685782 |
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 |
2030 |
1826 |
86.20 |
|
|
|
2 |
A |
1467 |
1320 |
32.57 |
|
|
|
3 |
A |
1390 |
1251 |
137.91 |
|
|
|
4 |
A |
1179 |
1061 |
283.14 |
|
|
|
5 |
A |
768 |
691 |
0.73 |
|
|
|
6 |
A |
716 |
645 |
1.69 |
|
|
|
7 |
A |
552 |
497 |
0.18 |
|
|
|
8 |
A |
484 |
436 |
2.49 |
|
|
|
9 |
A |
389 |
350 |
3.34 |
|
|
|
10 |
A |
276 |
248 |
0.03 |
|
|
|
11 |
A |
201 |
181 |
0.65 |
|
|
|
12 |
A |
103 |
93 |
1.16 |
|
|
|
13 |
A |
48 |
44 |
0.00 |
|
|
|
14 |
B |
1993 |
1794 |
200.10 |
|
|
|
15 |
B |
1386 |
1247 |
246.99 |
|
|
|
16 |
B |
1253 |
1128 |
132.40 |
|
|
|
17 |
B |
998 |
898 |
188.51 |
|
|
|
18 |
B |
701 |
631 |
8.99 |
|
|
|
19 |
B |
642 |
577 |
8.62 |
|
|
|
20 |
B |
579 |
521 |
8.65 |
|
|
|
21 |
B |
431 |
388 |
13.14 |
|
|
|
22 |
B |
308 |
277 |
8.15 |
|
|
|
23 |
B |
219 |
197 |
8.63 |
|
|
|
24 |
B |
121 |
109 |
1.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9116.4 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 8203.9 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 C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.162 |
1.581 |
-0.365 |
C2 |
0.156 |
0.714 |
0.571 |
C3 |
-0.156 |
-0.714 |
0.571 |
C4 |
0.162 |
-1.581 |
-0.365 |
F5 |
0.156 |
2.876 |
-0.345 |
F6 |
-0.848 |
1.258 |
-1.470 |
F7 |
0.829 |
1.158 |
1.677 |
F8 |
-0.829 |
-1.158 |
1.677 |
F9 |
0.848 |
-1.258 |
-1.470 |
F10 |
-0.156 |
-2.876 |
-0.345 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
C4 |
F5 |
F6 |
F7 |
F8 |
F9 |
F10 |
C1 | | 1.3149 | 2.4784 | 3.1781 | 1.3338 | 1.3408 | 2.3091 | 3.4807 | 3.2090 | 4.4570 |
C2 | 1.3149 | | 1.4613 | 2.4784 | 2.3486 | 2.3391 | 1.3688 | 2.3865 | 2.9214 | 3.7183 | C3 | 2.4784 | 1.4613 | | 1.3149 | 3.7183 | 2.9214 | 2.3865 | 1.3688 | 2.3391 | 2.3486 | C4 | 3.1781 | 2.4784 | 1.3149 | | 4.4570 | 3.2090 | 3.4807 | 2.3091 | 1.3408 | 1.3338 | F5 | 1.3338 | 2.3486 | 3.7183 | 4.4570 | | 2.2121 | 2.7384 | 4.6186 | 4.3397 | 5.7608 | F6 | 1.3408 | 2.3391 | 2.9214 | 3.2090 | 2.2121 | | 3.5681 | 3.9673 | 3.0339 | 4.3397 | F7 | 2.3091 | 1.3688 | 2.3865 | 3.4807 | 2.7384 | 3.5681 | | 2.8477 | 3.9673 | 4.6186 | F8 | 3.4807 | 2.3865 | 1.3688 | 2.3091 | 4.6186 | 3.9673 | 2.8477 | | 3.5681 | 2.7384 | F9 | 3.2090 | 2.9214 | 2.3391 | 1.3408 | 4.3397 | 3.0339 | 3.9673 | 3.5681 | | 2.2121 | F10 | 4.4570 | 3.7183 | 2.3486 | 1.3338 | 5.7608 | 4.3397 | 4.6186 | 2.7384 | 2.2121 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
126.356 |
|
C1 |
C2 |
F7 |
118.712 |
C2 |
C1 |
F5 |
124.919 |
|
C2 |
C1 |
F6 |
123.476 |
C2 |
C3 |
C4 |
126.356 |
|
C2 |
C3 |
F8 |
114.927 |
C3 |
C2 |
F7 |
114.927 |
|
C3 |
C4 |
F9 |
123.476 |
C3 |
C4 |
F10 |
124.919 |
|
C4 |
C3 |
F8 |
118.712 |
F5 |
C1 |
F6 |
111.605 |
|
F9 |
C4 |
F10 |
111.605 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.601 |
|
|
|
2 |
C |
0.227 |
|
|
|
3 |
C |
0.227 |
|
|
|
4 |
C |
0.601 |
|
|
|
5 |
F |
-0.263 |
|
|
|
6 |
F |
-0.271 |
|
|
|
7 |
F |
-0.294 |
|
|
|
8 |
F |
-0.294 |
|
|
|
9 |
F |
-0.271 |
|
|
|
10 |
F |
-0.263 |
|
|
|
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 |
-0.797 |
0.797 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-53.101 |
-2.475 |
0.000 |
y |
-2.475 |
-59.927 |
0.000 |
z |
0.000 |
0.000 |
-60.280 |
|
Traceless |
| x | y | z |
x |
7.002 |
-2.475 |
0.000 |
y |
-2.475 |
-3.237 |
0.000 |
z |
0.000 |
0.000 |
-3.766 |
|
Polar |
3z2-r2 | -7.531 |
x2-y2 | 6.826 |
xy | -2.475 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.687 |
-0.145 |
0.000 |
y |
-0.145 |
7.885 |
0.000 |
z |
0.000 |
0.000 |
6.312 |
<r2> (average value of r
2) Å
2
<r2> |
397.253 |
(<r2>)1/2 |
19.931 |