Jump to
S1C2
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -278.260311 |
Energy at 298.15K | |
HF Energy | -278.260311 |
Nuclear repulsion energy | 126.074869 |
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 M06-2X/6-311G**
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 |
3088 |
3088 |
0.00 |
211.98 |
0.08 |
0.15 |
2 |
Ag |
1529 |
1529 |
0.00 |
14.80 |
0.75 |
0.86 |
3 |
Ag |
1476 |
1476 |
0.00 |
2.25 |
0.34 |
0.50 |
4 |
Ag |
1120 |
1120 |
0.00 |
9.83 |
0.75 |
0.86 |
5 |
Ag |
1104 |
1104 |
0.00 |
6.09 |
0.21 |
0.35 |
6 |
Ag |
468 |
468 |
0.00 |
2.88 |
0.50 |
0.67 |
7 |
Au |
3162 |
3162 |
46.05 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1250 |
1250 |
5.06 |
0.00 |
0.00 |
0.00 |
9 |
Au |
827 |
827 |
0.11 |
0.00 |
0.00 |
0.00 |
10 |
Au |
125 |
125 |
14.32 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3137 |
3137 |
0.00 |
117.34 |
0.75 |
0.86 |
12 |
Bg |
1309 |
1309 |
0.00 |
13.72 |
0.75 |
0.86 |
13 |
Bg |
1188 |
1188 |
0.00 |
3.73 |
0.75 |
0.86 |
14 |
Bu |
3095 |
3095 |
49.26 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1536 |
1536 |
3.21 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1374 |
1374 |
12.25 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
1129 |
1129 |
209.33 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
283 |
283 |
20.81 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13599.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13599.4 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 M06-2X/6-311G**
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.425 |
0.626 |
0.000 |
C2 |
-0.425 |
-0.626 |
0.000 |
F3 |
-0.425 |
1.716 |
0.000 |
F4 |
0.425 |
-1.716 |
0.000 |
H5 |
1.052 |
0.666 |
0.892 |
H6 |
1.052 |
0.666 |
-0.892 |
H7 |
-1.052 |
-0.666 |
0.892 |
H8 |
-1.052 |
-0.666 |
-0.892 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5136 | 1.3815 | 2.3424 | 1.0913 | 1.0913 | 2.1557 | 2.1557 |
C2 | 1.5136 | | 2.3424 | 1.3815 | 2.1557 | 2.1557 | 1.0913 | 1.0913 | F3 | 1.3815 | 2.3424 | | 3.5355 | 2.0193 | 2.0193 | 2.6200 | 2.6200 | F4 | 2.3424 | 1.3815 | 3.5355 | | 2.6200 | 2.6200 | 2.0193 | 2.0193 | H5 | 1.0913 | 2.1557 | 2.0193 | 2.6200 | | 1.7848 | 2.4898 | 3.0635 | H6 | 1.0913 | 2.1557 | 2.0193 | 2.6200 | 1.7848 | | 3.0635 | 2.4898 | H7 | 2.1557 | 1.0913 | 2.6200 | 2.0193 | 2.4898 | 3.0635 | | 1.7848 | H8 | 2.1557 | 1.0913 | 2.6200 | 2.0193 | 3.0635 | 2.4898 | 1.7848 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
107.929 |
|
C1 |
C2 |
H7 |
110.643 |
C1 |
C2 |
H8 |
110.643 |
|
C2 |
C1 |
F3 |
107.929 |
C2 |
C1 |
H5 |
110.643 |
|
C2 |
C1 |
H6 |
110.643 |
F3 |
C1 |
H5 |
108.930 |
|
F3 |
C1 |
H6 |
108.930 |
F4 |
C2 |
H7 |
108.930 |
|
F4 |
C2 |
H8 |
108.930 |
H5 |
C1 |
H6 |
109.713 |
|
H7 |
C2 |
H8 |
109.713 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.019 |
|
|
|
2 |
C |
0.019 |
|
|
|
3 |
F |
-0.283 |
|
|
|
4 |
F |
-0.283 |
|
|
|
5 |
H |
0.132 |
|
|
|
6 |
H |
0.132 |
|
|
|
7 |
H |
0.132 |
|
|
|
8 |
H |
0.132 |
|
|
|
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 |
-21.962 |
2.957 |
0.000 |
y |
2.957 |
-29.211 |
0.000 |
z |
0.000 |
0.000 |
-21.400 |
|
Traceless |
| x | y | z |
x |
3.344 |
2.957 |
0.000 |
y |
2.957 |
-7.530 |
0.000 |
z |
0.000 |
0.000 |
4.186 |
|
Polar |
3z2-r2 | 8.371 |
x2-y2 | 7.249 |
xy | 2.957 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.588 |
0.050 |
0.000 |
y |
0.050 |
3.566 |
0.000 |
z |
0.000 |
0.000 |
3.353 |
<r2> (average value of r
2) Å
2
<r2> |
87.616 |
(<r2>)1/2 |
9.360 |
Jump to
S1C1
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -278.260914 |
Energy at 298.15K | |
HF Energy | -278.260914 |
Nuclear repulsion energy | 128.313243 |
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 M06-2X/6-311G**
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 |
3130 |
3130 |
16.56 |
88.91 |
0.75 |
0.86 |
2 |
A |
3081 |
3081 |
27.79 |
186.60 |
0.03 |
0.05 |
3 |
A |
1504 |
1504 |
0.00 |
1.42 |
0.75 |
0.86 |
4 |
A |
1464 |
1464 |
17.43 |
2.83 |
0.31 |
0.47 |
5 |
A |
1319 |
1319 |
2.97 |
15.76 |
0.72 |
0.83 |
6 |
A |
1159 |
1159 |
85.71 |
3.67 |
0.65 |
0.79 |
7 |
A |
1142 |
1142 |
7.02 |
1.77 |
0.38 |
0.55 |
8 |
A |
896 |
896 |
23.16 |
5.21 |
0.25 |
0.40 |
9 |
A |
329 |
329 |
0.39 |
0.39 |
0.41 |
0.58 |
10 |
A |
148 |
148 |
3.92 |
0.06 |
0.75 |
0.86 |
11 |
B |
3142 |
3142 |
33.93 |
13.80 |
0.75 |
0.86 |
12 |
B |
3073 |
3073 |
11.70 |
35.90 |
0.75 |
0.86 |
13 |
B |
1502 |
1502 |
9.02 |
11.13 |
0.75 |
0.86 |
14 |
B |
1419 |
1419 |
9.29 |
0.82 |
0.75 |
0.86 |
15 |
B |
1281 |
1281 |
7.29 |
4.80 |
0.75 |
0.86 |
16 |
B |
1130 |
1130 |
52.41 |
3.38 |
0.75 |
0.86 |
17 |
B |
923 |
923 |
37.68 |
3.04 |
0.75 |
0.86 |
18 |
B |
503 |
503 |
17.73 |
0.63 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13572.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13572.1 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 M06-2X/6-311G**
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.267 |
0.702 |
0.513 |
C2 |
-0.267 |
-0.702 |
0.513 |
F3 |
-0.267 |
1.407 |
-0.547 |
F4 |
0.267 |
-1.407 |
-0.547 |
H5 |
-0.013 |
1.209 |
1.441 |
H6 |
1.354 |
0.692 |
0.407 |
H7 |
0.013 |
-1.209 |
1.441 |
H8 |
-1.354 |
-0.692 |
0.407 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5024 | 1.3800 | 2.3608 | 1.0935 | 1.0922 | 2.1394 | 2.1404 |
C2 | 1.5024 | | 2.3608 | 1.3800 | 2.1394 | 2.1404 | 1.0935 | 1.0922 | F3 | 1.3800 | 2.3608 | | 2.8648 | 2.0135 | 2.0114 | 3.2973 | 2.5495 | F4 | 2.3608 | 1.3800 | 2.8648 | | 3.2973 | 2.5495 | 2.0135 | 2.0114 | H5 | 1.0935 | 2.1394 | 2.0135 | 3.2973 | | 1.7898 | 2.4175 | 2.5455 | H6 | 1.0922 | 2.1404 | 2.0114 | 2.5495 | 1.7898 | | 2.5455 | 3.0408 | H7 | 2.1394 | 1.0935 | 3.2973 | 2.0135 | 2.4175 | 2.5455 | | 1.7898 | H8 | 2.1404 | 1.0922 | 2.5495 | 2.0114 | 2.5455 | 3.0408 | 1.7898 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
109.911 |
|
C1 |
C2 |
H7 |
110.010 |
C1 |
C2 |
H8 |
110.168 |
|
C2 |
C1 |
F3 |
109.911 |
C2 |
C1 |
H5 |
110.010 |
|
C2 |
C1 |
H6 |
110.168 |
F3 |
C1 |
H5 |
108.432 |
|
F3 |
C1 |
H6 |
108.340 |
F4 |
C2 |
H7 |
108.432 |
|
F4 |
C2 |
H8 |
108.340 |
H5 |
C1 |
H6 |
109.942 |
|
H7 |
C2 |
H8 |
109.942 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.023 |
|
|
|
2 |
C |
0.023 |
|
|
|
3 |
F |
-0.278 |
|
|
|
4 |
F |
-0.278 |
|
|
|
5 |
H |
0.120 |
|
|
|
6 |
H |
0.135 |
|
|
|
7 |
H |
0.120 |
|
|
|
8 |
H |
0.135 |
|
|
|
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 |
2.769 |
2.769 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.586 |
1.594 |
0.000 |
y |
1.594 |
-26.067 |
0.000 |
z |
0.000 |
0.000 |
-22.200 |
|
Traceless |
| x | y | z |
x |
2.547 |
1.594 |
0.000 |
y |
1.594 |
-4.174 |
0.000 |
z |
0.000 |
0.000 |
1.627 |
|
Polar |
3z2-r2 | 3.253 |
x2-y2 | 4.480 |
xy | 1.594 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.460 |
0.069 |
0.000 |
y |
0.069 |
3.632 |
0.000 |
z |
0.000 |
0.000 |
3.497 |
<r2> (average value of r
2) Å
2
<r2> |
78.812 |
(<r2>)1/2 |
8.878 |