Vibrational Frequencies calculated at B3PW91/cc-pVTZ
| 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 |
3189 |
3067 |
30.11 |
|
|
|
| 2 |
A1 |
2242 |
2156 |
627.02 |
|
|
|
| 3 |
A1 |
1404 |
1350 |
18.04 |
|
|
|
| 4 |
A1 |
1174 |
1129 |
5.99 |
|
|
|
| 5 |
B1 |
589 |
566 |
43.83 |
|
|
|
| 6 |
B1 |
551 |
530 |
87.11 |
|
|
|
| 7 |
B2 |
3286 |
3160 |
10.40 |
|
|
|
| 8 |
B2 |
981 |
944 |
6.25 |
|
|
|
| 9 |
B2 |
440 |
423 |
2.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6927.5 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 6661.5 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.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.464 |
|
|
|
| 2 |
C |
0.309 |
|
|
|
| 3 |
O |
-0.148 |
|
|
|
| 4 |
H |
0.151 |
|
|
|
| 5 |
H |
0.151 |
|
|
|
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 |
-1.428 |
1.428 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.781 |
0.000 |
0.000 |
| y |
0.000 |
-15.193 |
0.000 |
| z |
0.000 |
0.000 |
-17.733 |
|
| Traceless |
| | x | y | z |
| x |
-2.318 |
0.000 |
0.000 |
| y |
0.000 |
3.064 |
0.000 |
| z |
0.000 |
0.000 |
-0.746 |
|
| Polar |
| 3z2-r2 | -1.492 |
| x2-y2 | -3.588 |
| 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 |
2.410 |
0.000 |
0.000 |
| y |
0.000 |
2.694 |
0.000 |
| z |
0.000 |
0.000 |
5.775 |
<r2> (average value of r
2) Å
2
| <r2> |
40.057 |
| (<r2>)1/2 |
6.329 |