Vibrational Frequencies calculated at mPW1PW91/STO-3G
| 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' |
3770 |
3313 |
5.19 |
|
|
|
| 2 |
A' |
3741 |
3288 |
177.80 |
|
|
|
| 3 |
A' |
2496 |
2193 |
15.16 |
|
|
|
| 4 |
A' |
1438 |
1264 |
45.10 |
|
|
|
| 5 |
A' |
1071 |
942 |
25.08 |
|
|
|
| 6 |
A' |
744 |
654 |
18.12 |
|
|
|
| 7 |
A' |
392 |
345 |
7.58 |
|
|
|
| 8 |
A" |
627 |
551 |
30.10 |
|
|
|
| 9 |
A" |
415 |
365 |
0.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7347.0 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 6457.3 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.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.015 |
|
|
|
| 2 |
C |
-0.165 |
|
|
|
| 3 |
O |
-0.202 |
|
|
|
| 4 |
H |
0.116 |
|
|
|
| 5 |
H |
0.235 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.467 |
-0.352 |
0.000 |
1.509 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.488 |
-2.501 |
0.000 |
| y |
-2.501 |
-12.606 |
0.000 |
| z |
0.000 |
0.000 |
-16.233 |
|
| Traceless |
| | x | y | z |
| x |
-0.068 |
-2.501 |
0.000 |
| y |
-2.501 |
2.755 |
0.000 |
| z |
0.000 |
0.000 |
-2.687 |
|
| Polar |
| 3z2-r2 | -5.373 |
| x2-y2 | -1.882 |
| xy | -2.501 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.871 |
-0.578 |
0.000 |
| y |
-0.578 |
3.668 |
0.000 |
| z |
0.000 |
0.000 |
0.320 |
<r2> (average value of r
2) Å
2
| <r2> |
40.910 |
| (<r2>)1/2 |
6.396 |