Vibrational Frequencies calculated at B3PW91/6-31G*
| 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 |
3220 |
3081 |
26.74 |
|
|
|
| 2 |
A1 |
2259 |
2161 |
535.58 |
|
|
|
| 3 |
A1 |
1429 |
1367 |
17.31 |
|
|
|
| 4 |
A1 |
1185 |
1133 |
7.79 |
|
|
|
| 5 |
B1 |
591 |
566 |
76.96 |
|
|
|
| 6 |
B1 |
545 |
522 |
84.49 |
|
|
|
| 7 |
B2 |
3313 |
3170 |
7.81 |
|
|
|
| 8 |
B2 |
999 |
955 |
9.92 |
|
|
|
| 9 |
B2 |
440 |
421 |
2.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6990.6 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 6687.9 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.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.560 |
|
|
|
| 2 |
C |
0.489 |
|
|
|
| 3 |
O |
-0.380 |
|
|
|
| 4 |
H |
0.225 |
|
|
|
| 5 |
H |
0.225 |
|
|
|
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 |
-1.508 |
1.508 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.000 |
0.000 |
-1.544 |
1.544 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.399 |
0.000 |
0.000 |
| y |
0.000 |
-14.838 |
0.000 |
| z |
0.000 |
0.000 |
-17.496 |
|
| Traceless |
| | x | y | z |
| x |
-2.232 |
0.000 |
0.000 |
| y |
0.000 |
3.110 |
0.000 |
| z |
0.000 |
0.000 |
-0.878 |
|
| Polar |
| 3z2-r2 | -1.755 |
| x2-y2 | -3.561 |
| 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 |
1.486 |
0.000 |
0.000 |
| y |
0.000 |
2.256 |
0.000 |
| z |
0.000 |
0.000 |
5.369 |
<r2> (average value of r
2) Å
2
| <r2> |
40.258 |
| (<r2>)1/2 |
6.345 |