Vibrational Frequencies calculated at BLYP/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 |
A |
3600 |
3571 |
17.68 |
|
|
|
| 2 |
A |
3183 |
3158 |
29.96 |
|
|
|
| 3 |
A |
3038 |
3014 |
29.25 |
|
|
|
| 4 |
A |
1463 |
1451 |
8.49 |
|
|
|
| 5 |
A |
1348 |
1337 |
31.58 |
|
|
|
| 6 |
A |
1159 |
1150 |
68.41 |
|
|
|
| 7 |
A |
1042 |
1033 |
49.29 |
|
|
|
| 8 |
A |
663 |
657 |
61.50 |
|
|
|
| 9 |
A |
455 |
452 |
90.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7975.7 cm
-1
Scaled (by 0.9919) Zero Point Vibrational Energy (zpe) 7911.1 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.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.145 |
|
|
|
| 2 |
O |
-0.493 |
|
|
|
| 3 |
H |
0.135 |
|
|
|
| 4 |
H |
0.114 |
|
|
|
| 5 |
H |
0.390 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.137 |
1.479 |
0.245 |
1.506 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.517 |
2.094 |
-0.737 |
| y |
2.094 |
-10.927 |
-0.056 |
| z |
-0.737 |
-0.056 |
-13.827 |
|
| Traceless |
| | x | y | z |
| x |
0.860 |
2.094 |
-0.737 |
| y |
2.094 |
1.746 |
-0.056 |
| z |
-0.737 |
-0.056 |
-2.605 |
|
| Polar |
| 3z2-r2 | -5.211 |
| x2-y2 | -0.591 |
| xy | 2.094 |
| xz | -0.737 |
| yz | -0.056 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.827 |
0.170 |
-0.063 |
| y |
0.170 |
2.352 |
0.006 |
| z |
-0.063 |
0.006 |
1.194 |
<r2> (average value of r
2) Å
2
| <r2> |
20.732 |
| (<r2>)1/2 |
4.553 |