Vibrational Frequencies calculated at B1B95/3-21G
| 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 |
3556 |
3402 |
12.64 |
|
|
|
| 2 |
A |
3298 |
3156 |
23.56 |
|
|
|
| 3 |
A |
3140 |
3005 |
16.85 |
|
|
|
| 4 |
A |
1515 |
1450 |
3.62 |
|
|
|
| 5 |
A |
1372 |
1312 |
31.06 |
|
|
|
| 6 |
A |
1166 |
1115 |
56.53 |
|
|
|
| 7 |
A |
1051 |
1005 |
74.31 |
|
|
|
| 8 |
A |
597 |
571 |
136.39 |
|
|
|
| 9 |
A |
444 |
425 |
81.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8069.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 7720.1 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 B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.225 |
|
|
|
| 2 |
O |
-0.530 |
|
|
|
| 3 |
H |
0.207 |
|
|
|
| 4 |
H |
0.176 |
|
|
|
| 5 |
H |
0.372 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.016 |
1.695 |
0.203 |
1.707 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.132 |
-2.311 |
0.787 |
| y |
-2.311 |
-10.772 |
-0.043 |
| z |
0.787 |
-0.043 |
-13.776 |
|
| Traceless |
| | x | y | z |
| x |
1.142 |
-2.311 |
0.787 |
| y |
-2.311 |
1.682 |
-0.043 |
| z |
0.787 |
-0.043 |
-2.824 |
|
| Polar |
| 3z2-r2 | -5.648 |
| x2-y2 | -0.360 |
| xy | -2.311 |
| xz | 0.787 |
| yz | -0.043 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.626 |
-0.211 |
0.042 |
| y |
-0.211 |
2.059 |
-0.004 |
| z |
0.042 |
-0.004 |
0.802 |
<r2> (average value of r
2) Å
2
| <r2> |
20.757 |
| (<r2>)1/2 |
4.556 |