Vibrational Frequencies calculated at PBEPBEultrafine/6-311+G(3df,2pd)
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 |
3801 |
3763 |
81.43 |
|
|
|
2 |
A |
3613 |
3577 |
34.20 |
|
|
|
3 |
A |
3586 |
3550 |
326.57 |
|
|
|
4 |
A |
2997 |
2967 |
15.73 |
|
|
|
5 |
A |
1738 |
1720 |
353.17 |
|
|
|
6 |
A |
1607 |
1591 |
84.97 |
|
|
|
7 |
A |
1352 |
1338 |
2.79 |
|
|
|
8 |
A |
1275 |
1262 |
13.53 |
|
|
|
9 |
A |
1104 |
1092 |
230.38 |
|
|
|
10 |
A |
1019 |
1009 |
4.57 |
|
|
|
11 |
A |
686 |
679 |
128.85 |
|
|
|
12 |
A |
618 |
612 |
41.31 |
|
|
|
13 |
A |
524 |
519 |
115.51 |
|
|
|
14 |
A |
345 |
342 |
133.51 |
|
|
|
15 |
A |
165 |
164 |
9.22 |
|
|
|
16 |
A |
76 |
75 |
107.13 |
|
|
|
17 |
A |
71 |
70 |
5.48 |
|
|
|
18 |
A |
51 |
50 |
16.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12312.8 cm
-1
Scaled (by 0.99) Zero Point Vibrational Energy (zpe) 12189.6 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 PBEPBEultrafine/6-311+G(3df,2pd)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
H |
0.239 |
|
|
|
2 |
O |
-0.401 |
|
|
|
3 |
O |
-0.591 |
|
|
|
4 |
H |
0.148 |
|
|
|
5 |
C |
0.708 |
|
|
|
6 |
O |
-0.381 |
|
|
|
7 |
H |
0.084 |
|
|
|
8 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.836 |
0.758 |
0.750 |
2.123 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.000 |
0.000 |
0.000 |
y |
0.000 |
0.000 |
0.000 |
z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
<r2> |
0.000 |
(<r2>)1/2 |
0.000 |