Vibrational Frequencies calculated at B3LYPultrafine/cc-pVTZ
| 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 |
3185 |
3079 |
116.05 |
|
|
|
| 2 |
A1 |
1547 |
1495 |
1.53 |
|
|
|
| 3 |
A1 |
944 |
912 |
73.40 |
|
|
|
| 4 |
E |
3178 |
3072 |
7.69 |
|
|
|
| 4 |
E |
3178 |
3072 |
7.69 |
|
|
|
| 5 |
E |
1650 |
1595 |
9.47 |
|
|
|
| 5 |
E |
1650 |
1595 |
9.47 |
|
|
|
| 6 |
E |
1157 |
1119 |
22.39 |
|
|
|
| 6 |
E |
1157 |
1119 |
22.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8822.8 cm
-1
Scaled (by 0.9667) Zero Point Vibrational Energy (zpe) 8529.0 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 B3LYPultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.190 |
|
|
|
| 2 |
O |
-0.587 |
|
|
|
| 3 |
H |
0.132 |
|
|
|
| 4 |
H |
0.132 |
|
|
|
| 5 |
H |
0.132 |
|
|
|
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 |
-5.124 |
5.124 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.413 |
0.000 |
0.000 |
| y |
0.000 |
-11.413 |
0.000 |
| z |
0.000 |
0.000 |
-12.762 |
|
| Traceless |
| | x | y | z |
| x |
0.674 |
0.000 |
0.000 |
| y |
0.000 |
0.674 |
0.000 |
| z |
0.000 |
0.000 |
-1.349 |
|
| Polar |
| 3z2-r2 | -2.697 |
| x2-y2 | 0.000 |
| 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 |
1.920 |
0.000 |
0.000 |
| y |
0.000 |
1.920 |
0.000 |
| z |
0.000 |
0.000 |
3.276 |
<r2> (average value of r
2) Å
2
| <r2> |
20.174 |
| (<r2>)1/2 |
4.492 |