Vibrational Frequencies calculated at BLYP/TZVP
| 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 |
3568 |
3559 |
40.50 |
|
|
|
| 2 |
A |
3313 |
3304 |
0.99 |
|
|
|
| 3 |
A |
1542 |
1538 |
31.33 |
|
|
|
| 4 |
A |
1475 |
1471 |
177.25 |
|
|
|
| 5 |
A |
1162 |
1159 |
89.93 |
|
|
|
| 6 |
A |
979 |
977 |
119.40 |
|
|
|
| 7 |
A |
699 |
697 |
2.54 |
|
|
|
| 8 |
A |
597 |
595 |
0.00 |
|
|
|
| 9 |
A |
267 |
267 |
210.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6800.6 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 6783.6 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 BLYP/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.221 |
|
|
|
| 2 |
N |
0.040 |
|
|
|
| 3 |
N |
-0.253 |
|
|
|
| 4 |
H |
0.203 |
|
|
|
| 5 |
H |
0.233 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.617 |
0.739 |
-0.002 |
3.691 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.722 |
0.348 |
-0.004 |
| y |
0.348 |
-17.195 |
0.001 |
| z |
-0.004 |
0.001 |
-17.899 |
|
| Traceless |
| | x | y | z |
| x |
1.824 |
0.348 |
-0.004 |
| y |
0.348 |
-0.384 |
0.001 |
| z |
-0.004 |
0.001 |
-1.440 |
|
| Polar |
| 3z2-r2 | -2.880 |
| x2-y2 | 1.472 |
| xy | 0.348 |
| xz | -0.004 |
| yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.230 |
0.081 |
-0.000 |
| y |
0.081 |
3.212 |
0.000 |
| z |
-0.000 |
0.000 |
1.880 |
<r2> (average value of r
2) Å
2
| <r2> |
37.088 |
| (<r2>)1/2 |
6.090 |