Vibrational Frequencies calculated at LSDA/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' |
3379 |
3319 |
4.95 |
|
|
|
| 2 |
A' |
3177 |
3120 |
5.67 |
|
|
|
| 3 |
A' |
1629 |
1599 |
12.44 |
|
|
|
| 4 |
A' |
1341 |
1317 |
23.99 |
|
|
|
| 5 |
A' |
1075 |
1055 |
126.16 |
|
|
|
| 6 |
A' |
875 |
859 |
23.76 |
|
|
|
| 7 |
A" |
3293 |
3234 |
9.15 |
|
|
|
| 8 |
A" |
1230 |
1208 |
0.28 |
|
|
|
| 9 |
A" |
401 |
394 |
219.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8199.7 cm
-1
Scaled (by 0.982) Zero Point Vibrational Energy (zpe) 8052.1 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 LSDA/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.497 |
|
|
|
| 2 |
O |
-0.458 |
|
|
|
| 3 |
H |
0.364 |
|
|
|
| 4 |
H |
0.296 |
|
|
|
| 5 |
H |
0.296 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.233 |
0.581 |
0.000 |
0.626 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.493 |
-4.097 |
0.000 |
| y |
-4.097 |
-12.309 |
0.000 |
| z |
0.000 |
0.000 |
-11.108 |
|
| Traceless |
| | x | y | z |
| x |
1.215 |
-4.097 |
0.000 |
| y |
-4.097 |
-1.508 |
0.000 |
| z |
0.000 |
0.000 |
0.293 |
|
| Polar |
| 3z2-r2 | 0.585 |
| x2-y2 | 1.816 |
| xy | -4.097 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.505 |
-0.587 |
0.000 |
| y |
-0.587 |
2.002 |
0.000 |
| z |
0.000 |
0.000 |
1.368 |
<r2> (average value of r
2) Å
2
| <r2> |
21.227 |
| (<r2>)1/2 |
4.607 |