Vibrational Frequencies calculated at B3LYPultrafine/cc-pVDZ
| 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' |
3384 |
3282 |
3.98 |
|
|
|
| 2 |
A' |
3105 |
3012 |
41.68 |
|
|
|
| 3 |
A' |
3003 |
2913 |
49.63 |
|
|
|
| 4 |
A' |
1718 |
1666 |
24.14 |
|
|
|
| 5 |
A' |
1475 |
1430 |
4.01 |
|
|
|
| 6 |
A' |
1369 |
1328 |
45.56 |
|
|
|
| 7 |
A' |
1067 |
1035 |
31.14 |
|
|
|
| 8 |
A" |
1166 |
1131 |
41.23 |
|
|
|
| 9 |
A" |
1081 |
1049 |
13.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8683.3 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 8422.8 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-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.020 |
|
|
|
| 2 |
N |
-0.155 |
|
|
|
| 3 |
H |
0.015 |
|
|
|
| 4 |
H |
0.035 |
|
|
|
| 5 |
H |
0.085 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.293 |
1.225 |
0.000 |
1.781 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.589 |
1.845 |
0.000 |
| y |
1.845 |
-12.555 |
0.000 |
| z |
0.000 |
0.000 |
-13.214 |
|
| Traceless |
| | x | y | z |
| x |
1.295 |
1.845 |
0.000 |
| y |
1.845 |
-0.154 |
0.000 |
| z |
0.000 |
0.000 |
-1.142 |
|
| Polar |
| 3z2-r2 | -2.284 |
| x2-y2 | 0.966 |
| xy | 1.845 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.664 |
0.276 |
0.000 |
| y |
0.276 |
3.727 |
0.000 |
| z |
0.000 |
0.000 |
1.357 |
<r2> (average value of r
2) Å
2
| <r2> |
19.592 |
| (<r2>)1/2 |
4.426 |