Vibrational Frequencies calculated at PBEPBEultrafine/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' |
3290 |
3271 |
6.68 |
|
|
|
| 2 |
A' |
3032 |
3014 |
41.50 |
|
|
|
| 3 |
A' |
2923 |
2906 |
57.71 |
|
|
|
| 4 |
A' |
1667 |
1657 |
21.36 |
|
|
|
| 5 |
A' |
1429 |
1420 |
1.90 |
|
|
|
| 6 |
A' |
1326 |
1319 |
42.65 |
|
|
|
| 7 |
A' |
1031 |
1025 |
30.19 |
|
|
|
| 8 |
A" |
1135 |
1128 |
39.33 |
|
|
|
| 9 |
A" |
1038 |
1032 |
13.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8435.1 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 8386.2 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.007 |
|
|
|
| 2 |
N |
-0.150 |
|
|
|
| 3 |
H |
0.024 |
|
|
|
| 4 |
H |
0.046 |
|
|
|
| 5 |
H |
0.088 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.250 |
1.163 |
0.000 |
1.708 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.597 |
1.813 |
0.000 |
| y |
1.813 |
-12.602 |
0.000 |
| z |
0.000 |
0.000 |
-13.241 |
|
| Traceless |
| | x | y | z |
| x |
1.324 |
1.813 |
0.000 |
| y |
1.813 |
-0.183 |
0.000 |
| z |
0.000 |
0.000 |
-1.141 |
|
| Polar |
| 3z2-r2 | -2.283 |
| x2-y2 | 1.004 |
| xy | 1.813 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.771 |
0.264 |
0.000 |
| y |
0.264 |
3.799 |
0.000 |
| z |
0.000 |
0.000 |
1.380 |
<r2> (average value of r
2) Å
2
| <r2> |
19.773 |
| (<r2>)1/2 |
4.447 |