Vibrational Frequencies calculated at BLYP/aug-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' |
3297 |
3291 |
3.94 |
|
|
|
| 2 |
A' |
3036 |
3030 |
32.05 |
|
|
|
| 3 |
A' |
2928 |
2922 |
60.21 |
|
|
|
| 4 |
A' |
1635 |
1631 |
19.05 |
|
|
|
| 5 |
A' |
1439 |
1436 |
4.99 |
|
|
|
| 6 |
A' |
1327 |
1324 |
38.97 |
|
|
|
| 7 |
A' |
1042 |
1040 |
31.35 |
|
|
|
| 8 |
A" |
1124 |
1122 |
43.93 |
|
|
|
| 9 |
A" |
1057 |
1055 |
15.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8442.0 cm
-1
Scaled (by 0.9981) Zero Point Vibrational Energy (zpe) 8426.0 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 BLYP/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.873 |
|
|
|
| 2 |
N |
-0.088 |
|
|
|
| 3 |
H |
-0.314 |
|
|
|
| 4 |
H |
-0.402 |
|
|
|
| 5 |
H |
-0.068 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.322 |
1.458 |
0.000 |
1.968 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.123 |
2.064 |
0.000 |
| y |
2.064 |
-13.219 |
0.000 |
| z |
0.000 |
0.000 |
-13.907 |
|
| Traceless |
| | x | y | z |
| x |
1.440 |
2.064 |
0.000 |
| y |
2.064 |
-0.204 |
0.000 |
| z |
0.000 |
0.000 |
-1.236 |
|
| Polar |
| 3z2-r2 | -2.472 |
| x2-y2 | 1.096 |
| xy | 2.064 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.490 |
0.095 |
-0.000 |
| y |
0.095 |
4.626 |
0.001 |
| z |
-0.000 |
0.001 |
2.617 |
<r2> (average value of r
2) Å
2
| <r2> |
20.163 |
| (<r2>)1/2 |
4.490 |