Vibrational Frequencies calculated at B97D3/daug-cc-pVTZ
| 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' |
3354 |
3354 |
2.87 |
|
|
|
| 2 |
A' |
3049 |
3049 |
36.84 |
|
|
|
| 3 |
A' |
2948 |
2948 |
65.99 |
|
|
|
| 4 |
A' |
1659 |
1659 |
21.04 |
|
|
|
| 5 |
A' |
1458 |
1458 |
4.95 |
|
|
|
| 6 |
A' |
1342 |
1342 |
40.69 |
|
|
|
| 7 |
A' |
1052 |
1052 |
33.67 |
|
|
|
| 8 |
A" |
1139 |
1139 |
41.02 |
|
|
|
| 9 |
A" |
1066 |
1066 |
16.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8533.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8533.0 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 B97D3/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.334 |
|
|
|
| 2 |
N |
-0.954 |
|
|
|
| 3 |
H |
0.502 |
|
|
|
| 4 |
H |
0.525 |
|
|
|
| 5 |
H |
0.261 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.314 |
1.432 |
0.000 |
1.944 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.853 |
2.036 |
0.000 |
| y |
2.036 |
-12.902 |
0.000 |
| z |
0.000 |
0.000 |
-13.691 |
|
| Traceless |
| | x | y | z |
| x |
1.443 |
2.036 |
0.000 |
| y |
2.036 |
-0.130 |
0.000 |
| z |
0.000 |
0.000 |
-1.313 |
|
| Polar |
| 3z2-r2 | -2.627 |
| x2-y2 | 1.049 |
| xy | 2.036 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.449 |
0.085 |
0.000 |
| y |
0.085 |
4.513 |
0.000 |
| z |
0.000 |
0.000 |
2.639 |
<r2> (average value of r
2) Å
2
| <r2> |
19.768 |
| (<r2>)1/2 |
4.446 |