Vibrational Frequencies calculated at HSEh1PBE/6-311G**
| 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' |
3471 |
3333 |
0.74 |
|
|
|
| 2 |
A' |
3127 |
3003 |
39.19 |
|
|
|
| 3 |
A' |
3027 |
2907 |
51.08 |
|
|
|
| 4 |
A' |
1740 |
1671 |
23.60 |
|
|
|
| 5 |
A' |
1499 |
1440 |
5.92 |
|
|
|
| 6 |
A' |
1379 |
1324 |
42.79 |
|
|
|
| 7 |
A' |
1079 |
1036 |
35.29 |
|
|
|
| 8 |
A" |
1181 |
1134 |
49.80 |
|
|
|
| 9 |
A" |
1105 |
1061 |
16.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8803.9 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 8455.2 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 HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.090 |
|
|
|
| 2 |
N |
-0.310 |
|
|
|
| 3 |
H |
0.100 |
|
|
|
| 4 |
H |
0.124 |
|
|
|
| 5 |
H |
0.176 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.408 |
1.396 |
0.000 |
1.983 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.499 |
1.992 |
0.000 |
| y |
1.992 |
-12.600 |
0.000 |
| z |
0.000 |
0.000 |
-13.422 |
|
| Traceless |
| | x | y | z |
| x |
1.512 |
1.992 |
0.000 |
| y |
1.992 |
-0.140 |
0.000 |
| z |
0.000 |
0.000 |
-1.372 |
|
| Polar |
| 3z2-r2 | -2.745 |
| x2-y2 | 1.101 |
| xy | 1.992 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.656 |
0.219 |
0.000 |
| y |
0.219 |
3.813 |
0.000 |
| z |
0.000 |
0.000 |
1.527 |
<r2> (average value of r
2) Å
2
| <r2> |
19.456 |
| (<r2>)1/2 |
4.411 |