Vibrational Frequencies calculated at B1B95/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' |
3476 |
3476 |
0.89 |
|
|
|
| 2 |
A' |
3140 |
3140 |
29.42 |
|
|
|
| 3 |
A' |
3043 |
3043 |
48.26 |
|
|
|
| 4 |
A' |
1735 |
1735 |
24.48 |
|
|
|
| 5 |
A' |
1492 |
1492 |
6.97 |
|
|
|
| 6 |
A' |
1367 |
1367 |
40.45 |
|
|
|
| 7 |
A' |
1070 |
1070 |
36.14 |
|
|
|
| 8 |
A" |
1171 |
1171 |
43.29 |
|
|
|
| 9 |
A" |
1106 |
1106 |
17.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8798.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8798.9 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 B1B95/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-1.106 |
|
|
|
| 2 |
N |
-0.964 |
|
|
|
| 3 |
H |
0.818 |
|
|
|
| 4 |
H |
0.898 |
|
|
|
| 5 |
H |
0.354 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.356 |
1.465 |
0.000 |
1.996 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.717 |
2.047 |
0.000 |
| y |
2.047 |
-12.732 |
0.000 |
| z |
0.000 |
0.000 |
-13.647 |
|
| Traceless |
| | x | y | z |
| x |
1.472 |
2.047 |
0.000 |
| y |
2.047 |
-0.050 |
0.000 |
| z |
0.000 |
0.000 |
-1.422 |
|
| Polar |
| 3z2-r2 | -2.844 |
| x2-y2 | 1.015 |
| xy | 2.047 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.260 |
0.110 |
0.000 |
| y |
0.110 |
4.303 |
0.000 |
| z |
0.000 |
0.000 |
2.526 |
<r2> (average value of r
2) Å
2
| <r2> |
19.500 |
| (<r2>)1/2 |
4.416 |