Vibrational Frequencies calculated at B3LYPultrafine/TZVP
| 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' |
3422 |
3296 |
2.04 |
|
|
|
| 2 |
A' |
3116 |
3002 |
35.74 |
|
|
|
| 3 |
A' |
3014 |
2903 |
50.64 |
|
|
|
| 4 |
A' |
1715 |
1652 |
23.17 |
|
|
|
| 5 |
A' |
1502 |
1447 |
6.62 |
|
|
|
| 6 |
A' |
1372 |
1322 |
37.79 |
|
|
|
| 7 |
A' |
1078 |
1039 |
37.96 |
|
|
|
| 8 |
A" |
1170 |
1127 |
51.36 |
|
|
|
| 9 |
A" |
1113 |
1072 |
14.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8750.4 cm
-1
Scaled (by 0.9634) Zero Point Vibrational Energy (zpe) 8430.1 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 B3LYPultrafine/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.131 |
|
|
|
| 2 |
N |
-0.254 |
|
|
|
| 3 |
H |
0.088 |
|
|
|
| 4 |
H |
0.121 |
|
|
|
| 5 |
H |
0.175 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.488 |
1.469 |
0.000 |
2.091 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.818 |
2.112 |
0.000 |
| y |
2.112 |
-12.940 |
0.000 |
| z |
0.000 |
0.000 |
-13.684 |
|
| Traceless |
| | x | y | z |
| x |
1.493 |
2.112 |
0.000 |
| y |
2.112 |
-0.189 |
0.000 |
| z |
0.000 |
0.000 |
-1.305 |
|
| Polar |
| 3z2-r2 | -2.609 |
| x2-y2 | 1.121 |
| xy | 2.112 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.823 |
0.193 |
0.000 |
| y |
0.193 |
4.138 |
0.000 |
| z |
0.000 |
0.000 |
1.812 |
<r2> (average value of r
2) Å
2
| <r2> |
19.671 |
| (<r2>)1/2 |
4.435 |