Vibrational Frequencies calculated at B2PLYP=FULLultrafine/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' |
3286 |
3286 |
0.37 |
122.82 |
0.32 |
0.48 |
| 2 |
A' |
3137 |
3137 |
22.12 |
90.51 |
0.73 |
0.84 |
| 3 |
A' |
3055 |
3055 |
71.41 |
204.03 |
0.09 |
0.17 |
| 4 |
A' |
3053 |
3053 |
40.67 |
126.47 |
0.04 |
0.08 |
| 5 |
A' |
1854 |
1854 |
12.12 |
44.72 |
0.20 |
0.34 |
| 6 |
A' |
1550 |
1550 |
6.47 |
13.93 |
0.36 |
0.52 |
| 7 |
A' |
1517 |
1517 |
10.12 |
17.39 |
0.65 |
0.78 |
| 8 |
A' |
1435 |
1435 |
0.19 |
9.02 |
0.68 |
0.81 |
| 9 |
A' |
1207 |
1207 |
2.33 |
5.53 |
0.42 |
0.60 |
| 10 |
A' |
1095 |
1095 |
4.68 |
2.93 |
0.21 |
0.34 |
| 11 |
A' |
1070 |
1070 |
40.71 |
0.30 |
0.21 |
0.35 |
| 12 |
A' |
987 |
987 |
4.55 |
8.83 |
0.40 |
0.58 |
| 13 |
A' |
946 |
946 |
16.37 |
6.62 |
0.50 |
0.66 |
| 14 |
A' |
678 |
678 |
0.52 |
14.34 |
0.61 |
0.76 |
| 15 |
A' |
323 |
323 |
1.80 |
1.49 |
0.74 |
0.85 |
| 16 |
A" |
3120 |
3120 |
54.65 |
104.81 |
0.75 |
0.86 |
| 17 |
A" |
3110 |
3110 |
29.31 |
92.13 |
0.75 |
0.86 |
| 18 |
A" |
1510 |
1510 |
9.46 |
12.42 |
0.75 |
0.86 |
| 19 |
A" |
1136 |
1136 |
0.92 |
1.76 |
0.75 |
0.86 |
| 20 |
A" |
1062 |
1062 |
0.41 |
2.99 |
0.75 |
0.86 |
| 21 |
A" |
1002 |
1002 |
2.25 |
7.28 |
0.75 |
0.86 |
| 22 |
A" |
707 |
707 |
33.28 |
0.94 |
0.75 |
0.86 |
| 23 |
A" |
292 |
292 |
13.43 |
0.98 |
0.75 |
0.86 |
| 24 |
A" |
158 |
158 |
0.41 |
0.36 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 18644.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 18644.9 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 B2PLYP=FULLultrafine/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.119 |
|
|
|
| 2 |
C |
-0.421 |
|
|
|
| 3 |
C |
-0.244 |
|
|
|
| 4 |
C |
-0.738 |
|
|
|
| 5 |
H |
0.193 |
|
|
|
| 6 |
H |
0.193 |
|
|
|
| 7 |
H |
0.201 |
|
|
|
| 8 |
H |
0.228 |
|
|
|
| 9 |
H |
0.234 |
|
|
|
| 10 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.113 |
0.846 |
0.000 |
0.854 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.755 |
-0.536 |
0.010 |
| y |
-0.536 |
-25.466 |
0.003 |
| z |
0.010 |
0.003 |
-25.884 |
|
| Traceless |
| | x | y | z |
| x |
1.919 |
-0.536 |
0.010 |
| y |
-0.536 |
-0.646 |
0.003 |
| z |
0.010 |
0.003 |
-1.273 |
|
| Polar |
| 3z2-r2 | -2.546 |
| x2-y2 | 1.710 |
| xy | -0.536 |
| xz | 0.010 |
| yz | 0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.816 |
-0.493 |
-0.003 |
| y |
-0.493 |
7.221 |
-0.002 |
| z |
-0.003 |
-0.002 |
4.552 |
<r2> (average value of r
2) Å
2
| <r2> |
80.599 |
| (<r2>)1/2 |
8.978 |