Vibrational Frequencies calculated at B3LYP/LANL2DZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1' |
3638 |
3497 |
0.00 |
|
|
|
| 2 |
A1' |
2672 |
2569 |
0.00 |
|
|
|
| 3 |
A1' |
958 |
920 |
0.00 |
|
|
|
| 4 |
A1' |
868 |
834 |
0.00 |
|
|
|
| 5 |
A2' |
1351 |
1299 |
0.00 |
|
|
|
| 6 |
A2' |
1271 |
1221 |
0.00 |
|
|
|
| 7 |
A2' |
1064 |
1023 |
0.00 |
|
|
|
| 8 |
A2" |
1004 |
965 |
273.03 |
|
|
|
| 9 |
A2" |
746 |
717 |
93.57 |
|
|
|
| 10 |
A2" |
464 |
446 |
34.46 |
|
|
|
| 11 |
E' |
3640 |
3499 |
34.90 |
|
|
|
| 11 |
E' |
3640 |
3499 |
34.90 |
|
|
|
| 12 |
E' |
2661 |
2557 |
289.50 |
|
|
|
| 12 |
E' |
2661 |
2557 |
289.50 |
|
|
|
| 13 |
E' |
1489 |
1432 |
522.12 |
|
|
|
| 13 |
E' |
1489 |
1432 |
522.11 |
|
|
|
| 14 |
E' |
1411 |
1356 |
32.45 |
|
|
|
| 14 |
E' |
1411 |
1356 |
32.44 |
|
|
|
| 15 |
E' |
1098 |
1056 |
0.13 |
|
|
|
| 15 |
E' |
1098 |
1056 |
0.13 |
|
|
|
| 16 |
E' |
947 |
911 |
0.36 |
|
|
|
| 16 |
E' |
947 |
911 |
0.36 |
|
|
|
| 17 |
E' |
539 |
518 |
0.60 |
|
|
|
| 17 |
E' |
539 |
518 |
0.60 |
|
|
|
| 18 |
E" |
967 |
929 |
0.00 |
|
|
|
| 18 |
E" |
967 |
929 |
0.00 |
|
|
|
| 19 |
E" |
783 |
753 |
0.00 |
|
|
|
| 19 |
E" |
783 |
753 |
0.00 |
|
|
|
| 20 |
E" |
311 |
299 |
0.00 |
|
|
|
| 20 |
E" |
311 |
299 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20864.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 20054.7 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 B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.424 |
|
|
|
| 2 |
N |
-0.424 |
|
|
|
| 3 |
N |
-0.424 |
|
|
|
| 4 |
B |
0.011 |
|
|
|
| 5 |
B |
0.011 |
|
|
|
| 6 |
B |
0.011 |
|
|
|
| 7 |
H |
0.310 |
|
|
|
| 8 |
H |
0.310 |
|
|
|
| 9 |
H |
0.310 |
|
|
|
| 10 |
H |
0.104 |
|
|
|
| 11 |
H |
0.104 |
|
|
|
| 12 |
H |
0.104 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.400 |
0.000 |
0.000 |
| y |
0.000 |
-33.400 |
0.000 |
| z |
0.000 |
0.000 |
-38.549 |
|
| Traceless |
| | x | y | z |
| x |
2.574 |
0.000 |
0.000 |
| y |
0.000 |
2.574 |
0.000 |
| z |
0.000 |
0.000 |
-5.149 |
|
| Polar |
| 3z2-r2 | -10.297 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.181 |
0.000 |
0.000 |
| y |
0.000 |
9.180 |
0.000 |
| z |
0.000 |
0.000 |
4.584 |
<r2> (average value of r
2) Å
2
| <r2> |
134.886 |
| (<r2>)1/2 |
11.614 |