Jump to
S2C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -152.058696 |
| Energy at 298.15K | |
| HF Energy | -152.058696 |
| Nuclear repulsion energy | 62.167178 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
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 |
Σg |
2088 |
2007 |
0.00 |
87.56 |
0.62 |
0.76 |
| 2 |
Σg |
903 |
868 |
0.00 |
107.91 |
0.46 |
0.63 |
| 3 |
Σu |
1505 |
1447 |
298.92 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
390 |
374 |
0.00 |
15.26 |
0.75 |
0.86 |
| 4 |
Πg |
390 |
374 |
0.00 |
15.26 |
0.75 |
0.86 |
| 5 |
Πu |
187 |
179 |
19.09 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
187 |
179 |
19.09 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2824.0 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 2714.4 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.
Geometric Data calculated at B3LYP/LANL2DZ
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.653 |
| C2 |
0.000 |
0.000 |
-0.653 |
| C3 |
0.000 |
0.000 |
1.994 |
| C4 |
0.000 |
0.000 |
-1.994 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.3057 | 1.3413 | 2.6470 |
C2 | 1.3057 | | 2.6470 | 1.3413 | C3 | 1.3413 | 2.6470 | | 3.9883 | C4 | 2.6470 | 1.3413 | 3.9883 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
180.000 |
|
C2 |
C1 |
C3 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.049 |
|
|
|
| 2 |
C |
-0.049 |
|
|
|
| 3 |
C |
0.049 |
|
|
|
| 4 |
C |
0.049 |
|
|
|
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 |
-21.993 |
0.000 |
0.000 |
| y |
0.000 |
-21.993 |
0.000 |
| z |
0.000 |
0.000 |
-34.128 |
|
| Traceless |
| | x | y | z |
| x |
6.067 |
0.000 |
0.000 |
| y |
0.000 |
6.067 |
0.000 |
| z |
0.000 |
0.000 |
-12.135 |
|
| Polar |
| 3z2-r2 | -24.269 |
| 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 |
3.432 |
0.000 |
0.000 |
| y |
0.000 |
3.432 |
0.000 |
| z |
0.000 |
0.000 |
13.512 |
<r2> (average value of r
2) Å
2
| <r2> |
69.096 |
| (<r2>)1/2 |
8.312 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -152.031835 |
| Energy at 298.15K | |
| HF Energy | -152.031835 |
| Nuclear repulsion energy | 62.090573 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
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 |
Σg |
2095 |
2014 |
0.00 |
87.88 |
0.39 |
0.56 |
| 2 |
Σg |
902 |
867 |
0.00 |
91.77 |
0.35 |
0.51 |
| 3 |
Σu |
1521 |
1462 |
379.17 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
506 |
486 |
0.00 |
6.63 |
0.75 |
0.86 |
| 4 |
Πg |
343 |
330 |
0.00 |
10.59 |
0.75 |
0.86 |
| 5 |
Πu |
224 |
215 |
2.94 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
168 |
162 |
29.43 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2879.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 2767.8 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.
Geometric Data calculated at B3LYP/LANL2DZ
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.655 |
| C2 |
0.000 |
0.000 |
-0.655 |
| C3 |
0.000 |
0.000 |
1.996 |
| C4 |
0.000 |
0.000 |
-1.996 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.3098 | 1.3414 | 2.6512 |
C2 | 1.3098 | | 2.6512 | 1.3414 | C3 | 1.3414 | 2.6512 | | 3.9926 | C4 | 2.6512 | 1.3414 | 3.9926 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.050 |
|
|
|
| 2 |
C |
-0.050 |
|
|
|
| 3 |
C |
0.050 |
|
|
|
| 4 |
C |
0.050 |
|
|
|
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 |
-23.986 |
0.000 |
0.000 |
| y |
0.000 |
-20.150 |
0.000 |
| z |
0.000 |
0.000 |
-33.855 |
|
| Traceless |
| | x | y | z |
| x |
3.016 |
0.000 |
0.000 |
| y |
0.000 |
8.771 |
0.000 |
| z |
0.000 |
0.000 |
-11.787 |
|
| Polar |
| 3z2-r2 | -23.574 |
| x2-y2 | -3.836 |
| 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 |
3.076 |
0.000 |
0.000 |
| y |
0.000 |
3.142 |
0.000 |
| z |
0.000 |
0.000 |
12.941 |
<r2> (average value of r
2) Å
2
| <r2> |
69.207 |
| (<r2>)1/2 |
8.319 |