Jump to
S1C2
S2C1
S2C2
Energy calculated at LSDA/6-31G**
| | hartrees |
| Energy at 0K | -130.644762 |
| Energy at 298.15K | -130.643910 |
| HF Energy | -130.644762 |
| Nuclear repulsion energy | 47.208841 |
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 LSDA/6-31G**
| 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' |
3360 |
3297 |
69.46 |
|
|
|
| 2 |
A' |
1873 |
1838 |
17.88 |
|
|
|
| 3 |
A' |
1273 |
1249 |
3.31 |
|
|
|
| 4 |
A' |
447 |
439 |
5.17 |
|
|
|
| 5 |
A' |
261 |
257 |
55.15 |
|
|
|
| 6 |
A" |
450 |
442 |
2.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3831.9 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 3760.3 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 LSDA/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.029 |
-1.216 |
0.000 |
| C2 |
0.000 |
0.081 |
0.000 |
| N3 |
-0.081 |
1.291 |
0.000 |
| H4 |
0.394 |
-2.231 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2970 | 2.5093 | 1.0787 |
C2 | 1.2970 | | 1.2129 | 2.3450 | N3 | 2.5093 | 1.2129 | | 3.5538 | H4 | 1.0787 | 2.3450 | 3.5538 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
177.445 |
|
C2 |
C1 |
H4 |
161.506 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at LSDA/6-31G**
| | hartrees |
| Energy at 0K | -130.644657 |
| Energy at 298.15K | |
| HF Energy | -130.644657 |
| Nuclear repulsion energy | 47.225923 |
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 LSDA/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3386 |
3323 |
88.18 |
|
|
|
| 2 |
Σ |
1862 |
1827 |
18.27 |
|
|
|
| 3 |
Σ |
1285 |
1261 |
3.24 |
|
|
|
| 4 |
Π |
452 |
443 |
2.21 |
|
|
|
| 4 |
Π |
452 |
443 |
2.21 |
|
|
|
| 5 |
Π |
182i |
179i |
52.35 |
|
|
|
| 5 |
Π |
182i |
179i |
52.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3535.8 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 3469.7 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.
Geometric Data calculated at LSDA/6-31G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.211 |
| C2 |
0.000 |
0.000 |
0.080 |
| N3 |
0.000 |
0.000 |
1.296 |
| H4 |
0.000 |
0.000 |
-2.287 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2909 | 2.5069 | 1.0764 |
C2 | 1.2909 | | 1.2159 | 2.3674 | N3 | 2.5069 | 1.2159 | | 3.5833 | H4 | 1.0764 | 2.3674 | 3.5833 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
180.000 |
|
C2 |
C1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.052 |
|
|
|
| 2 |
C |
0.269 |
|
|
|
| 3 |
N |
-0.442 |
|
|
|
| 4 |
H |
0.225 |
|
|
|
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 |
-3.261 |
3.261 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.897 |
0.000 |
0.000 |
| y |
0.000 |
-16.897 |
0.000 |
| z |
0.000 |
0.000 |
-15.064 |
|
| Traceless |
| | x | y | z |
| x |
-0.916 |
0.000 |
0.000 |
| y |
0.000 |
-0.916 |
0.000 |
| z |
0.000 |
0.000 |
1.833 |
|
| Polar |
| 3z2-r2 | 3.666 |
| 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 |
1.650 |
0.000 |
0.000 |
| y |
0.000 |
1.650 |
0.000 |
| z |
0.000 |
0.000 |
6.286 |
<r2> (average value of r
2) Å
2
| <r2> |
35.997 |
| (<r2>)1/2 |
6.000 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at LSDA/6-31G**
| | hartrees |
| Energy at 0K | -130.619852 |
| Energy at 298.15K | -130.619265 |
| HF Energy | -130.619852 |
| Nuclear repulsion energy | 46.915250 |
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 LSDA/6-31G**
| 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' |
3031 |
2974 |
3.91 |
|
|
|
| 2 |
A' |
2074 |
2035 |
10.71 |
|
|
|
| 3 |
A' |
1145 |
1124 |
9.96 |
|
|
|
| 4 |
A' |
842 |
826 |
87.29 |
|
|
|
| 5 |
A' |
445 |
437 |
22.23 |
|
|
|
| 6 |
A" |
313 |
307 |
10.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3924.5 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 3851.1 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.
Geometric Data calculated at LSDA/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.247 |
-1.248 |
0.000 |
| C2 |
0.000 |
0.085 |
0.000 |
| N3 |
-0.401 |
1.212 |
0.000 |
| H4 |
1.326 |
-1.506 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3550 | 2.5438 | 1.1090 |
C2 | 1.3550 | | 1.1967 | 2.0706 | N3 | 2.5438 | 1.1967 | | 3.2202 | H4 | 1.1090 | 2.0706 | 3.2202 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.130 |
|
|
|
| 2 |
C |
0.320 |
|
|
|
| 3 |
N |
-0.375 |
|
|
|
| 4 |
H |
0.186 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.898 |
-1.179 |
0.000 |
2.234 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.128 |
-1.790 |
0.000 |
| y |
-1.790 |
-20.796 |
0.000 |
| z |
0.000 |
0.000 |
-15.549 |
|
| Traceless |
| | x | y | z |
| x |
2.044 |
-1.790 |
0.000 |
| y |
-1.790 |
-4.957 |
0.000 |
| z |
0.000 |
0.000 |
2.913 |
|
| Polar |
| 3z2-r2 | 5.826 |
| x2-y2 | 4.668 |
| xy | -1.790 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.683 |
-1.284 |
0.000 |
| y |
-1.284 |
5.980 |
0.000 |
| z |
0.000 |
0.000 |
2.170 |
<r2> (average value of r
2) Å
2
| <r2> |
36.110 |
| (<r2>)1/2 |
6.009 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at LSDA/6-31G**
| | hartrees |
| Energy at 0K | -130.619852 |
| Energy at 298.15K | -130.619265 |
| HF Energy | -130.619852 |
| Nuclear repulsion energy | 46.915250 |
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 LSDA/6-31G**
Geometric Data calculated at LSDA/6-31G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability