Jump to
S1C2
S2C1
S2C2
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -131.470192 |
| Energy at 298.15K | -131.469410 |
| HF Energy | -131.470192 |
| Nuclear repulsion energy | 47.582324 |
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/cc-pVTZ
| 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' |
3394 |
3280 |
47.30 |
|
|
|
| 2 |
A' |
1762 |
1703 |
33.89 |
|
|
|
| 3 |
A' |
1251 |
1209 |
5.62 |
|
|
|
| 4 |
A' |
449 |
434 |
4.87 |
|
|
|
| 5 |
A' |
313 |
303 |
44.49 |
|
|
|
| 6 |
A" |
445 |
430 |
0.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3806.9 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 3679.7 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 B3LYP/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.103 |
-1.206 |
0.000 |
| C2 |
0.000 |
0.084 |
0.000 |
| N3 |
-0.172 |
1.270 |
0.000 |
| H4 |
0.584 |
-2.157 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2942 | 2.4919 | 1.0656 |
C2 | 1.2942 | | 1.1989 | 2.3159 | N3 | 2.4919 | 1.1989 | | 3.5100 | H4 | 1.0656 | 2.3159 | 3.5100 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.334 |
|
C2 |
C1 |
H4 |
157.769 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -131.469977 |
| Energy at 298.15K | |
| HF Energy | -131.469977 |
| Nuclear repulsion energy | 47.620884 |
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/cc-pVTZ
| 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 |
3434 |
3320 |
69.04 |
|
|
|
| 2 |
Σ |
1726 |
1668 |
34.68 |
|
|
|
| 3 |
Σ |
1276 |
1234 |
3.86 |
|
|
|
| 4 |
Π |
444 |
429 |
0.22 |
|
|
|
| 4 |
Π |
444 |
429 |
0.22 |
|
|
|
| 5 |
Π |
222i |
214i |
47.81 |
|
|
|
| 5 |
Π |
222i |
214i |
47.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3440.4 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 3325.5 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/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.202 |
| C2 |
0.000 |
0.000 |
0.080 |
| N3 |
0.000 |
0.000 |
1.285 |
| H4 |
0.000 |
0.000 |
-2.265 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2826 | 2.4875 | 1.0623 |
C2 | 1.2826 | | 1.2048 | 2.3450 | N3 | 2.4875 | 1.2048 | | 3.5498 | H4 | 1.0623 | 2.3450 | 3.5498 | |
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 B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.141 |
|
|
|
| 2 |
C |
0.037 |
|
|
|
| 3 |
N |
-0.065 |
|
|
|
| 4 |
H |
0.169 |
|
|
|
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 |
-3.228 |
3.228 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.337 |
0.000 |
0.000 |
| y |
0.000 |
-17.337 |
0.000 |
| z |
0.000 |
0.000 |
-15.658 |
|
| Traceless |
| | x | y | z |
| x |
-0.839 |
0.000 |
0.000 |
| y |
0.000 |
-0.839 |
0.000 |
| z |
0.000 |
0.000 |
1.678 |
|
| Polar |
| 3z2-r2 | 3.357 |
| 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 |
2.419 |
0.000 |
0.000 |
| y |
0.000 |
2.419 |
0.000 |
| z |
0.000 |
0.000 |
6.664 |
<r2> (average value of r
2) Å
2
| <r2> |
35.881 |
| (<r2>)1/2 |
5.990 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -131.445640 |
| Energy at 298.15K | -131.445098 |
| HF Energy | -131.445640 |
| Nuclear repulsion energy | 47.228807 |
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/cc-pVTZ
| 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' |
3072 |
2969 |
4.63 |
|
|
|
| 2 |
A' |
2090 |
2021 |
21.70 |
|
|
|
| 3 |
A' |
1093 |
1056 |
39.41 |
|
|
|
| 4 |
A' |
942 |
911 |
45.28 |
|
|
|
| 5 |
A' |
461 |
446 |
23.66 |
|
|
|
| 6 |
A" |
315 |
305 |
11.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3986.7 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 3853.5 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.060 |
-1.275 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.208 |
1.248 |
0.000 |
| H4 |
1.093 |
-1.640 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3681 | 2.5368 | 1.0956 |
C2 | 1.3681 | | 1.1743 | 2.0481 | N3 | 2.5368 | 1.1743 | | 3.1673 | H4 | 1.0956 | 2.0481 | 3.1673 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.144 |
|
|
|
| 2 |
C |
-0.005 |
|
|
|
| 3 |
N |
-0.008 |
|
|
|
| 4 |
H |
0.157 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.700 |
-1.432 |
0.000 |
2.222 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.151 |
-2.431 |
0.000 |
| y |
-2.431 |
-21.015 |
0.000 |
| z |
0.000 |
0.000 |
-15.977 |
|
| Traceless |
| | x | y | z |
| x |
1.345 |
-2.431 |
0.000 |
| y |
-2.431 |
-4.451 |
0.000 |
| z |
0.000 |
0.000 |
3.106 |
|
| Polar |
| 3z2-r2 | 6.212 |
| x2-y2 | 3.864 |
| xy | -2.431 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.992 |
-0.570 |
0.000 |
| y |
-0.570 |
6.601 |
0.000 |
| z |
0.000 |
0.000 |
2.782 |
<r2> (average value of r
2) Å
2
| <r2> |
36.182 |
| (<r2>)1/2 |
6.015 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -131.445640 |
| Energy at 298.15K | -131.445098 |
| HF Energy | -131.445640 |
| Nuclear repulsion energy | 47.228807 |
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/cc-pVTZ
Geometric Data calculated at B3LYP/cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability