Jump to
S1C2
S2C1
S2C2
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -131.273773 |
| Energy at 298.15K | -131.273069 |
| HF Energy | -131.273773 |
| Nuclear repulsion energy | 47.173897 |
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 PBE1PBE/cc-pVDZ
| 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' |
3404 |
3273 |
44.58 |
|
|
|
| 2 |
A' |
1821 |
1751 |
37.54 |
|
|
|
| 3 |
A' |
1244 |
1197 |
7.95 |
|
|
|
| 4 |
A' |
471 |
452 |
17.44 |
|
|
|
| 5 |
A' |
370 |
356 |
28.02 |
|
|
|
| 6 |
A" |
446 |
429 |
0.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3877.9 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 3728.6 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 PBE1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.079 |
-1.224 |
0.000 |
| C2 |
0.000 |
0.088 |
0.000 |
| N3 |
-0.159 |
1.280 |
0.000 |
| H4 |
0.637 |
-2.147 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3141 | 2.5152 | 1.0791 |
C2 | 1.3141 | | 1.2027 | 2.3242 | N3 | 2.5152 | 1.2027 | | 3.5185 | H4 | 1.0791 | 2.3242 | 3.5185 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.862 |
|
C2 |
C1 |
H4 |
152.277 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -131.273244 |
| Energy at 298.15K | |
| HF Energy | -131.273244 |
| Nuclear repulsion energy | 47.230629 |
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 PBE1PBE/cc-pVDZ
| 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 |
3467 |
3334 |
76.15 |
|
|
|
| 2 |
Σ |
1756 |
1688 |
41.26 |
|
|
|
| 3 |
Σ |
1284 |
1234 |
5.50 |
|
|
|
| 4 |
Π |
445 |
428 |
0.21 |
|
|
|
| 4 |
Π |
445 |
428 |
0.21 |
|
|
|
| 5 |
Π |
261i |
251i |
43.24 |
|
|
|
| 5 |
Π |
261i |
251i |
43.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3437.3 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 3305.0 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 PBE1PBE/cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.213 |
| C2 |
0.000 |
0.000 |
0.084 |
| N3 |
0.000 |
0.000 |
1.295 |
| H4 |
0.000 |
0.000 |
-2.287 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2969 | 2.5082 | 1.0734 |
C2 | 1.2969 | | 1.2113 | 2.3703 | N3 | 2.5082 | 1.2113 | | 3.5816 | H4 | 1.0734 | 2.3703 | 3.5816 | |
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 PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.027 |
|
|
|
| 2 |
C |
0.033 |
|
|
|
| 3 |
N |
-0.137 |
|
|
|
| 4 |
H |
0.077 |
|
|
|
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 |
-3.136 |
3.136 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.113 |
0.000 |
0.000 |
| y |
0.000 |
-17.113 |
0.000 |
| z |
0.000 |
0.000 |
-15.054 |
|
| Traceless |
| | x | y | z |
| x |
-1.029 |
0.000 |
0.000 |
| y |
0.000 |
-1.029 |
0.000 |
| z |
0.000 |
0.000 |
2.059 |
|
| Polar |
| 3z2-r2 | 4.118 |
| 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 |
1.825 |
0.000 |
0.000 |
| y |
0.000 |
1.825 |
0.000 |
| z |
0.000 |
0.000 |
6.213 |
<r2> (average value of r
2) Å
2
| <r2> |
36.100 |
| (<r2>)1/2 |
6.008 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -131.242451 |
| Energy at 298.15K | -131.241903 |
| HF Energy | -131.242451 |
| Nuclear repulsion energy | 46.870456 |
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 PBE1PBE/cc-pVDZ
| 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' |
3087 |
2968 |
7.01 |
|
|
|
| 2 |
A' |
2132 |
2050 |
22.17 |
|
|
|
| 3 |
A' |
1101 |
1058 |
33.43 |
|
|
|
| 4 |
A' |
949 |
912 |
43.81 |
|
|
|
| 5 |
A' |
454 |
437 |
22.96 |
|
|
|
| 6 |
A" |
315 |
303 |
9.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4018.9 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 3864.1 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 PBE1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.063 |
-1.286 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.215 |
1.255 |
0.000 |
| H4 |
1.122 |
-1.620 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3797 | 2.5566 | 1.1103 |
C2 | 1.3797 | | 1.1828 | 2.0470 | N3 | 2.5566 | 1.1828 | | 3.1708 | H4 | 1.1103 | 2.0470 | 3.1708 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.021 |
|
|
|
| 2 |
C |
0.005 |
|
|
|
| 3 |
N |
-0.108 |
|
|
|
| 4 |
H |
0.124 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.716 |
-1.294 |
0.000 |
2.149 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.828 |
-2.432 |
0.000 |
| y |
-2.432 |
-20.646 |
0.000 |
| z |
0.000 |
0.000 |
-15.747 |
|
| Traceless |
| | x | y | z |
| x |
1.369 |
-2.432 |
0.000 |
| y |
-2.432 |
-4.358 |
0.000 |
| z |
0.000 |
0.000 |
2.990 |
|
| Polar |
| 3z2-r2 | 5.979 |
| x2-y2 | 3.818 |
| xy | -2.432 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.559 |
-0.676 |
0.000 |
| y |
-0.676 |
6.148 |
0.000 |
| z |
0.000 |
0.000 |
2.315 |
<r2> (average value of r
2) Å
2
| <r2> |
36.316 |
| (<r2>)1/2 |
6.026 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -131.242451 |
| Energy at 298.15K | -131.241903 |
| HF Energy | -131.242451 |
| Nuclear repulsion energy | 46.870456 |
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 PBE1PBE/cc-pVDZ
Geometric Data calculated at PBE1PBE/cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability