Jump to
S1C2
S2C1
S2C2
Energy calculated at PBE1PBE/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -131.280081 |
| Energy at 298.15K | -131.279392 |
| HF Energy | -131.280081 |
| Nuclear repulsion energy | 47.196966 |
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/aug-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' |
3396 |
3265 |
37.72 |
|
|
|
| 2 |
A' |
1814 |
1744 |
42.16 |
|
|
|
| 3 |
A' |
1235 |
1188 |
7.72 |
|
|
|
| 4 |
A' |
479 |
460 |
25.94 |
|
|
|
| 5 |
A' |
388 |
373 |
15.40 |
|
|
|
| 6 |
A" |
431 |
414 |
0.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3871.2 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 3722.6 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/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.082 |
-1.224 |
0.000 |
| C2 |
0.000 |
0.088 |
0.000 |
| N3 |
-0.163 |
1.279 |
0.000 |
| H4 |
0.651 |
-2.138 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3146 | 2.5146 | 1.0771 |
C2 | 1.3146 | | 1.2017 | 2.3195 | N3 | 2.5146 | 1.2017 | | 3.5124 | H4 | 1.0771 | 2.3195 | 3.5124 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.763 |
|
C2 |
C1 |
H4 |
151.625 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at PBE1PBE/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -131.279316 |
| Energy at 298.15K | |
| HF Energy | -131.279316 |
| Nuclear repulsion energy | 47.259824 |
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/aug-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 |
3455 |
3322 |
68.92 |
|
|
|
| 2 |
Σ |
1747 |
1680 |
45.03 |
|
|
|
| 3 |
Σ |
1277 |
1228 |
4.59 |
|
|
|
| 4 |
Π |
432 |
416 |
0.04 |
|
|
|
| 4 |
Π |
432 |
416 |
0.04 |
|
|
|
| 5 |
Π |
341i |
328i |
45.45 |
|
|
|
| 5 |
Π |
341i |
328i |
45.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3330.3 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 3202.5 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 PBE1PBE/aug-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 |
1.294 |
| H4 |
0.000 |
0.000 |
-2.285 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2962 | 2.5068 | 1.0719 |
C2 | 1.2962 | | 1.2106 | 2.3681 | N3 | 2.5068 | 1.2106 | | 3.5787 | H4 | 1.0719 | 2.3681 | 3.5787 | |
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/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.651 |
|
|
|
| 2 |
C |
0.100 |
|
|
|
| 3 |
N |
-0.388 |
|
|
|
| 4 |
H |
-0.364 |
|
|
|
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 |
-3.330 |
3.330 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.481 |
0.000 |
0.000 |
| y |
0.000 |
-17.481 |
0.000 |
| z |
0.000 |
0.000 |
-15.588 |
|
| Traceless |
| | x | y | z |
| x |
-0.946 |
0.000 |
0.000 |
| y |
0.000 |
-0.946 |
0.000 |
| z |
0.000 |
0.000 |
1.892 |
|
| Polar |
| 3z2-r2 | 3.784 |
| 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 |
3.033 |
0.000 |
0.000 |
| y |
0.000 |
3.033 |
0.000 |
| z |
0.000 |
0.000 |
7.129 |
<r2> (average value of r
2) Å
2
| <r2> |
36.332 |
| (<r2>)1/2 |
6.028 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at PBE1PBE/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -131.249692 |
| Energy at 298.15K | -131.249120 |
| HF Energy | -131.249692 |
| Nuclear repulsion energy | 46.882816 |
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/aug-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' |
3086 |
2968 |
3.73 |
|
|
|
| 2 |
A' |
2119 |
2037 |
24.72 |
|
|
|
| 3 |
A' |
1095 |
1053 |
37.62 |
|
|
|
| 4 |
A' |
950 |
914 |
44.34 |
|
|
|
| 5 |
A' |
450 |
433 |
23.63 |
|
|
|
| 6 |
A" |
296 |
285 |
10.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3997.8 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 3844.3 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 PBE1PBE/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.070 |
-1.285 |
0.000 |
| C2 |
0.000 |
0.093 |
0.000 |
| N3 |
-0.221 |
1.254 |
0.000 |
| H4 |
1.126 |
-1.621 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3799 | 2.5561 | 1.1077 |
C2 | 1.3799 | | 1.1822 | 2.0501 | N3 | 2.5561 | 1.1822 | | 3.1746 | H4 | 1.1077 | 2.0501 | 3.1746 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.071 |
|
|
|
| 2 |
C |
0.267 |
|
|
|
| 3 |
N |
-0.270 |
|
|
|
| 4 |
H |
-0.069 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.720 |
-1.453 |
0.000 |
2.251 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.200 |
-2.459 |
0.000 |
| y |
-2.459 |
-21.180 |
0.000 |
| z |
0.000 |
0.000 |
-16.131 |
|
| Traceless |
| | x | y | z |
| x |
1.455 |
-2.459 |
0.000 |
| y |
-2.459 |
-4.514 |
0.000 |
| z |
0.000 |
0.000 |
3.059 |
|
| Polar |
| 3z2-r2 | 6.118 |
| x2-y2 | 3.980 |
| xy | -2.459 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.485 |
-0.522 |
0.000 |
| y |
-0.522 |
7.083 |
0.000 |
| z |
0.000 |
0.000 |
3.310 |
<r2> (average value of r
2) Å
2
| <r2> |
36.588 |
| (<r2>)1/2 |
6.049 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at PBE1PBE/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -131.249692 |
| Energy at 298.15K | -131.249120 |
| HF Energy | -131.249692 |
| Nuclear repulsion energy | 46.882816 |
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/aug-cc-pVDZ
Geometric Data calculated at PBE1PBE/aug-cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability