Jump to
S1C2
S2C1
S2C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -130.645062 |
| Energy at 298.15K | -130.644281 |
| HF Energy | -130.645062 |
| Nuclear repulsion energy | 46.471328 |
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 HF/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 |
A' |
3533 |
3180 |
17.96 |
|
|
|
| 2 |
A' |
1620 |
1458 |
80.26 |
|
|
|
| 3 |
A' |
1164 |
1048 |
1.33 |
|
|
|
| 4 |
A' |
457 |
411 |
29.11 |
|
|
|
| 5 |
A' |
376 |
338 |
3.06 |
|
|
|
| 6 |
A" |
393 |
354 |
1.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3771.3 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 3393.8 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.360 |
-1.187 |
0.000 |
| C2 |
0.000 |
0.077 |
0.000 |
| N3 |
-0.466 |
1.230 |
0.000 |
| H4 |
1.102 |
-1.948 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3142 | 2.5546 | 1.0629 |
C2 | 1.3142 | | 1.2440 | 2.3052 | N3 | 2.5546 | 1.2440 | | 3.5439 | H4 | 1.0629 | 2.3052 | 3.5439 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
173.897 |
|
C2 |
C1 |
H4 |
151.584 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -130.644385 |
| Energy at 298.15K | |
| HF Energy | -130.644385 |
| Nuclear repulsion energy | 46.546677 |
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 HF/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 |
Σ |
3587 |
3228 |
41.43 |
|
|
|
| 2 |
Σ |
1602 |
1442 |
68.27 |
|
|
|
| 3 |
Σ |
1177 |
1059 |
4.35 |
|
|
|
| 4 |
Π |
394 |
355 |
1.75 |
|
|
|
| 4 |
Π |
394 |
355 |
1.75 |
|
|
|
| 5 |
Π |
301i |
271i |
51.52 |
|
|
|
| 5 |
Π |
301i |
271i |
51.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3275.2 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 2947.3 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 HF/LANL2DZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.227 |
| C2 |
0.000 |
0.000 |
0.066 |
| N3 |
0.000 |
0.000 |
1.321 |
| H4 |
0.000 |
0.000 |
-2.284 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2924 | 2.5478 | 1.0579 |
C2 | 1.2924 | | 1.2555 | 2.3503 | N3 | 2.5478 | 1.2555 | | 3.6057 | H4 | 1.0579 | 2.3503 | 3.6057 | |
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 HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.270 |
|
|
|
| 2 |
C |
0.056 |
|
|
|
| 3 |
N |
-0.073 |
|
|
|
| 4 |
H |
0.287 |
|
|
|
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 |
-3.178 |
3.178 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.651 |
0.000 |
0.000 |
| y |
0.000 |
-17.651 |
0.000 |
| z |
0.000 |
0.000 |
-16.558 |
|
| Traceless |
| | x | y | z |
| x |
-0.547 |
0.000 |
0.000 |
| y |
0.000 |
-0.547 |
0.000 |
| z |
0.000 |
0.000 |
1.093 |
|
| Polar |
| 3z2-r2 | 2.186 |
| 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 |
1.637 |
0.000 |
0.000 |
| y |
0.000 |
1.637 |
0.000 |
| z |
0.000 |
0.000 |
5.496 |
<r2> (average value of r
2) Å
2
| <r2> |
37.288 |
| (<r2>)1/2 |
6.106 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -130.566878 |
| Energy at 298.15K | -130.566450 |
| HF Energy | -130.566878 |
| Nuclear repulsion energy | 46.763213 |
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 HF/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 |
A' |
3250 |
2925 |
17.50 |
|
|
|
| 2 |
A' |
2245 |
2020 |
23.64 |
|
|
|
| 3 |
A' |
1123 |
1011 |
112.84 |
|
|
|
| 4 |
A' |
979 |
881 |
3.88 |
|
|
|
| 5 |
A' |
484 |
436 |
30.19 |
|
|
|
| 6 |
A" |
406 |
365 |
7.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4243.7 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 3818.9 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.152 |
-1.295 |
0.000 |
| C2 |
0.000 |
0.109 |
0.000 |
| N3 |
0.015 |
1.276 |
0.000 |
| H4 |
0.809 |
-1.814 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.4115 | 2.5754 | 1.0925 |
C2 | 1.4115 | | 1.1668 | 2.0863 | N3 | 2.5754 | 1.1668 | | 3.1902 | H4 | 1.0925 | 2.0863 | 3.1902 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.042 |
|
|
|
| 2 |
C |
-0.104 |
|
|
|
| 3 |
N |
-0.020 |
|
|
|
| 4 |
H |
0.166 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.884 |
-2.021 |
0.000 |
2.763 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.595 |
-3.855 |
0.000 |
| y |
-3.855 |
-21.623 |
0.000 |
| z |
0.000 |
0.000 |
-16.197 |
|
| Traceless |
| | x | y | z |
| x |
0.315 |
-3.855 |
0.000 |
| y |
-3.855 |
-4.227 |
0.000 |
| z |
0.000 |
0.000 |
3.912 |
|
| Polar |
| 3z2-r2 | 7.823 |
| x2-y2 | 3.028 |
| xy | -3.855 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.165 |
-0.028 |
0.000 |
| y |
-0.028 |
5.980 |
0.000 |
| z |
0.000 |
0.000 |
2.436 |
<r2> (average value of r
2) Å
2
| <r2> |
37.346 |
| (<r2>)1/2 |
6.111 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -130.566878 |
| Energy at 298.15K | -130.566450 |
| HF Energy | -130.566878 |
| Nuclear repulsion energy | 46.763213 |
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 HF/LANL2DZ
Geometric Data calculated at HF/LANL2DZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability