Jump to
S1C2
S2C1
S2C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -131.393870 |
| Energy at 298.15K | -131.393154 |
| HF Energy | -131.393870 |
| Nuclear repulsion energy | 47.586881 |
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 B1B95/6-311G*
| 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 |
3263 |
33.23 |
|
|
|
| 2 |
A' |
1796 |
1721 |
35.20 |
|
|
|
| 3 |
A' |
1246 |
1194 |
8.10 |
|
|
|
| 4 |
A' |
469 |
449 |
12.52 |
|
|
|
| 5 |
A' |
356 |
341 |
40.81 |
|
|
|
| 6 |
A" |
456 |
438 |
1.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3863.2 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 3703.3 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.070 |
-1.212 |
0.000 |
| C2 |
0.000 |
0.086 |
0.000 |
| N3 |
-0.144 |
1.272 |
0.000 |
| H4 |
0.591 |
-2.144 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3000 | 2.4930 | 1.0678 |
C2 | 1.3000 | | 1.1944 | 2.3072 | N3 | 2.4930 | 1.1944 | | 3.4941 | H4 | 1.0678 | 2.3072 | 3.4941 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.141 |
|
C2 |
C1 |
H4 |
153.869 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -131.393484 |
| Energy at 298.15K | |
| HF Energy | -131.393484 |
| Nuclear repulsion energy | 47.640559 |
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 B1B95/6-311G*
| 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 |
3459 |
3316 |
57.20 |
|
|
|
| 2 |
Σ |
1735 |
1663 |
38.00 |
|
|
|
| 3 |
Σ |
1284 |
1230 |
5.75 |
|
|
|
| 4 |
Π |
457 |
438 |
0.47 |
|
|
|
| 4 |
Π |
457 |
438 |
0.47 |
|
|
|
| 5 |
Π |
239i |
229i |
53.19 |
|
|
|
| 5 |
Π |
239i |
229i |
53.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3456.0 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 3312.9 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 B1B95/6-311G*
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 |
0.082 |
| N3 |
0.000 |
0.000 |
1.284 |
| H4 |
0.000 |
0.000 |
-2.266 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2839 | 2.4864 | 1.0635 |
C2 | 1.2839 | | 1.2025 | 2.3475 | N3 | 2.4864 | 1.2025 | | 3.5500 | H4 | 1.0635 | 2.3475 | 3.5500 | |
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 B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.074 |
|
|
|
| 2 |
C |
0.026 |
|
|
|
| 3 |
N |
-0.242 |
|
|
|
| 4 |
H |
0.291 |
|
|
|
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 |
-3.259 |
3.259 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.176 |
0.000 |
0.000 |
| y |
0.000 |
-17.176 |
0.000 |
| z |
0.000 |
0.000 |
-15.244 |
|
| Traceless |
| | x | y | z |
| x |
-0.966 |
0.000 |
0.000 |
| y |
0.000 |
-0.966 |
0.000 |
| z |
0.000 |
0.000 |
1.932 |
|
| Polar |
| 3z2-r2 | 3.864 |
| 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 |
1.889 |
0.000 |
0.000 |
| y |
0.000 |
1.889 |
0.000 |
| z |
0.000 |
0.000 |
6.331 |
<r2> (average value of r
2) Å
2
| <r2> |
35.716 |
| (<r2>)1/2 |
5.976 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -131.367907 |
| Energy at 298.15K | -131.367366 |
| HF Energy | -131.367907 |
| Nuclear repulsion energy | 47.231754 |
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 B1B95/6-311G*
| 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' |
3089 |
2961 |
10.70 |
|
|
|
| 2 |
A' |
2128 |
2040 |
21.87 |
|
|
|
| 3 |
A' |
1094 |
1049 |
40.90 |
|
|
|
| 4 |
A' |
956 |
916 |
42.42 |
|
|
|
| 5 |
A' |
459 |
440 |
24.67 |
|
|
|
| 6 |
A" |
321 |
308 |
10.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4023.3 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 3856.7 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.069 |
-1.277 |
0.000 |
| C2 |
0.000 |
0.093 |
0.000 |
| N3 |
-0.219 |
1.245 |
0.000 |
| H4 |
1.116 |
-1.610 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3712 | 2.5378 | 1.0983 |
C2 | 1.3712 | | 1.1726 | 2.0359 | N3 | 2.5378 | 1.1726 | | 3.1514 | H4 | 1.0983 | 2.0359 | 3.1514 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.137 |
|
|
|
| 2 |
C |
0.107 |
|
|
|
| 3 |
N |
-0.219 |
|
|
|
| 4 |
H |
0.249 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.790 |
-1.345 |
0.000 |
2.240 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.847 |
-2.474 |
0.000 |
| y |
-2.474 |
-21.004 |
0.000 |
| z |
0.000 |
0.000 |
-15.797 |
|
| Traceless |
| | x | y | z |
| x |
1.553 |
-2.474 |
0.000 |
| y |
-2.474 |
-4.682 |
0.000 |
| z |
0.000 |
0.000 |
3.129 |
|
| Polar |
| 3z2-r2 | 6.257 |
| x2-y2 | 4.157 |
| xy | -2.474 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.578 |
-0.672 |
0.000 |
| y |
-0.672 |
6.262 |
0.000 |
| z |
0.000 |
0.000 |
2.388 |
<r2> (average value of r
2) Å
2
| <r2> |
36.047 |
| (<r2>)1/2 |
6.004 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -131.367907 |
| Energy at 298.15K | -131.367366 |
| HF Energy | -131.367907 |
| Nuclear repulsion energy | 47.231754 |
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 B1B95/6-311G*
Geometric Data calculated at B1B95/6-311G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability