Jump to
S1C2
S2C1
S2C2
Energy calculated at B3LYPultrafine/6-31G*
| | hartrees |
| Energy at 0K | -131.421176 |
| Energy at 298.15K | -131.420490 |
| HF Energy | -131.421176 |
| Nuclear repulsion energy | 47.232050 |
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 B3LYPultrafine/6-31G*
| 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' |
3405 |
3262 |
35.17 |
|
|
|
| 2 |
A' |
1801 |
1725 |
29.76 |
|
|
|
| 3 |
A' |
1248 |
1195 |
6.05 |
|
|
|
| 4 |
A' |
476 |
456 |
27.57 |
|
|
|
| 5 |
A' |
390 |
374 |
27.13 |
|
|
|
| 6 |
A" |
452 |
433 |
2.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3886.0 cm
-1
Scaled (by 0.958) Zero Point Vibrational Energy (zpe) 3722.7 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 B3LYPultrafine/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.082 |
-1.221 |
0.000 |
| C2 |
0.000 |
0.084 |
0.000 |
| N3 |
-0.162 |
1.280 |
0.000 |
| H4 |
0.640 |
-2.136 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3075 | 2.5123 | 1.0718 |
C2 | 1.3075 | | 1.2064 | 2.3103 | N3 | 2.5123 | 1.2064 | | 3.5082 | H4 | 1.0718 | 2.3103 | 3.5082 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.890 |
|
C2 |
C1 |
H4 |
152.191 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3LYPultrafine/6-31G*
| | hartrees |
| Energy at 0K | -131.420571 |
| Energy at 298.15K | |
| HF Energy | -131.420571 |
| Nuclear repulsion energy | 47.286550 |
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 B3LYPultrafine/6-31G*
| 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 |
3464 |
3318 |
65.91 |
|
|
|
| 2 |
Σ |
1747 |
1674 |
32.21 |
|
|
|
| 3 |
Σ |
1286 |
1232 |
4.01 |
|
|
|
| 4 |
Π |
454 |
435 |
1.00 |
|
|
|
| 4 |
Π |
454 |
435 |
1.00 |
|
|
|
| 5 |
Π |
290i |
278i |
50.72 |
|
|
|
| 5 |
Π |
290i |
278i |
50.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3412.1 cm
-1
Scaled (by 0.958) Zero Point Vibrational Energy (zpe) 3268.8 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 B3LYPultrafine/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.211 |
| C2 |
0.000 |
0.000 |
0.080 |
| N3 |
0.000 |
0.000 |
1.295 |
| H4 |
0.000 |
0.000 |
-2.278 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2903 | 2.5054 | 1.0670 |
C2 | 1.2903 | | 1.2151 | 2.3572 | N3 | 2.5054 | 1.2151 | | 3.5723 | H4 | 1.0670 | 2.3572 | 3.5723 | |
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 B3LYPultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.079 |
|
|
|
| 2 |
C |
0.313 |
|
|
|
| 3 |
N |
-0.471 |
|
|
|
| 4 |
H |
0.238 |
|
|
|
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 |
-3.262 |
3.262 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.869 |
0.000 |
0.000 |
| y |
0.000 |
-16.869 |
0.000 |
| z |
0.000 |
0.000 |
-15.233 |
|
| Traceless |
| | x | y | z |
| x |
-0.818 |
0.000 |
0.000 |
| y |
0.000 |
-0.818 |
0.000 |
| z |
0.000 |
0.000 |
1.635 |
|
| Polar |
| 3z2-r2 | 3.270 |
| 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 |
1.621 |
0.000 |
0.000 |
| y |
0.000 |
1.621 |
0.000 |
| z |
0.000 |
0.000 |
6.152 |
<r2> (average value of r
2) Å
2
| <r2> |
35.949 |
| (<r2>)1/2 |
5.996 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3LYPultrafine/6-31G*
| | hartrees |
| Energy at 0K | -131.395174 |
| Energy at 298.15K | -131.394614 |
| HF Energy | -131.395174 |
| Nuclear repulsion energy | 46.894931 |
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 B3LYPultrafine/6-31G*
| 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' |
3079 |
2950 |
14.07 |
|
|
|
| 2 |
A' |
2105 |
2016 |
17.56 |
|
|
|
| 3 |
A' |
1100 |
1054 |
38.15 |
|
|
|
| 4 |
A' |
939 |
900 |
48.46 |
|
|
|
| 5 |
A' |
443 |
424 |
22.22 |
|
|
|
| 6 |
A" |
326 |
312 |
10.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3995.6 cm
-1
Scaled (by 0.958) Zero Point Vibrational Energy (zpe) 3827.8 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 B3LYPultrafine/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.131 |
-1.278 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.282 |
1.243 |
0.000 |
| H4 |
1.188 |
-1.585 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3761 | 2.5542 | 1.1008 |
C2 | 1.3761 | | 1.1848 | 2.0553 | N3 | 2.5542 | 1.1848 | | 3.1872 | H4 | 1.1008 | 2.0553 | 3.1872 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.122 |
|
|
|
| 2 |
C |
0.331 |
|
|
|
| 3 |
N |
-0.404 |
|
|
|
| 4 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.803 |
-1.323 |
0.000 |
2.236 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.483 |
-2.132 |
0.000 |
| y |
-2.132 |
-20.901 |
0.000 |
| z |
0.000 |
0.000 |
-15.527 |
|
| Traceless |
| | x | y | z |
| x |
1.731 |
-2.132 |
0.000 |
| y |
-2.132 |
-4.896 |
0.000 |
| z |
0.000 |
0.000 |
3.165 |
|
| Polar |
| 3z2-r2 | 6.330 |
| x2-y2 | 4.418 |
| xy | -2.132 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.449 |
-0.948 |
0.000 |
| y |
-0.948 |
6.010 |
0.000 |
| z |
0.000 |
0.000 |
2.170 |
<r2> (average value of r
2) Å
2
| <r2> |
36.259 |
| (<r2>)1/2 |
6.022 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3LYPultrafine/6-31G*
| | hartrees |
| Energy at 0K | -131.395174 |
| Energy at 298.15K | -131.394614 |
| HF Energy | -131.395174 |
| Nuclear repulsion energy | 46.894931 |
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 B3LYPultrafine/6-31G*
Geometric Data calculated at B3LYPultrafine/6-31G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability