Jump to
S1C2
S2C1
S2C2
Energy calculated at LSDA/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -130.649110 |
| Energy at 298.15K | -130.648156 |
| HF Energy | -130.649110 |
| Nuclear repulsion energy | 47.401737 |
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 LSDA/6-31G(2df,p)
| 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' |
3387 |
3333 |
82.03 |
|
|
|
| 2 |
A' |
1857 |
1827 |
22.32 |
|
|
|
| 3 |
A' |
1274 |
1254 |
3.22 |
|
|
|
| 4 |
A' |
450 |
443 |
2.26 |
|
|
|
| 5 |
A' |
183 |
180 |
52.11 |
|
|
|
| 6 |
A" |
452 |
445 |
1.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3801.6 cm
-1
Scaled (by 0.984) Zero Point Vibrational Energy (zpe) 3740.8 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 LSDA/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.035 |
-1.207 |
0.000 |
| C2 |
0.000 |
0.080 |
0.000 |
| N3 |
-0.071 |
1.288 |
0.000 |
| H4 |
0.286 |
-2.252 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2872 | 2.4976 | 1.0748 |
C2 | 1.2872 | | 1.2107 | 2.3493 | N3 | 2.4976 | 1.2107 | | 3.5584 | H4 | 1.0748 | 2.3493 | 3.5584 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
178.201 |
|
C2 |
C1 |
H4 |
168.049 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at LSDA/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -130.649088 |
| Energy at 298.15K | |
| HF Energy | -130.649088 |
| Nuclear repulsion energy | 47.414917 |
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 LSDA/6-31G(2df,p)
| 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 |
3401 |
3347 |
90.13 |
|
|
|
| 2 |
Σ |
1853 |
1824 |
22.34 |
|
|
|
| 3 |
Σ |
1279 |
1259 |
3.07 |
|
|
|
| 4 |
Π |
451 |
444 |
1.26 |
|
|
|
| 4 |
Π |
451 |
444 |
1.26 |
|
|
|
| 5 |
Π |
133i |
131i |
48.62 |
|
|
|
| 5 |
Π |
133i |
131i |
48.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3584.5 cm
-1
Scaled (by 0.984) Zero Point Vibrational Energy (zpe) 3527.1 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 LSDA/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.205 |
| C2 |
0.000 |
0.000 |
0.079 |
| N3 |
0.000 |
0.000 |
1.291 |
| H4 |
0.000 |
0.000 |
-2.279 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2845 | 2.4964 | 1.0738 |
C2 | 1.2845 | | 1.2119 | 2.3582 | N3 | 2.4964 | 1.2119 | | 3.5701 | H4 | 1.0738 | 2.3582 | 3.5701 | |
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 LSDA/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.204 |
|
|
|
| 2 |
C |
0.242 |
|
|
|
| 3 |
N |
-0.301 |
|
|
|
| 4 |
H |
0.264 |
|
|
|
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 |
-3.238 |
3.238 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.876 |
0.000 |
0.000 |
| y |
0.000 |
-16.876 |
0.000 |
| z |
0.000 |
0.000 |
-15.003 |
|
| Traceless |
| | x | y | z |
| x |
-0.937 |
0.000 |
0.000 |
| y |
0.000 |
-0.937 |
0.000 |
| z |
0.000 |
0.000 |
1.873 |
|
| Polar |
| 3z2-r2 | 3.747 |
| 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 |
2.027 |
0.000 |
0.000 |
| y |
0.000 |
2.027 |
0.000 |
| z |
0.000 |
0.000 |
6.309 |
<r2> (average value of r
2) Å
2
| <r2> |
35.767 |
| (<r2>)1/2 |
5.981 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at LSDA/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -130.625196 |
| Energy at 298.15K | -130.624634 |
| HF Energy | -130.625196 |
| Nuclear repulsion energy | 47.072158 |
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 LSDA/6-31G(2df,p)
| 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' |
3038 |
2989 |
2.84 |
|
|
|
| 2 |
A' |
2069 |
2036 |
12.45 |
|
|
|
| 3 |
A' |
1140 |
1121 |
11.53 |
|
|
|
| 4 |
A' |
854 |
841 |
83.05 |
|
|
|
| 5 |
A' |
465 |
457 |
24.04 |
|
|
|
| 6 |
A" |
314 |
309 |
12.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3939.6 cm
-1
Scaled (by 0.984) Zero Point Vibrational Energy (zpe) 3876.6 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 LSDA/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.185 |
-1.255 |
0.000 |
| C2 |
0.000 |
0.084 |
0.000 |
| N3 |
-0.337 |
1.227 |
0.000 |
| H4 |
1.250 |
-1.562 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3512 | 2.5357 | 1.1081 |
C2 | 1.3512 | | 1.1916 | 2.0666 | N3 | 2.5357 | 1.1916 | | 3.2087 | H4 | 1.1081 | 2.0666 | 3.2087 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.279 |
|
|
|
| 2 |
C |
0.312 |
|
|
|
| 3 |
N |
-0.250 |
|
|
|
| 4 |
H |
0.217 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.740 |
-1.234 |
0.000 |
2.133 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.258 |
-1.885 |
0.000 |
| y |
-1.885 |
-20.557 |
0.000 |
| z |
0.000 |
0.000 |
-15.614 |
|
| Traceless |
| | x | y | z |
| x |
1.827 |
-1.885 |
0.000 |
| y |
-1.885 |
-4.621 |
0.000 |
| z |
0.000 |
0.000 |
2.793 |
|
| Polar |
| 3z2-r2 | 5.587 |
| x2-y2 | 4.299 |
| xy | -1.885 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.805 |
-1.043 |
0.000 |
| y |
-1.043 |
6.155 |
0.000 |
| z |
0.000 |
0.000 |
2.435 |
<r2> (average value of r
2) Å
2
| <r2> |
35.939 |
| (<r2>)1/2 |
5.995 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at LSDA/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -130.625196 |
| Energy at 298.15K | -130.624634 |
| HF Energy | -130.625196 |
| Nuclear repulsion energy | 47.072158 |
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 LSDA/6-31G(2df,p)
Geometric Data calculated at LSDA/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability