Jump to
S1C2
S2C1
S2C2
Energy calculated at B2PLYP/TZVP
| | hartrees |
| Energy at 0K | -131.336851 |
| Energy at 298.15K | -131.336233 |
| HF Energy | -131.212352 |
| Nuclear repulsion energy | 47.509917 |
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 B2PLYP/TZVP
| 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' |
3383 |
3229 |
32.43 |
|
|
|
| 2 |
A' |
1882 |
1796 |
17.76 |
|
|
|
| 3 |
A' |
1187 |
1133 |
13.27 |
|
|
|
| 4 |
A' |
556 |
531 |
31.76 |
|
|
|
| 5 |
A' |
396 |
378 |
11.09 |
|
|
|
| 6 |
A" |
446 |
426 |
1.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3925.2 cm
-1
Scaled (by 0.9544) Zero Point Vibrational Energy (zpe) 3746.2 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 B2PLYP/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.029 |
-1.225 |
0.000 |
| C2 |
0.000 |
0.093 |
0.000 |
| N3 |
-0.114 |
1.273 |
0.000 |
| H4 |
0.624 |
-2.113 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3183 | 2.5019 | 1.0688 |
C2 | 1.3183 | | 1.1853 | 2.2924 | N3 | 2.5019 | 1.1853 | | 3.4652 | H4 | 1.0688 | 2.2924 | 3.4652 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.738 |
|
C2 |
C1 |
H4 |
147.439 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B2PLYP/TZVP
| | hartrees |
| Energy at 0K | -131.335606 |
| Energy at 298.15K | |
| HF Energy | -131.211809 |
| Nuclear repulsion energy | 47.623625 |
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 B2PLYP/TZVP
| 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 |
3465 |
3307 |
75.31 |
|
|
|
| 2 |
Σ |
1721 |
1642 |
26.25 |
|
|
|
| 3 |
Σ |
1266 |
1208 |
9.73 |
|
|
|
| 4 |
Π |
439 |
419 |
0.04 |
|
|
|
| 4 |
Π |
439 |
419 |
0.04 |
|
|
|
| 5 |
Π |
396i |
378i |
59.24 |
|
|
|
| 5 |
Π |
396i |
378i |
59.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3269.2 cm
-1
Scaled (by 0.9544) Zero Point Vibrational Energy (zpe) 3120.1 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 B2PLYP/TZVP
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 |
0.085 |
| N3 |
0.000 |
0.000 |
1.284 |
| H4 |
0.000 |
0.000 |
-2.267 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2903 | 2.4887 | 1.0622 |
C2 | 1.2903 | | 1.1983 | 2.3526 | N3 | 2.4887 | 1.1983 | | 3.5509 | H4 | 1.0622 | 2.3526 | 3.5509 | |
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 B2PLYP/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.179 |
|
|
|
| 2 |
C |
0.019 |
|
|
|
| 3 |
N |
-0.069 |
|
|
|
| 4 |
H |
0.228 |
|
|
|
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 |
-3.390 |
3.390 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.468 |
0.000 |
0.000 |
| y |
0.000 |
-17.468 |
0.000 |
| z |
0.000 |
0.000 |
-16.018 |
|
| Traceless |
| | x | y | z |
| x |
-0.725 |
0.000 |
0.000 |
| y |
0.000 |
-0.725 |
0.000 |
| z |
0.000 |
0.000 |
1.450 |
|
| Polar |
| 3z2-r2 | 2.900 |
| 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 |
2.099 |
0.000 |
0.000 |
| y |
0.000 |
2.099 |
0.000 |
| z |
0.000 |
0.000 |
6.733 |
<r2> (average value of r
2) Å
2
| <r2> |
36.039 |
| (<r2>)1/2 |
6.003 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B2PLYP/TZVP
| | hartrees |
| Energy at 0K | -131.315692 |
| Energy at 298.15K | -131.315131 |
| HF Energy | -131.175656 |
| Nuclear repulsion energy | 47.032721 |
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 B2PLYP/TZVP
| 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' |
3096 |
2955 |
7.55 |
|
|
|
| 2 |
A' |
2088 |
1992 |
22.82 |
|
|
|
| 3 |
A' |
1077 |
1028 |
41.72 |
|
|
|
| 4 |
A' |
948 |
905 |
38.16 |
|
|
|
| 5 |
A' |
433 |
413 |
22.26 |
|
|
|
| 6 |
A" |
322 |
308 |
9.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3981.8 cm
-1
Scaled (by 0.9544) Zero Point Vibrational Energy (zpe) 3800.3 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 B2PLYP/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.150 |
-1.274 |
0.000 |
| C2 |
0.000 |
0.093 |
0.000 |
| N3 |
-0.302 |
1.234 |
0.000 |
| H4 |
1.211 |
-1.549 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3757 | 2.5483 | 1.0959 |
C2 | 1.3757 | | 1.1797 | 2.0401 | N3 | 2.5483 | 1.1797 | | 3.1668 | H4 | 1.0959 | 2.0401 | 3.1668 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.130 |
|
|
|
| 2 |
C |
0.061 |
|
|
|
| 3 |
N |
-0.057 |
|
|
|
| 4 |
H |
0.126 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.909 |
-1.260 |
0.000 |
2.287 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.009 |
-2.263 |
0.000 |
| y |
-2.263 |
-22.020 |
0.000 |
| z |
0.000 |
0.000 |
-16.038 |
|
| Traceless |
| | x | y | z |
| x |
2.020 |
-2.263 |
0.000 |
| y |
-2.263 |
-5.496 |
0.000 |
| z |
0.000 |
0.000 |
3.477 |
|
| Polar |
| 3z2-r2 | 6.953 |
| x2-y2 | 5.011 |
| xy | -2.263 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.987 |
-0.859 |
0.000 |
| y |
-0.859 |
6.663 |
0.000 |
| z |
0.000 |
0.000 |
2.671 |
<r2> (average value of r
2) Å
2
| <r2> |
36.550 |
| (<r2>)1/2 |
6.046 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B2PLYP/TZVP
| | hartrees |
| Energy at 0K | -131.315692 |
| Energy at 298.15K | -131.315131 |
| HF Energy | -131.175656 |
| Nuclear repulsion energy | 47.032721 |
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 B2PLYP/TZVP
Geometric Data calculated at B2PLYP/TZVP
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability