Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -225.054890 |
| Energy at 298.15K | -225.061111 |
| HF Energy | -225.054890 |
| Nuclear repulsion energy | 123.741401 |
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 HSEh1PBE/cc-pVDZ
| 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 |
3701 |
3560 |
33.59 |
|
|
|
| 2 |
A |
3582 |
3446 |
1.69 |
|
|
|
| 3 |
A |
1862 |
1791 |
381.84 |
|
|
|
| 4 |
A |
1606 |
1545 |
0.69 |
|
|
|
| 5 |
A |
1185 |
1140 |
3.78 |
|
|
|
| 6 |
A |
974 |
937 |
7.51 |
|
|
|
| 7 |
A |
615 |
592 |
87.16 |
|
|
|
| 8 |
A |
473 |
455 |
1.10 |
|
|
|
| 9 |
A |
392 |
377 |
71.09 |
|
|
|
| 10 |
B |
3701 |
3560 |
29.72 |
|
|
|
| 11 |
B |
3579 |
3442 |
41.07 |
|
|
|
| 12 |
B |
1618 |
1556 |
211.37 |
|
|
|
| 13 |
B |
1438 |
1383 |
165.19 |
|
|
|
| 14 |
B |
1061 |
1020 |
20.61 |
|
|
|
| 15 |
B |
801 |
770 |
89.08 |
|
|
|
| 16 |
B |
587 |
564 |
123.26 |
|
|
|
| 17 |
B |
550 |
529 |
154.69 |
|
|
|
| 18 |
B |
444 |
427 |
72.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14082.6 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 13546.1 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 HSEh1PBE/cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.144 |
| O2 |
0.000 |
0.000 |
1.359 |
| N3 |
0.000 |
1.159 |
-0.615 |
| N4 |
0.000 |
-1.159 |
-0.615 |
| H5 |
0.245 |
1.972 |
-0.062 |
| H6 |
0.490 |
1.115 |
-1.502 |
| H7 |
-0.245 |
-1.972 |
-0.062 |
| H8 |
-0.490 |
-1.115 |
-1.502 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2151 | 1.3850 | 1.3850 | 1.9982 | 2.0470 | 1.9982 | 2.0470 |
O2 | 1.2151 | | 2.2889 | 2.2889 | 2.4434 | 3.1090 | 2.4434 | 3.1090 | N3 | 1.3850 | 2.2889 | | 2.3172 | 1.0138 | 1.0141 | 3.1889 | 2.4887 | N4 | 1.3850 | 2.2889 | 2.3172 | | 3.1889 | 2.4887 | 1.0138 | 1.0141 | H5 | 1.9982 | 2.4434 | 1.0138 | 3.1889 | | 1.6936 | 3.9752 | 3.4845 | H6 | 2.0470 | 3.1090 | 1.0141 | 2.4887 | 1.6936 | | 3.4845 | 2.4352 | H7 | 1.9982 | 2.4434 | 3.1889 | 1.0138 | 3.9752 | 3.4845 | | 1.6936 | H8 | 2.0470 | 3.1090 | 2.4887 | 1.0141 | 3.4845 | 2.4352 | 1.6936 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
111.886 |
|
C1 |
N3 |
H6 |
116.279 |
| C1 |
N4 |
H7 |
111.886 |
|
C1 |
N4 |
H8 |
116.279 |
| O2 |
C1 |
N3 |
123.226 |
|
O2 |
C1 |
N4 |
123.226 |
| N3 |
C1 |
N4 |
113.547 |
|
H5 |
N3 |
H6 |
113.266 |
| H7 |
N4 |
H8 |
113.266 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.172 |
|
|
|
| 2 |
O |
-0.293 |
|
|
|
| 3 |
N |
-0.165 |
|
|
|
| 4 |
N |
-0.165 |
|
|
|
| 5 |
H |
0.119 |
|
|
|
| 6 |
H |
0.107 |
|
|
|
| 7 |
H |
0.119 |
|
|
|
| 8 |
H |
0.107 |
|
|
|
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 |
-3.503 |
3.503 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.957 |
3.431 |
0.000 |
| y |
3.431 |
-17.734 |
0.000 |
| z |
0.000 |
0.000 |
-24.571 |
|
| Traceless |
| | x | y | z |
| x |
-2.805 |
3.431 |
0.000 |
| y |
3.431 |
6.530 |
0.000 |
| z |
0.000 |
0.000 |
-3.725 |
|
| Polar |
| 3z2-r2 | -7.450 |
| x2-y2 | -6.223 |
| xy | 3.431 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.271 |
0.239 |
0.000 |
| y |
0.239 |
4.698 |
0.000 |
| z |
0.000 |
0.000 |
4.743 |
<r2> (average value of r
2) Å
2
| <r2> |
68.167 |
| (<r2>)1/2 |
8.256 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -225.052863 |
| Energy at 298.15K | -225.058717 |
| HF Energy | -225.052863 |
| Nuclear repulsion energy | 123.769237 |
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 HSEh1PBE/cc-pVDZ
| 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' |
3730 |
3588 |
35.32 |
|
|
|
| 2 |
A' |
3605 |
3468 |
9.67 |
|
|
|
| 3 |
A' |
1851 |
1781 |
400.83 |
|
|
|
| 4 |
A' |
1614 |
1553 |
15.58 |
|
|
|
| 5 |
A' |
1179 |
1134 |
4.16 |
|
|
|
| 6 |
A' |
981 |
944 |
8.20 |
|
|
|
| 7 |
A' |
785 |
755 |
36.94 |
|
|
|
| 8 |
A' |
547 |
526 |
55.36 |
|
|
|
| 9 |
A' |
485 |
466 |
65.67 |
|
|
|
| 10 |
A' |
437 |
420 |
244.04 |
|
|
|
| 11 |
A" |
3728 |
3586 |
35.42 |
|
|
|
| 12 |
A" |
3597 |
3460 |
37.01 |
|
|
|
| 13 |
A" |
1611 |
1550 |
244.41 |
|
|
|
| 14 |
A" |
1440 |
1385 |
150.35 |
|
|
|
| 15 |
A" |
1027 |
988 |
18.46 |
|
|
|
| 16 |
A" |
577 |
555 |
30.20 |
|
|
|
| 17 |
A" |
444 |
427 |
88.09 |
|
|
|
| 18 |
A" |
202 |
195 |
33.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13920.2 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 13389.8 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 HSEh1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.140 |
0.000 |
| O2 |
0.043 |
1.357 |
0.000 |
| N3 |
0.043 |
-0.605 |
1.162 |
| N4 |
0.043 |
-0.605 |
-1.162 |
| H5 |
-0.182 |
-0.064 |
1.987 |
| H6 |
-0.321 |
-1.549 |
1.158 |
| H7 |
-0.182 |
-0.064 |
-1.987 |
| H8 |
-0.321 |
-1.549 |
-1.158 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2168 | 1.3804 | 1.3804 | 2.0066 | 2.0747 | 2.0066 | 2.0747 |
O2 | 1.2168 | | 2.2797 | 2.2797 | 2.4527 | 3.1490 | 2.4527 | 3.1490 | N3 | 1.3804 | 2.2797 | | 2.3233 | 1.0120 | 1.0117 | 3.2026 | 2.5306 | N4 | 1.3804 | 2.2797 | 2.3233 | | 3.2026 | 2.5306 | 1.0120 | 1.0117 | H5 | 2.0066 | 2.4527 | 1.0120 | 3.2026 | | 1.7066 | 3.9738 | 3.4808 | H6 | 2.0747 | 3.1490 | 1.0117 | 2.5306 | 1.7066 | | 3.4808 | 2.3159 | H7 | 2.0066 | 2.4527 | 3.2026 | 1.0120 | 3.9738 | 3.4808 | | 1.7066 | H8 | 2.0747 | 3.1490 | 2.5306 | 1.0117 | 3.4808 | 2.3159 | 1.7066 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.111 |
|
C1 |
N3 |
H6 |
119.499 |
| C1 |
N4 |
H7 |
113.111 |
|
C1 |
N4 |
H8 |
119.499 |
| O2 |
C1 |
N3 |
122.613 |
|
O2 |
C1 |
N4 |
122.613 |
| N3 |
C1 |
N4 |
114.598 |
|
H5 |
N3 |
H6 |
114.982 |
| H7 |
N4 |
H8 |
114.982 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.179 |
|
|
|
| 2 |
O |
-0.302 |
|
|
|
| 3 |
N |
-0.156 |
|
|
|
| 4 |
N |
-0.156 |
|
|
|
| 5 |
H |
0.120 |
|
|
|
| 6 |
H |
0.098 |
|
|
|
| 7 |
H |
0.120 |
|
|
|
| 8 |
H |
0.098 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.786 |
-3.823 |
0.000 |
4.220 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.564 |
1.821 |
0.000 |
| y |
1.821 |
-24.011 |
0.000 |
| z |
0.000 |
0.000 |
-17.144 |
|
| Traceless |
| | x | y | z |
| x |
-3.986 |
1.821 |
0.000 |
| y |
1.821 |
-3.158 |
0.000 |
| z |
0.000 |
0.000 |
7.144 |
|
| Polar |
| 3z2-r2 | 14.288 |
| x2-y2 | -0.552 |
| xy | 1.821 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.169 |
0.189 |
0.000 |
| y |
0.189 |
4.766 |
0.000 |
| z |
0.000 |
0.000 |
4.728 |
<r2> (average value of r
2) Å
2
| <r2> |
68.236 |
| (<r2>)1/2 |
8.261 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -225.051651 |
| Energy at 298.15K | |
| HF Energy | -225.051651 |
| Nuclear repulsion energy | 123.935148 |
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 HSEh1PBE/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3787 |
3643 |
55.04 |
|
|
|
| 2 |
A1 |
3644 |
3506 |
5.77 |
|
|
|
| 3 |
A1 |
1844 |
1774 |
441.71 |
|
|
|
| 4 |
A1 |
1591 |
1531 |
4.57 |
|
|
|
| 5 |
A1 |
1140 |
1096 |
0.29 |
|
|
|
| 6 |
A1 |
991 |
954 |
6.91 |
|
|
|
| 7 |
A1 |
476 |
458 |
3.05 |
|
|
|
| 8 |
A2 |
381 |
366 |
0.00 |
|
|
|
| 9 |
A2 |
432i |
416i |
0.00 |
|
|
|
| 10 |
B1 |
784 |
754 |
7.53 |
|
|
|
| 11 |
B1 |
572 |
551 |
9.58 |
|
|
|
| 12 |
B1 |
341i |
328i |
430.26 |
|
|
|
| 13 |
B2 |
3786 |
3641 |
47.21 |
|
|
|
| 14 |
B2 |
3636 |
3497 |
63.68 |
|
|
|
| 15 |
B2 |
1607 |
1546 |
354.97 |
|
|
|
| 16 |
B2 |
1440 |
1385 |
126.91 |
|
|
|
| 17 |
B2 |
985 |
947 |
9.33 |
|
|
|
| 18 |
B2 |
566 |
544 |
15.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13227.7 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 12723.7 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 HSEh1PBE/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.142 |
| O2 |
0.000 |
0.000 |
1.360 |
| N3 |
0.000 |
1.155 |
-0.597 |
| N4 |
0.000 |
-1.155 |
-0.597 |
| H5 |
0.000 |
2.022 |
-0.083 |
| H6 |
0.000 |
1.181 |
-1.604 |
| H7 |
0.000 |
-2.022 |
-0.083 |
| H8 |
0.000 |
-1.181 |
-1.604 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2187 | 1.3711 | 1.3711 | 2.0344 | 2.1076 | 2.0344 | 2.1076 |
O2 | 1.2187 | | 2.2729 | 2.2729 | 2.4841 | 3.1911 | 2.4841 | 3.1911 | N3 | 1.3711 | 2.2729 | | 2.3101 | 1.0082 | 1.0075 | 3.2185 | 2.5435 | N4 | 1.3711 | 2.2729 | 2.3101 | | 3.2185 | 2.5435 | 1.0082 | 1.0075 | H5 | 2.0344 | 2.4841 | 1.0082 | 3.2185 | | 1.7389 | 4.0441 | 3.5458 | H6 | 2.1076 | 3.1911 | 1.0075 | 2.5435 | 1.7389 | | 3.5458 | 2.3611 | H7 | 2.0344 | 2.4841 | 3.2185 | 1.0082 | 4.0441 | 3.5458 | | 1.7389 | H8 | 2.1076 | 3.1911 | 2.5435 | 1.0075 | 3.5458 | 2.3611 | 1.7389 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.707 |
|
C1 |
N3 |
H6 |
124.053 |
| C1 |
N4 |
H7 |
116.707 |
|
C1 |
N4 |
H8 |
124.053 |
| O2 |
C1 |
N3 |
122.603 |
|
O2 |
C1 |
N4 |
122.603 |
| N3 |
C1 |
N4 |
114.793 |
|
H5 |
N3 |
H6 |
119.240 |
| H7 |
N4 |
H8 |
119.240 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.197 |
|
|
|
| 2 |
O |
-0.313 |
|
|
|
| 3 |
N |
-0.157 |
|
|
|
| 4 |
N |
-0.157 |
|
|
|
| 5 |
H |
0.120 |
|
|
|
| 6 |
H |
0.096 |
|
|
|
| 7 |
H |
0.120 |
|
|
|
| 8 |
H |
0.096 |
|
|
|
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 |
-4.278 |
4.278 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.066 |
0.000 |
0.000 |
| y |
0.000 |
-16.128 |
0.000 |
| z |
0.000 |
0.000 |
-23.325 |
|
| Traceless |
| | x | y | z |
| x |
-5.339 |
0.000 |
0.000 |
| y |
0.000 |
8.067 |
0.000 |
| z |
0.000 |
0.000 |
-2.728 |
|
| Polar |
| 3z2-r2 | -5.456 |
| x2-y2 | -8.938 |
| 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 |
2.031 |
0.000 |
0.000 |
| y |
0.000 |
4.716 |
0.000 |
| z |
0.000 |
0.000 |
4.757 |
<r2> (average value of r
2) Å
2
| <r2> |
68.155 |
| (<r2>)1/2 |
8.256 |