supporting information - connecting repositoriesplanar t1 state geometries described by (i) a...
TRANSCRIPT
Supporting Information� Copyright Wiley-VCH Verlag GmbH & Co. KGaA, 69451 Weinheim, 2013
Aromaticity Effects on the Profiles of the Lowest Triplet-State Potential-Energy Surfaces for Rotation about the C=C Bonds of Olefins with Five-Membered Ring Substituents: An Example of the Impact of Baird�s Rule
Jun Zhu ,[a, b] Heather A. Fogarty,[a] Helene Mçllerstedt,[c] Maria Brink,[c] andHenrik Ottosson*[a]
chem_201300008_sm_miscellaneous_information.pdf
S1
An analysis of the correlation between excitation localization and T1 PES profile
Figure S1: Energy changes along the T1 PESs (∆E(T1) = E(T1;twisted) - E(T1;planar)) (kcal mol-1) plotted
against the degree of (anti)aromaticity at the planar T1 structure (NICS(T1;planar,1)zz) (ppm) for set A
olefins CH2=CH(C4H3X) (X = CH+, SiH+, BH, AlH, CH2, SiH2, O, S, NH, and CH-). The solid line
displays the least-squares fit against all ten data points whereas the dashed line displays a fit which
excludes the data points of A7 (X = O) and A9 (X = NH). Results from M06-2X/6-311++G(d,p) and
GIAO/M06-2X/6-311++G(d,p)//M06-2X/6-311++G(d,p) calculations.
As can be seen in Figure S1, the correlation between ∆E(T1) and the aromaticity of the planar T1 olefin,
NICS(T1;1)zz, is weakened by the inclusion of two olefins, A7 (X = O) and A9 (X = NH), as these two
species are more aromatic at their planar T1 structures than could be anticipated based on Baird’s rule on
T1 state antiaromaticity of 6π-electron cycles. With A7 and A9 removed from data used in the least-
squares fit, an r2 value of 0.941 is found for a linear fit (see dashed line of Figure S1). A similar yet
stronger deviation is observed for B7 – B9 (vide infra), and this feature is related to where in the molecule
S2
it is most favorable to distribute the two unpaired same-spin electrons of the triplet biradical. It is
noteworthy that none of the five-ring substituents -C4H3X are antiaromatic in the T1 state because the
NICS(1)zz values are negative for each of A1 – A10. The rings should instead be categorized as either
aromatic or nonaromatic.
Figure S2: Energy changes along the T1 PESs (∆E(T1) = E(T1;twisted) - E(T1;planar)) (kcal mol-1) plotted
against the olefinic C=C bond length (Å) for the planar T1 structures of set A olefins CH2=CH(C4H3X) (X
= CH+, SiH+, BH, AlH, CH2, SiH2, O, S, NH, and CH-). Results from M06-2X/6-311++G(d,p) and
GIAO/M06-2X/6-311++G(d,p)//M06-2X/6-311++G(d,p) calculations.
In the T1 state, the olefin bond lengths of A1 – A4 are short (1.357 - 1.373 Å, Figure S2) because the
triplet excitation is nearly fully localized to the ring which then becomes aromatic. In contrast, species A7
– A10 have long olefin bonds in the T1 state (1.435 - 1.461 Å, Figure S2) because the antiaromatic 6π-
electron rings force the triplet excitation to be distributed over both the olefinic C=C bond and the ring. In
S3
terms of the olefinic C=C bond length, A5 and A6 with X = CH2 and SiH2 have bond lengths which are in
between those of the olefins with 4n and 4n+2 π-electron substituents, respectively. And once again,
olefin A6 tends toward the olefins with T1 state aromatic 4π-electron substituents whereas olefin A5 tends
toward the olefins with 6π-electron substituents.
In Figure S3 it is seen that olefins B7 – B9 have NICS(T1;planar;1)zz values which are typical of
aromatic species, although these compounds in T1 should be influenced by antiaromaticity according to
Baird’s rule. Indeed, if the data points of B7 – B9 are excluded from the least-squares fit in Figure S3, an
r2 of 0.928 is obtained for a linear fit of the remaining seven data points. This finding strongly resembles
the observation made based on Figure S1.
Even though A9 in Figure S1 is an outlier, a comparison of B9 with A9 gives an explanation to the
exceptionally poor correlation for the complete set B. For planar A9 in the T1 state, the spin density reveal
that the triplet biradical character is distributed both to the C7 atom and the five-membered ring, whereas
in planar B9 it is almost fully localized to the olefinic C=C bond so that the pyrrole-ring can regain 6π-
electron (S0) aromaticity (for spin densities, see Fig. S7). This is also reflected in the NICS(T1;1)zz values
of A9 and B9 which are -6.6 and -15.7 ppm, respectively (in S0 the corresponding NICS(S0;1)zz values are
-27.8 and -28.0 ppm). Thus, the pyrrole-rings in the planar T1 structures of A9 and B9 both have some
influence of S0 aromaticity, however, this influence is greater in B9. As a result, the aromaticity gain upon
twist about the C=C bond in the T1 state of B9 is smaller than in A9 (-9.1 vs. -15.6 ppm, respectively) as
seen in Figures 3 and 6. Clearly, there is a competition between two limiting resonance structures from the
planar T1 state geometries described by (i) a markedly stabilized 6π-electron closed-shell aromatic ring
and a triplet biradical olefin bond with strong Pauli repulsion between the two adjacent same-spin
electrons, and (ii) a destabilized antiaromatic triplet biradical 6π-electron ring and a strong olefin π-bond.
This competition will be determined by the relative magnitudes of the stabilizing and destabilizing factors
in the two situations, and in B7 – B9 the first situation prevails. The extent of coupling between the ring
S4
and the olefin is dictated by the lobe sizes of the HOMO and LUMO in the S0 state (or equivalently, the
two SOMOs of the T1 state) at the C2 and C3 atoms of five-ring substituents, i.e., the connection points to
the olefin.
Figure S3: Energy changes along the T1 PESs (∆E(T1) = E(T1;twisted) - E(T1;planar)) (kcal mol-1) plotted
against the degrees of (anti)aromaticity of the planar T1 structures (NICS(T1;planar,1)zz) (ppm) of set B
olefins CH2=CH(C4H3X) (X = CH+, SiH+, BH, AlH, CH2, SiH2, O, S, NH, and CH-). The solid line
displays the least-squares fit against all ten data points whereas the dashed line displays a fit which
excludes the data points of B7 (X = O), B8 (X = S), and B9 (X = NH). Results from M06-2X/6-
311++G(d,p) and GIAO/M06-2X/6-311++G(d,p)//M06-2X/6-311++G(d,p) calculations.
With regard to the correlation between ∆E(T1) and the olefinic C=C bond lengths, the correlation
displayed in Figure S3 is negligible when compared to that of Figure S1. In this case, one contributing
factor which reduces the correlation is found through a comparison of B6 and A6 (X = SiH2) as there is a
large difference in olefinic C=C bond length in the two species (1.383 Å in A6 vs. 1.353 Å in B6). It is
S5
noteworthy that despite the longer C=C bond in A6 the rotational barrier in the T1 state is even higher for
A6 than for B6. The spin density distributions in the two olefins reveal a significant spin density increase
on the C2 from 0.54 electron in A6 to 0.94 electron in B6 suggesting a triplet excitation almost fully
localized to the ring in the latter olefin. As a consequence, the olefinic C=C bond in the planar T1 structure
of B6 has similar length as in the olefins with 4π-electron substituents, and it is even shorter than in B1
(1.353 vs. 1.367 Å). Interestingly though, the ∆E(T1) of B6 and B1 differ by more than 20 kcal/mol,
although the olefinic C=C bond is longer in the latter compound.
Figure S4: Energy changes along the T1 PESs (∆E(T1) = E(T1;twisted) - E(T1;planar)) (kcal mol-1) plotted
against the olefinic C=C bond length (Å) in the planar T1 structures of set B olefins CH2=CH(C4H3X) (X
= CH+, SiH+, BH, AlH, CH2, SiH2, O, S, NH, and CH-). Results from M06-2X/6-311++G(d,p) and
GIAO/M06-2X/6-311++G(d,p)//M06-2X/6-311++G(d,p) calculations.
S6
With regard to the spin density distribution it could be noted that the spin density of the ring is
reflected in the NICS values, and in that way also reflect the degree of triplet state aromaticity. E.g., all set
A olefins with 4π-electron substituents (A1 – A4) prefer planar olefin structures in T1 state because these
structures allow the biradical triplet aromatic character to localize to the ring in accordance with Baird’s
rule. The spin densities in the rings of A1 – A4 (1.610 – 1.864, Table S2) are therefore much higher than
in A7 – A10 with 6π-electron substituents (0.738 – 1.110), and the olefins A5 and A6 have intermediate
values (1.326 and 1.558, respectively). The general tendency for the triplet state is; the larger the spin
density in a ring the higher the aromaticity of that ring which strongly points to the importance of T1 state
aromaticity. Therefore, the spin density in the ring has similar correlation against the energy difference
between planar and twisted olefin structures in T1 (∆E(T1)) as the NICS values, and a moderate correlation
is found between the spin density in the ring and ∆E(T1) (linear fit; r2 = 0.799), which is slightly better
than that between ∆E(T1) and the NICS value of the ring (linear fit; r2 = 0.726).
S7
Table S1. Calculated energies (kcal mol-1), NICS values (ppm), and olefinic C=C bond lengths (Å) at M062X/6-311++G(d,p) level for sets A and B compounds. .
S0 T1(planar) T1(perpendicular) X
E/G NICS(S0;1)zz E NICS(T1;1)zz C6=C7 E/G NICS(T1;1)zz
∆E(T1)/∆G(T1) ∆NICS(T1;1)zz
A1* CH+ 0.0/0.0 80.2 2.8/1.9 -16.1 1.367 28.1/25.4 2.9 25.3/23.5 19.0
A2 SiH+ 0.0/0.0 38.1 11.4/10.3 -14.0 1.373 32.6/30.2 -0.9 21.2/19.9 13.1
A3 BH 0.0/0.0 34.3 17.4/16.6 -15.1 1.357 38.6/35.5 1.5 21.2/18.9 16.6
A4 AlH 0.0/0.0 13 34.2/32.2 -8.6 1.367 48.3/44.8 3.4 14.1/12.6 12.0
A5 CH2 0.0/0.0 -8.3 47.5/44.2 -2.2 1.399 52.4/47.9 -6.1 4.9/3.7 -3.9
A6 SiH2 0.0/0.0 2.5 41.6/39.0 -3.4 1.383 50.1/46.1 0.1 8.5/7.1 3.5
A7 O 0.0/0.0 -24.3 60.9/56.7 -5.0 1.448 57.3/53.0 -19.1 -3.6/-3.7 -14.1
A8 S 0.0/0.0 -23.9 58.6/55.2 -1.3 1.435 55.7/52.2 -18.5 -2.9/-2.9 -17.2
A9 NH 0.0/0.0 -27.8 63.5/59.2 -6.6 1.461 56.5/53.2 -22.2 -7.0/-6.0 -15.6
A10* CH- 0.0/0.0 -27.6 62.2/57.8 -0.2 1.459 58.9/54.8 -21.0 -3.3/-3.0 -20.8
B2 SiH+ 0.0/0.0 23.7 23.4/21.6 -15.2 1.362 42.8/39.6 4.4 19.4/18.0 19.6
B3 BH 0.0/0.0 28.5 24.1/22.4 -17.8 1.343 43.6/40.5 3.6 19.5/18.2 21.4
B4 AlH 0.0/0.0 11.0 40.7/39.1 -12.2 1.345 51.6/48.6 3.1 10.9/9.6 15.3
B5 CH2 0.0/0.0 -10.9 58.6/53.9 -0.5 1.394 57.0/53.1 -8.6 -1.6/-0.9 -8.1
B6 SiH2 0.0/0.0 0.1 50.3/46.5 -3.6 1.353 54.5/50.8 -1.1 4.2/4.2 2.5
B7 O 0.0/0.0 -24.6 70.3/65.5 -11.2 1.483 59.7/55.9 -21.8 -10.6/-9.6 -10.6
B8 S 0.0/0.0 -25.5 68.7/64.2 -7.0 1.474 58.9/55.1 -21.8 -9.8/-9.1 -14.8
B9 NH 0.0/0.0 -28.0 70.9/66.7 -15.7 1.494 59.9/56.6 -24.8 -11.0/-10.1 -9.1
* B1 and B10 are omitted as they are same with A1 and A10.
S8
Table S2. Calculated spin densities at the two olefinic carbons (Colefin) and in the rings of the set A olefins
at M062X/6-311++G(d,p) level.
T1(planar) T1(perpendicular) X
Colefin Ring Colefin Ring
A1 CH+ 0.487 1.610 1.022 1.057
A2 SiH+ 0.399 1.702 0.971 1.105
A3 BH 0.256 1.836 1.057 1.042
A4 AlH 0.229 1.864 1.138 0.930
A5 CH2 0.674 1.326 1.441 0.583
A6 SiH2 0.462 1.558 1.316 0.720
A7 O 1.153 0.974 1.658 0.377
A8 S 1.010 1.110 1.643 0.400
A9 NH 1.269 0.865 1.666 0.367
A10 CH- 1.383 0.738 1.598 0.404
S9
HC
S0 T1-planar T1-twisted
H
H
HC
HH
HC
HH
++ +
1.421
1.4371.391
1.421 1.438
1.409
1.367
1.411
1.448
1.357
1.4541.4501.410
1.396
1.345
1.4521.407
1.3601.4861.334
1.524
HSi
HH
HSi
HH
HSi
HH
+
+ +
1.399
1.4501.400
1.805 1.823
1.404
1.373
1.408
1.449
1.355
1.4591.8351.789
1.397
1.503
1.3481.450
1.3361.8551.796
1.354
HB
HH
HB
HH
HB
HH
1.378
1.4561.430
1.541 1.554
1.420
1.357
1.393
1.462
1.346
1.4661.5791.536
1.407
1.503
1.3461.454
1.3371.6011.570
1.344
HAl
H
H
HAl
HH
HAl
HH
1.373
1.4691.438
1.929 1.949
1.408
1.367
1.417
1.447
1.352
1.4691.9671.932
1.389
1.496
1.3501.456
1.3361.9691.945
1.347
A1
A2
A3
A4
H2C
HH
H2C
HH
H2C
HH
1.364
1.4741.421
1.503 1.517
1.369
1.399
1.420
1.421
1.362
1.4651.5181.503
1.365
1.464
1.3521.454
1.3351.5061.502
1.344
A5
S10
Figure S5: Optimized bond lengths (Å) at M062X/6-311++G(d,p) level for a series of five-membered
ring substituented set A olefins, CH2=CH(C4H4X) (X = CH+, SiH+, BH, AlH, CH2, SiH2, O, S, CH-, and
NH).
S11
S12
Figure S6: Optimized bond lengths (Å) at M062X/6-311++G(d,p) level for a series of five-membered
ring substituented set B olefins, CH2=CH(C4H4X) (X = CH+, SiH+, BH, AlH, CH2, SiH2, O, S, CH-, and
NH).
S13
Figure S7: Spin densities on carbon and nitrogen atoms of planar olefins A9 and B9 in triplet state.
Complete Gaussian 09 reference (reference 44)
M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman, G. Scalmani, V.
Barone, B. Mennucci, G. A. Petersson, H. Nakatsuji, M. Caricato, X. Li, H. P. Hratchian, A. F. Izmaylov,
J. Bloino, G. Zheng, J. L. Sonnenberg, M. Hada, M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida,
T. Nakajima, Y. Honda, O. Kitao, H. Nakai, T. Vreven, J. A. Montgomery, Jr., J. E. Peralta, F. Ogliaro, M.
Bearpark, J. J. Heyd, E. Brothers, K. N. Kudin, V. N. Staroverov, R. Kobayashi, J. Normand, K.
Raghavachari, A. Rendell, J. C. Burant, S. S. Iyengar, J. Tomasi, M. Cossi, N. Rega, N. J. Millam, M.
Klene, J. E. Knox, J. B. Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gomperts, R. E. Stratmann, O.
Yazyev, A. J. Austin, R. Cammi, C. Pomelli, J. W. Ochterski, R. L. Martin, K. Morokuma, V. G.
Zakrzewski, G. A. Voth, P. Salvador, J. J. Dannenberg, S. Dapprich, A. D. Daniels, Ö. Farkas, J. B.
Foresman, J. V. Ortiz, J. Cioslowski, D. Fox,. Gaussian 09, Revision A.1; Gaussian, Inc., Wallingford, CT,
2009. Table S3. Calculated relative energies of A1, A2 and A10 in gas phase and in THF solvent phase. Calculations performed with the SCRF-PCM model as described in Computational Methods.
S0 T1(planar) T1(perpendicular) Species
X
Gas phase THF Gas phase THF Gas phase THF
A1 CH+ 0.0/0.0 0.0/0.0 2.8/1.9 3.0/2.3 28.1/25.4 27.0/23.9
A2 SiH+ 0.0/0.0 0.0/0.0 11.4/10.3 14.6/13.6 32.6/30.2 34.5/31.5
A10 CH- 0.0/0.0 0.0/0.0 62.2/57.8 62.7/58.4 58.9/54.8 56.4/51.9
S14
Cartesian coordinates for all the compounds calculated in this study
A1-S0 Cs symmetry, NIMAG=0 E = -270.5255447 a.u.
C -0.43451600 -1.87156400 0.00000000
C -1.73529700 -1.07768200 0.00000000
C -1.44713400 0.23559300 0.00000000
C 0.00000000 0.34977900 0.00000000
H -0.38530400 -2.95165500 0.00000000
H -2.71964700 -1.52842800 0.00000000
H -2.13011200 1.07128700 0.00000000
C 0.68918400 1.57642900 0.00000000
H 0.11173200 2.49420800 0.00000000
C 2.04902200 1.61693000 0.00000000
H 2.65162900 0.71530200 0.00000000
H 2.58019700 2.56347300 0.00000000
H 1.63915800 -1.25247900 0.00000000
C 0.58746600 -1.01477000 0.00000000
A1-T1-planar Cs symmetry, NIMAG=0 E = -270.5210658 a.u. C -0.40018400 -1.92669800 0.00000000
C -1.63643300 -1.28964100 0.00000000
C -1.41574000 0.11378300 0.00000000
C 0.00000000 0.35767500 0.00000000
H -0.23223200 -2.99446100 0.00000000
H -2.60393000 -1.77135400 0.00000000
H -2.17953500 0.88061500 0.00000000
C 0.60272800 1.63071600 0.00000000
H -0.05751700 2.49224600 0.00000000
C 1.95501000 1.83359800 0.00000000
H 2.66267500 1.01281900 0.00000000
H 2.36303100 2.83646800 0.00000000
H 1.68404900 -1.14012100 0.00000000
C 0.62186300 -0.93880200 0.00000000
A1-T1-twisted Cs symmetry, NIMAG=1 E = -270.4807636 a.u. C 0.49790700 -1.88905900 0.00000000
C 1.70758100 -1.19263400 0.00000000
C -0.56374900 -0.96047300 0.00000000
C 1.43586900 0.19212300 0.00000000
C 0.00000000 0.37588300 0.00000000
C -0.67118100 1.55536200 0.00000000
C -2.12041000 1.67794300 0.00000000
H 0.38620700 -2.96451000 0.00000000
H 2.69432700 -1.63486300 0.00000000
H -1.62168900 -1.19130100 0.00000000
H 2.17073100 0.98731000 0.00000000
H -0.07485700 2.47237400 0.00000000
H -2.63541400 1.88805900 0.93149100
H -2.63541400 1.88805900 -0.93149100
A2-S0
Cs symmetry, NIMAG=0 E = -521.9157265 a.u. C -1.08996100 -1.89743600 0.00000000
C -1.92737700 -0.83338500 0.00000000
C -1.34414900 0.55183500 0.00000000
C 0.00000000 0.65849700 0.00000000
H -1.40486500 -2.93019100 0.00000000
H -3.00821200 -0.94436800 0.00000000
H -2.00733500 1.41078900 0.00000000
C 0.80218400 1.86697000 0.00000000
H 0.25560600 2.80553900 0.00000000
C 2.13836300 1.86884800 0.00000000
H 2.72254500 0.95282000 0.00000000
H 2.69837200 2.79511100 0.00000000
H 1.87143400 -1.71096100 0.00000000
Si 0.52843500 -1.11933700 0.00000000
A2-T1-planar Cs symmetry, NIMAG=0 E = -521.8975502 a.u. C 0.89232500 -1.93699600 0.00000000
C 1.88263500 -0.94755800 0.00000000
C 1.43454300 0.37737900 0.00000000
C 0.00000000 0.58957000 0.00000000
H 1.12892600 -2.99294100 0.00000000
H 2.93900100 -1.18767600 0.00000000
H 2.11815900 1.21984200 0.00000000
C -0.55368400 1.87970500 0.00000000
H 0.13188600 2.72368400 0.00000000
C -1.90148700 2.13930400 0.00000000
H -2.63680900 1.34138900 0.00000000
H -2.27478900 3.15527100 0.00000000
H -2.08366700 -1.57329000 0.00000000
Si -0.70347900 -1.09247900 0.00000000
A2-T1-twisted Cs symmetry, NIMAG=1 E = -521.8638282 a.u. C 1.01246300 -1.86147000 0.00000000
C 1.94313200 -0.81983900 0.00000000
C 1.44314700 0.49617200 0.00000000
C 0.00000000 0.62164900 0.00000000
H 1.31351400 -2.90055200 0.00000000
H 3.01097200 -1.00763500 0.00000000
H 2.09208700 1.36493100 0.00000000
C -0.68052600 1.79316500 0.00000000
H -0.10337300 2.72398000 0.00000000
C -2.13553700 1.89831100 0.00000000
H -2.65029000 2.11712300 0.92963100
H -2.65029000 2.11712300 -0.92963100
H -1.96409000 -1.66334500 0.00000000
Si -0.61032900 -1.10854000 0.00000000
A3-S0 Cs symmetry, NIMAG=0 E = -257.5646667 a.u.
C -0.44087600 -2.09639300 0.00000000
C -1.57719100 -1.37955700 0.00000000
C -1.31794100 0.10137000 0.00000000
C 0.00000000 0.37392300 0.00000000
H -0.41878200 -3.17755100 0.00000000
H -2.58610700 -1.78144600 0.00000000
H -2.11962200 0.83410400 0.00000000
C 0.57842800 1.70787500 0.00000000
H -0.11829900 2.54433300 0.00000000
C 1.89181500 1.95597200 0.00000000
H 2.61627400 1.14916500 0.00000000
H 2.27444000 2.96906200 0.00000000
B 0.72979200 -1.05084300 0.00000000
H 1.89772900 -1.26259700 0.00000000
A3-T1-planar Cs symmetry, NIMAG=0 E = -257.5368928 a.u. C 0.06695600 -2.08212200 0.00000000
C 1.39219000 -1.54555100 0.00000000
C 1.36580400 -0.16779000 0.00000000
C 0.00000000 0.33588800 0.00000000
H -0.10691600 -3.15149500 0.00000000
H 2.30165200 -2.13427500 0.00000000
H 2.24602800 0.46653700 0.00000000
C -0.28971800 1.72589700 0.00000000
H 0.54792000 2.42164700 0.00000000
C -1.54827700 2.23405700 0.00000000
H -2.41055500 1.57758300 0.00000000
H -1.72604300 3.30187200 0.00000000
B -0.93121500 -0.90792400 0.00000000
H -2.11774600 -0.94451900 0.00000000
A3-T1-twisted Cs symmetry, NIMAG=1 E = -257.5030906 a.u. C -1.85067400 0.94307000 0.00002100
C -2.02908000 -0.45234500 0.00001800
C -0.81853200 -1.14221800 -0.00002200
C 0.30505100 -0.20623000 -0.00004300
H -2.69613800 1.62004800 0.00005200
H -2.99225700 -0.95116100 0.00005100
H -0.71923700 -2.22176400 -0.00002500
C 1.59830500 -0.57824900 -0.00002600
H 1.83682900 -1.64766300 0.00001000
C 2.73380700 0.34975100 0.00002300
H 3.21158100 0.63625700 0.92859500
H 3.21127000 0.63686800 -0.92851600
B -0.34218400 1.23371100 -0.00000600
H 0.22560500 2.27619300 0.00002900
A4-S0 Cs symmetry, NIMAG=0 E = -475.1443517 a.u. C 0.97545500 -2.06354200 0.00000000
C 1.83750800 -1.02796400 0.00000000
C 1.32876000 0.37895000 0.00000000
C 0.00000000 0.61876700 0.00000000
H 1.35805400 -3.07687800 0.00000000
H 2.91849400 -1.16176900 0.00000000
H 2.06356600 1.18502200 0.00000000
C -0.54433000 1.96947700 0.00000000
H 0.17293400 2.79114800 0.00000000
C -1.84986000 2.25461400 0.00000000
H -2.59672200 1.46633300 0.00000000
H -2.20885900 3.27646900 0.00000000
H -2.24777600 -1.72508200 0.00000000
Al -0.76499200 -1.19515800 0.00000000
A4-T1-planar Cs symmetry, NIMAG=0 E = -475.0899151 a.u. C 0.82821500 -2.05792000 0.00000000
C 1.83609800 -1.03194300 0.00000000
C 1.43691100 0.28145400 0.00000000
C 0.00000000 0.58481000 0.00000000
H 1.16711600 -3.08802400 0.00000000
H 2.89493800 -1.27572100 0.00000000
H 2.16720600 1.08801900 0.00000000
C -0.41974900 1.92931500 0.00000000
H 0.34432000 2.70878400 0.00000000
C -1.72662100 2.33063100 0.00000000
H -2.53227000 1.60398900 0.00000000
H -1.99835000 3.37839700 0.00000000
H -2.37911200 -1.61150400 0.00000000
Al -0.87638200 -1.15554000 0.00000000
A4-T1-twisted Cs symmetry, NIMAG=1 E = -475.0674190 a.u. C 0.97449100 -2.00510000 0.00000000
C 1.88122900 -0.95235800 0.00000000
C 1.42684000 0.39001500 0.00000000
C 0.00000000 0.62783400 0.00000000
H 1.36563500 -3.01576300 0.00000000
H 2.95558100 -1.12786500 0.00000000
H 2.13730900 1.21328800 0.00000000
C -0.53072000 1.87130600 0.00000000
H 0.13966300 2.73952500 0.00000000
C -1.97161300 2.15608100 0.00000000
H -2.49152800 2.36967800 0.92679200
H -2.49152800 2.36967800 -0.92679200
H -2.24978400 -1.71961700 0.00000000
Al -0.77282400 -1.18120000 0.00000000
A5-S0 Cs symmetry, NIMAG=0 E = -271.4481473 a.u. C -1.81612800 -0.83086300 -0.00004900
C -2.02891200 0.49610200 -0.00008600
C -0.73895300 1.18858000 0.00011200
C 0.26475600 0.28232100 0.00003500
H -2.56955800 -1.60615000 0.00009200
H -2.99178500 0.98897500 -0.00014600
H -0.61156900 2.26397300 0.00028800
C 1.68957900 0.57062500 -0.00008400
H 1.95737800 1.62453500 -0.00025300
C 2.65713600 -0.34986100 0.00001500
H 2.43177000 -1.41121800 0.00018000
H 3.70248200 -0.06807900 -0.00009200
C -0.33774200 -1.09781200 0.00000500
H -0.02864900 -1.67317700 0.88041800
H -0.02848600 -1.67341400 -0.88017700
A5-T1-planar Cs symmetry, NIMAG=0 E = -271.3724653 a.u. C 1.74218200 0.90682200 -0.00002200
C 2.02093600 -0.48624300 -0.00001200
C 0.86279400 -1.20653200 0.00002200
C -0.28788200 -0.28523900 0.00001500
H 2.47965100 1.69587500 -0.00003900
H 3.01733500 -0.90753500 -0.00002800
H 0.77380600 -2.28399600 0.00004600
C -1.61390400 -0.62564100 -0.00001800
H -1.86636800 -1.68274800 -0.00005000
C -2.65958700 0.30425100 -0.00000400
H -2.46359800 1.36888500 0.00003700
H -3.69239900 -0.01463200 -0.00003200
C 0.25613900 1.13084200 0.00001800
H -0.08622000 1.69728200 0.87849500
H -0.08627100 1.69731100 -0.87842000
A5-T1-twisted Cs symmetry, NIMAG=0 E = -271.3646600 a.u. C -1.75541300 -0.90198300 0.00001600
C -2.03833800 0.43355600 -0.00003100
C -0.83840300 1.19301700 -0.00004800
C 0.27779800 0.31342100 -0.00001000
H -2.47608100 -1.70744700 0.00002100
H -3.03318800 0.85927400 -0.00005900
H -0.77189300 2.27229600 -0.00008100
C 1.59780200 0.64905600 -0.00002700
C 2.68616100 -0.33135000 0.00000600
H 3.14561200 -0.65902600 0.92627800
H 3.14516200 -0.65959800 -0.92628800
H 1.85634600 1.70855800 -0.00004800
C -0.26622200 -1.10387500 0.00007200
H 0.07690200 -1.66264600 -0.87816200
H 0.07682400 -1.66245500 0.87846900
A6-S0 Cs symmetry, NIMAG=0 E = -522.8211916 a.u.
Si -0.47339500 -1.21027200 0.00006800
C -2.13042100 -0.34219500 -0.00001800
C -1.88343700 0.97979700 -0.00003900
C -0.46433800 1.40089000 -0.00003900
C 0.46951300 0.42477700 -0.00000700
C 1.90317500 0.67794300 -0.00003300
C 2.83843100 -0.27524900 -0.00003100
H -3.13678400 -0.73974200 -0.00000500
H -2.66538500 1.73421100 -0.00005900
H -0.20914600 2.45838200 -0.00007100
H 2.21130600 1.72258400 -0.00005600
H 2.57324400 -1.32848500 -0.00000900
H 3.89413600 -0.03437000 -0.00005200
H -0.21873200 -2.03216700 1.20503400
H -0.21863800 -2.03239000 -1.20472500
A6-T1-planar Cs symmetry, NIMAG=0 E = -522.7548033 a.u. Si -0.39300300 -1.25327900 0.00009000
C -2.06237500 -0.43518600 -0.00004300
C -1.88601300 0.99058600 -0.00005300
C -0.60118000 1.45003400 -0.00001300
C 0.45710100 0.42178600 0.00002100
C 1.80825400 0.73540700 -0.00006000
C 2.82724800 -0.19902500 -0.00005200
H -3.05502900 -0.86550100 -0.00006700
H -2.73177200 1.66959700 -0.00009000
H -0.35466400 2.50693000 -0.00001200
H 2.09026800 1.78806500 -0.00013200
H 2.61183400 -1.26186800 0.00001600
H 3.86710000 0.09838000 -0.00011500
H -0.09202800 -2.08557300 1.19346100
H -0.09187800 -2.08574300 -1.19312400
A6-T1-twisted Cs symmetry, NIMAG=1 E = -522.7413041 a.u. Si -0.35568900 -1.22755700 0.00009100
C -2.06506400 -0.47689700 0.00001400
C -1.93277500 0.89269800 -0.00005900
C -0.61938000 1.43554800 -0.00007900
C 0.45133100 0.48192600 -0.00002300
C 1.77184900 0.78666700 -0.00004600
C 2.83513000 -0.22430000 -0.00001200
H -3.03992600 -0.94640800 0.00002400
H -2.79272900 1.55651100 -0.00010300
H -0.43879100 2.50539800 -0.00014200
H 3.29966700 -0.54037900 0.92727300
H 3.29928500 -0.54084100 -0.92733100
H 2.07347900 1.83829400 -0.00009500
H -0.03392900 -2.03042300 -1.20338800
H -0.03396200 -2.03020600 1.20372300
A7-S0
Cs symmetry, NIMAG=0 E = -307.3785473 a.u. C -0.80621400 -1.64193200 0.00000000
C -1.88375800 -0.81948300 0.00000000
C -1.35815600 0.51101100 0.00000000
C 0.00000000 0.38970000 0.00000000
H -0.69379300 -2.71282400 0.00000000
H -2.91839200 -1.12077000 0.00000000
H -1.90922100 1.43759400 0.00000000
C 1.06123400 1.37756700 0.00000000
H 0.72124800 2.40802200 0.00000000
C 2.36287100 1.09058700 0.00000000
H 2.71024000 0.06430800 0.00000000
H 3.10604900 1.87710600 0.00000000
O 0.34100100 -0.92476800 0.00000000
A7-T1-planar Cs symmetry, NIMAG=0 E = -307.2815083 a.u. C -0.66049800 -1.68790700 0.00000000
C -1.82754700 -0.92910900 0.00000000
C -1.45862000 0.39742400 0.00000000
C 0.00000000 0.42877900 0.00000000
H -0.48515600 -2.75026000 0.00000000
H -2.82740000 -1.33365400 0.00000000
H -2.08944200 1.27105000 0.00000000
C 0.89338000 1.43644500 0.00000000
H 0.49936200 2.44494000 0.00000000
C 2.32619600 1.22503400 0.00000000
H 2.72709700 0.22257800 0.00000000
H 3.00466500 2.06419900 0.00000000
O 0.44167600 -0.89285500 0.00000000
A7-T1-twisted Cs symmetry, NIMAG=0 E = -307.2873206 a.u. C 1.52760200 -0.98092200 0.00006300
C 2.03553100 0.28663700 -0.00010500
C 0.92595600 1.15985600 0.00024200
C -0.21985100 0.35463700 -0.00002800
H 1.98764400 -1.95478800 -0.00011900
H 3.08117200 0.54893600 0.00057500
H 0.92900300 2.23753300 -0.00048700
C -1.57153400 0.65245800 -0.00017500
C -2.62169200 -0.36173900 0.00015100
H -3.01789900 -0.75895800 -0.92745600
H -3.01854100 -0.75800700 0.92785400
H -1.83166700 1.70783300 -0.00049000
O 0.17677700 -0.96101400 -0.00009600
A8-S0 Cs symmetry, NIMAG=0 E = -630.3539755 a.u. C -1.13537100 -1.63832400 0.00000000
C -2.01870200 -0.60155500 0.00000000
C -1.36648800 0.66362100 0.00000000
C 0.00000000 0.57009600 0.00000000
S 0.49742600 -1.09229800 0.00000000
H -1.34644200 -2.69653400 0.00000000
H -3.09171400 -0.73356800 0.00000000
H -1.88273500 1.61491400 0.00000000
C 0.94589500 1.67930900 0.00000000
H 0.48038400 2.66146100 0.00000000
C 2.27519400 1.58319900 0.00000000
H 2.78150200 0.62350000 0.00000000
H 2.89701200 2.46891900 0.00000000
A8-T1-planar Cs symmetry, NIMAG=0 E = -630.2605266 a.u. C -1.08838000 -1.64291600 0.00000000
C -2.02618300 -0.59114400 0.00000000
C -1.46475200 0.65261800 0.00000000
C 0.00000000 0.62416100 0.00000000
S 0.55415800 -1.08020600 0.00000000
H -1.29549000 -2.70125200 0.00000000
H -3.09205400 -0.77664700 0.00000000
H -2.00679500 1.58781600 0.00000000
C 0.85943500 1.66817800 0.00000000
H 0.42991600 2.66524800 0.00000000
C 2.28889600 1.54231600 0.00000000
H 2.76382200 0.57042500 0.00000000
H 2.91998100 2.41842800 0.00000000
A8-T1-twisted Cs symmetry, NIMAG=0 E = -630.2651393 a.u. C 1.87565400 -0.61914400 0.00023300
C 1.97415300 0.75031400 0.00005500
C 0.72584800 1.39345300 -0.00013100
C -0.35851500 0.49865200 -0.00002900
S 0.23573400 -1.15663600 -0.00014900
H 2.67843400 -1.34001300 0.00039700
H 2.92237500 1.27058000 0.00009000
H 0.58457000 2.46568800 -0.00023900
C -1.71559200 0.78480700 0.00005300
H -1.99587500 1.83703800 0.00008300
C -2.76187500 -0.23394100 0.00011500
H -3.19959200 -0.58599700 0.92789600
H -3.19970600 -0.58596900 -0.92761800
A9-S0 Cs symmetry, NIMAG=0 E = -287.5223688 a.u. C -0.74715400 -1.75013100 0.00000000
C -1.85243100 -0.93251400 0.00000000
C -1.38102900 0.40488900 0.00000000
C 0.00000000 0.36861100 0.00000000
H -0.66424400 -2.82457400 0.00000000
H -2.87894100 -1.26141300 0.00000000
H -1.97562900 1.30542200 0.00000000
C 0.94662600 1.46905800 0.00000000
H 0.48397500 2.45138600 0.00000000
C 2.27807900 1.37682800 0.00000000
H 2.79927900 0.42515200 0.00000000
H 2.89742500 2.26398800 0.00000000
H 1.31411500 -1.29133800 0.00000000
N 0.36563900 -0.95558100 0.00000000
A9-T1-planar Cs symmetry, NIMAG=1 E = -287.4211252 a.u. C -0.65301900 -1.76540700 0.00000000
C -1.82013900 -0.98878000 0.00000000
C -1.45785500 0.34140700 0.00000000
C 0.00000000 0.41895500 0.00000000
H -0.53010500 -2.83577100 0.00000000
H -2.82215400 -1.38820100 0.00000000
H -2.10408200 1.20448800 0.00000000
C 0.82271600 1.49742700 0.00000000
H 0.36397000 2.47725400 0.00000000
C 2.28020600 1.40316600 0.00000000
H 2.79470300 0.45248700 0.00000000
H 2.88843800 2.29481700 0.00000000
H 1.38835100 -1.21034300 0.00000000
N 0.42706100 -0.91933500 0.00000000
A9-T1-twisted Cs symmetry, NIMAG=0 E = -287.4322835 a.u. C 1.60928000 -0.97014300 -0.00012700
C 2.04658500 0.34247500 -0.00019400
C 0.91103300 1.16917200 -0.00000600
C -0.23198900 0.34095500 0.00024900
H 2.16454500 -1.89375200 0.00017300
H 3.07827200 0.65634700 -0.00013800
H 0.88572000 2.24732600 0.00035600
C -1.58990700 0.65904500 -0.00012700
C -2.64756200 -0.34975000 -0.00000900
H -3.10763600 -0.68474900 -0.92502300
H -3.10792900 -0.68406200 0.92510500
H -1.85192200 1.71350200 -0.00075700
H -0.35350900 -1.77271000 -0.00186700
N 0.24397300 -0.96177500 0.00049000
A10-S0 Cs symmetry, NIMAG=0 E = -270.8874895 a.u. C -0.38423100 -1.94123600 0.00000000
C -1.64414300 -1.28413700 0.00000000
C -1.40575200 0.09309400 0.00000000
C 0.00000000 0.31025300 0.00000000
H -0.22921200 -3.01404900 0.00000000
H -2.61384100 -1.76714800 0.00000000
H -2.15384900 0.87876800 0.00000000
C 0.62049100 1.61019200 0.00000000
H -0.08615700 2.44338500 0.00000000
C 1.93262900 1.92849300 0.00000000
H 2.70027900 1.16154700 0.00000000
H 2.26077400 2.96186100 0.00000000
H 1.68776200 -1.15357100 0.00000000
C 0.62004600 -0.96845800 0.00000000
A10-T1-planar Cs symmetry, NIMAG=1 E = -270.7884122 a.u. C 0.00000000 0.38751300 0.00000000
C 0.51586200 -0.98013900 0.00000000
C -0.55958500 -1.85671600 0.00000000
C -1.77303300 -1.08693600 0.00000000
C -1.44885500 0.25943800 0.00000000
H 1.56267100 -1.24848600 0.00000000
H -0.50563400 -2.93835700 0.00000000
H -2.77463900 -1.50105000 0.00000000
H -2.13664800 1.09508100 0.00000000
C 0.74442300 1.56440100 0.00000000
C 2.20344800 1.54547600 0.00000000
H 0.23008400 2.51952100 0.00000000
H 2.78047200 2.46221400 0.00000000
H 2.75012700 0.61285700 0.00000000
A10-T1-twisted Cs symmetry, NIMAG=0 E = -270.7936749 a.u. C -0.57767400 -1.86062400 0.00000000
C -1.77950000 -1.09292200 0.00000000
C -1.43472000 0.25714900 0.00000000
C 0.00000000 0.36520200 0.00000000
H -0.52066900 -2.94288300 0.00000000
H -2.78566700 -1.49571500 0.00000000
H -2.11605200 1.10010300 0.00000000
C 0.75096700 1.55727400 0.00000000
C 2.21277200 1.58839500 0.00000000
H 2.79618500 1.53616700 0.92073000
H 2.79618500 1.53616700 -0.92073000
H 0.21397000 2.50617100 0.00000000
H 1.55561700 -1.24504200 0.00000000
C 0.50489300 -0.98030300 0.00000000
B1-S0 (same with A1-S0) B1-T1-planar (same with A1-T1-planar) B1-T1-twisted (same with A1-T1-twisted)
B2-S0 Cs symmetry, NIMAG=0 E = -521.9251661 a.u. C 0.58563000 -1.75644300 0.00000000
C 1.03889800 -0.49710500 0.00000000
C 0.00000000 0.62606900 0.00000000
C -1.30886100 0.22770900 0.00000000
H 1.21387600 -2.63556800 0.00000000
H 2.09525300 -0.25662600 0.00000000
H -2.29237300 -2.56456600 0.00000000
Si -1.23357300 -1.55176900 0.00000000
C 0.40181800 2.01171400 0.00000000
H -0.40223100 2.74000000 0.00000000
C 1.67698800 2.43286500 0.00000000
H 2.52847800 1.76392300 0.00000000
H 1.90159000 3.49292800 0.00000000
H -2.14141500 0.91582600 0.00000000
B2-T1-planar Cs symmetry, NIMAG=0 E = -521.8879518 a.u. C 0.79258300 -1.63729200 0.00000000
C 1.09029500 -0.27992800 0.00000000
C 0.00000000 0.64131100 0.00000000
C -1.29986900 -0.00930500 0.00000000
H 1.56973000 -2.38978900 0.00000000
H 2.11708400 0.06693100 0.00000000
H -1.92574500 -2.92507600 0.00000000
Si -0.98845600 -1.80603000 0.00000000
C 0.09589100 2.05988200 0.00000000
H -0.83881200 2.61140800 0.00000000
C 1.26240400 2.76272200 0.00000000
H 2.23396200 2.28330000 0.00000000
H 1.25029400 3.84511200 0.00000000
H -2.21596300 0.56819500 0.00000000
B2-T1-twisted Cs symmetry, NIMAG=1 E = -521.8569935 a.u. C -1.22573200 1.35225000 -0.00117900
C 0.10853400 1.12146000 -0.00100300
C 0.57221600 -0.29418000 0.00008100
C -0.47847200 -1.25205500 0.00081400
H -1.66002600 2.34172300 -0.00193700
H 0.84809500 1.91749300 -0.00161300
H -3.39087400 -0.73170700 0.00041700
Si -1.99804800 -0.28204600 0.00007200
C 1.89699400 -0.64533300 0.00034900
H 2.12672500 -1.71383900 0.00116700
C 3.00980700 0.28922600 -0.00036700
H 3.50542400 0.53116100 0.93361100
H 3.53654500 0.49364000 -0.92645100
H -0.29329600 -2.31803700 0.00163000
B3-S0 Cs symmetry, NIMAG=0 E = -257.5670171 a.u. C -0.95568900 -1.78870900 0.00000000
C 0.20873500 -1.13143700 0.00000000
C 0.00000000 0.37797300 0.00000000
C -1.31646000 0.67567300 0.00000000
H -1.02529100 -2.86869700 0.00000000
H 1.19578900 -1.58086100 0.00000000
B -2.09287600 -0.68584700 0.00000000
H -3.26750800 -0.85522100 0.00000000
C 1.09550200 1.33501500 0.00000000
H 0.80464400 2.38229400 0.00000000
C 2.39257600 1.01344900 0.00000000
H 2.73238800 -0.01527800 0.00000000
H 3.15782400 1.77994400 0.00000000
H -1.68144800 1.69527500 0.00000000
B3-T1-planar Cs symmetry, NIMAG=0 E = -257.5285871 a.u. C -0.59541500 -1.93537700 0.00000000
C 0.46648100 -1.00479900 0.00000000
C 0.00000000 0.31574800 0.00000000
C -1.45936800 0.30062600 0.00000000
H -0.40115800 -3.00157600 0.00000000
H 1.51765000 -1.27052200 0.00000000
B -1.93133700 -1.16508500 0.00000000
H -3.04019100 -1.58517000 0.00000000
C 0.78859600 1.52694000 0.00000000
H 0.22453300 2.45588200 0.00000000
C 2.12989000 1.58946000 0.00000000
H 2.74556600 0.69720100 0.00000000
H 2.64416600 2.54188400 0.00000000
H -2.01499100 1.23214500 0.00000000
B3-T1-twisted Cs symmetry, NIMAG=1 E = -257.4974644 a.u. C 1.70353900 -1.04340000 -0.00005100
C 0.35164900 -1.05829500 -0.00003600
C -0.22782400 0.30861100 -0.00001400
C 0.87070200 1.25406300 -0.00003500
H 2.28684200 -1.95662500 -0.00020800
H -0.28425300 -1.93866800 -0.00019600
B 2.18240200 0.44434000 0.00032400
H 3.29388700 0.86053900 -0.00029700
C -1.54439300 0.60895900 -0.00016400
H -1.81895100 1.66611100 -0.00020800
C -2.63146700 -0.37391400 0.00012300
H -3.10325500 -0.67499100 0.92795000
H -3.10347300 -0.67533700 -0.92748000
H 0.68395000 2.32111800 -0.00012200
B4-S0 Cs symmetry, NIMAG=0 E = -475.1434746 a.u. C 0.56347600 -1.80493000 0.00000000
C 0.99364900 -0.53286700 0.00000000
C 0.00000000 0.60882800 0.00000000
C -1.31893100 0.30519100 0.00000000
H 1.29067200 -2.60834000 0.00000000
H 2.05131500 -0.28083500 0.00000000
H -2.55415700 -2.68351400 0.00000000
Al -1.37874600 -1.63791200 0.00000000
H -2.03861100 1.11692300 0.00000000
C 0.48476200 1.99610200 0.00000000
H -0.29999600 2.74846900 0.00000000
C 1.75720900 2.39959500 0.00000000
H 2.59437200 1.71307900 0.00000000
H 1.99911500 3.45556900 0.00000000
B4-T1-planar Cs symmetry, NIMAG=1 E = -475.0786729 a.u. C 0.82607600 -1.66791700 0.00000000
C 1.07483500 -0.27762600 0.00000000
C 0.00000000 0.61518300 0.00000000
C -1.34319100 -0.00612500 0.00000000
H 1.69246000 -2.32141200 0.00000000
H 2.09083100 0.10837300 0.00000000
H -2.06406400 -3.14833100 0.00000000
Al -1.08891200 -1.91952900 0.00000000
H -2.18529700 0.67921400 0.00000000
C 0.13879900 2.05761000 0.00000000
H -0.79589200 2.61261100 0.00000000
C 1.28520300 2.76105000 0.00000000
H 2.25959700 2.28709000 0.00000000
H 1.26789000 3.84327600 0.00000000
B4-T1-twisted Cs symmetry, NIMAG=0 E = -475.0612600 a.u. C -0.59401300 -1.75433700 0.00000000
C -1.00087300 -0.47035500 0.00000000
C 0.00000000 0.64576600 0.00000000
C 1.37325400 0.24878000 0.00000000
H -1.34487200 -2.53694200 0.00000000
H -2.05152800 -0.18104400 0.00000000
H 2.48467200 -2.77173500 0.00000000
Al 1.35032200 -1.68398700 0.00000000
H 2.11669300 1.03839900 0.00000000
C -0.40747900 1.95419200 0.00000000
H 0.37419100 2.71616000 0.00000000
C -1.79526300 2.42018100 0.00000000
H -2.29354900 2.68081500 0.92674400
H -2.29354900 2.68081500 -0.92674400
B5-S0 Cs symmetry, NIMAG=0 E = -271.4459591 a.u. C 1.65027400 0.99155900 0.00013200
C 0.31385700 1.09648200 0.00013200
C -0.28418200 -0.25375700 -0.00007400
C 0.71611900 -1.16024100 0.00005800
H 2.35893900 1.80817100 0.00019600
H -0.24940200 2.02001900 0.00016300
C 2.04053600 -0.45907900 0.00014200
H 2.64323600 -0.71985800 -0.87835200
H 2.64316500 -0.71990500 0.87866900
C -1.71260700 -0.55920700 -0.00020700
H -1.96519700 -1.61662100 -0.00028700
C -2.69173100 0.34561100 -0.00019500
H -2.48732700 1.41025100 -0.00008600
H -3.73211300 0.04528800 -0.00027900
H 0.59510800 -2.23555200 0.00004400
B5-T1-planar Cs symmetry, NIMAG=0 E = -271.3525110 a.u. C 1.60291500 1.01507300 0.00015600
C 0.25012200 1.08214400 0.00008000
C -0.33572300 -0.22764200 -0.00004100
C 0.82191800 -1.18217100 0.00000000
H 2.26387600 1.87250900 0.00024200
H -0.31769000 2.00304300 0.00009100
C 2.10760000 -0.41200500 0.00013800
H 2.73773900 -0.62412800 -0.87629900
H 2.73759700 -0.62420700 0.87665800
C -1.67127700 -0.57866600 -0.00015400
H -1.89260400 -1.64294400 -0.00021500
C -2.75416700 0.29906100 -0.00018600
H -2.61756000 1.37271400 -0.00012700
H -3.76838700 -0.07379800 -0.00027100
H 0.72870400 -2.25796000 -0.00003400
B5-T1-twisted Cs symmetry, NIMAG=0 E = -271.3550591 a.u. C -1.58843300 1.04413600 -0.00014100
C -0.25115500 1.08099800 0.00015600
C 0.29327100 -0.29562800 -0.00003000
C -0.79658900 -1.16527500 0.00001000
H -2.25022700 1.89988500 -0.00023200
H 0.36971500 1.96791400 0.00027100
C -2.07346500 -0.38282400 0.00003100
H -2.69541500 -0.60181300 0.87772000
H -2.69544500 -0.60190600 -0.87760800
C 1.64073700 -0.63329000 -0.00001400
H 1.89496800 -1.69291300 0.00009100
C 2.73103800 0.34113300 -0.00004000
H 3.19056900 0.66907500 0.92623000
H 3.19063500 0.66894100 -0.92631800
H -0.73721800 -2.24469000 0.00001300
B6-S0 Cs symmetry, NIMAG=0 E = -522.8203333 a.u. Si -2.01864100 -0.31605000 0.00008900
C -1.18544000 1.36003100 0.00001300
C 0.13917600 1.15041000 -0.00003300
C 0.60609500 -0.27086300 -0.00002700
C -0.37468400 -1.20058700 0.00002200
H -1.60453500 2.35803600 0.00001200
H 0.86304000 1.95906200 -0.00007600
H -2.84234200 -0.57708700 1.20308700
H -2.84250100 -0.57714800 -1.20278700
C 2.03197400 -0.61673400 -0.00006800
H 2.24364800 -1.68283300 -0.00006000
C 3.05064100 0.24388800 -0.00010800
H 2.90799400 1.31766400 -0.00011500
H 4.07404600 -0.11038700 -0.00013200
H -0.14495100 -2.25947600 0.00003000
B6-T1-planar Cs symmetry, NIMAG=0 E = -522.7400966 a.u. Si -2.07755400 -0.29580000 0.00009800
C -1.17192000 1.33378300 0.00001300
C 0.20973300 1.12513600 -0.00004100
C 0.66558800 -0.19487500 -0.00003200
C -0.45405100 -1.19260400 0.00002700
H -1.56867300 2.34160900 0.00000400
H 0.90818100 1.95591400 -0.00008900
H -2.93393500 -0.54305900 1.18917300
H -2.93407400 -0.54311200 -1.18886500
C 2.03429600 -0.61432300 -0.00007200
H 2.19444700 -1.68948400 -0.00006900
C 3.12665100 0.18373700 -0.00011000
H 3.05383700 1.26467700 -0.00011100
H 4.12165000 -0.24115900 -0.00014000
H -0.21745300 -2.24931100 0.00002000
B6-T1-twisted Cs symmetry, NIMAG=0 E = -522.7334809 a.u. Si -2.04175500 -0.25741700 0.00005400
C -1.11864800 1.37261200 -0.00000800
C 0.19842400 1.11866400 -0.00012800
C 0.62821400 -0.31000500 -0.00004500
C -0.44980700 -1.22100600 0.00000800
H -1.49862400 2.38675400 0.00002800
H 0.96173800 1.89278200 -0.00018100
H -2.88798600 -0.47447200 1.19787000
H -2.88810200 -0.47451600 -1.19767200
C 1.95864100 -0.67570900 -0.00012600
H 2.18051200 -1.74348300 -0.00059300
C 3.08944500 0.25233300 0.00018300
H 3.57247500 0.54129900 0.92686500
H 3.57228400 0.54196700 -0.92638900
H -0.26534400 -2.28782100 0.00002100
B7-S0 Cs symmetry, NIMAG=0
E = -307.3740293 a.u. C 1.70084600 0.85278100 -0.00003300
C 0.36915300 1.08477300 0.00003900
C -0.26354200 -0.21093800 -0.00000200
C 0.76050600 -1.10752100 -0.00008200
H 2.56296500 1.49803500 -0.00003800
H -0.10907700 2.05049400 0.00010900
O 1.95599900 -0.47777800 -0.00010700
C -1.68571200 -0.53803900 0.00004100
H -1.92384600 -1.59849200 -0.00000300
C -2.67617700 0.35227800 0.00013300
H -2.48432100 1.41954400 0.00018000
H -3.71170800 0.03724600 0.00016400
H 0.78754900 -2.18460800 -0.00013200
B7-T1-planar Cs symmetry, NIMAG=1 E = -307.2619207 a.u. C 1.63092800 0.91399000 -0.00003000
C 0.30101500 1.07474400 0.00004100
C -0.29327000 -0.26577100 0.00000200
C 0.85189100 -1.13031200 -0.00009200
H 2.44855300 1.61617600 -0.00003400
H -0.22163800 2.01647700 0.00011400
O 1.99670500 -0.40422900 -0.00011100
C -1.60807300 -0.61883500 0.00004400
H -1.86582900 -1.67167300 0.00000700
C -2.71891900 0.36305200 0.00013700
H -2.52290700 1.42501500 0.00016800
H -3.74476500 0.02823800 0.00016500
H 0.95150600 -2.20161400 -0.00015100
B7-T1-twisted Cs symmetry, NIMAG=0 E = -307.2788627 a.u. C 1.64416700 -0.91611900 0.00006000
C 0.30503300 -1.06877200 -0.00008000
C -0.26129200 0.26765900 -0.00000100
C 0.83537200 1.10879200 -0.00003400
H 2.46591800 -1.61223900 0.00010800
H -0.24284600 -1.99739600 -0.00014400
O 1.98642700 0.39898900 0.00001300
C -1.62823500 0.62653200 0.00000600
H -1.87708500 1.68540000 0.00001700
C -2.70662900 -0.35724400 0.00002200
H -3.15016100 -0.70700900 0.92662100
H -3.15023600 -0.70706900 -0.92650500
H 0.93249800 2.18132100 -0.00004200
B8-S0 Cs symmetry, NIMAG=0 E = -630.3528971 a.u. C 0.43645900 -1.10424500 0.00012100
C -0.58747600 -0.19520500 0.00005100
C -0.09029800 1.15080900 -0.00005100
C 1.26690600 1.21185500 0.00019400
S 1.98085900 -0.35552600 -0.00012300
H 0.35438200 -2.18092700 0.00017600
H -0.71920800 2.03048200 -0.00009000
H 1.89367100 2.09036800 0.00031000
C -1.99769000 -0.59286200 0.00006000
H -2.17727600 -1.66471200 0.00019600
C -3.04002800 0.23672200 -0.00009200
H -2.91891700 1.31404000 -0.00025000
H -4.05362700 -0.14327600 -0.00007200
B8-T1-planar Cs symmetry, NIMAG=1 E = -630.2433910 a.u. C -0.52139400 -1.14233000 -0.00006200
C 0.62491000 -0.25488700 0.00001400
C 0.15323900 1.13167100 0.00003800
C -1.18271400 1.24653700 -0.00001700
S -2.01451800 -0.29953500 -0.00008800
H -0.49416000 -2.22020900 -0.00009300
H 0.81564100 1.98568000 0.00009000
H -1.76760100 2.15432400 -0.00001500
C 1.92407700 -0.65892600 0.00005700
H 2.13090900 -1.72357900 0.00002200
C 3.08493600 0.24910400 0.00014600
H 2.96247200 1.32170300 0.00021900
H 4.08670100 -0.15237300 0.00013500
B8-T1-twisted Cs symmetry, NIMAG=0 E = -630.2590311 a.u. C 0.50206200 -1.12548000 -0.00009200
C -0.58843300 -0.26229900 0.00000000
C -0.14639000 1.11551900 0.00000500
C 1.20075100 1.24179700 -0.00007400
S 2.00144000 -0.29170700 0.00006000
H 0.47877700 -2.20445500 -0.00014400
H -0.83058000 1.95378700 0.00001100
H 1.78468600 2.14948800 -0.00012000
C -1.94273000 -0.67170200 0.00000800
H -2.14757400 -1.74025700 -0.00004000
C -3.06643400 0.25975300 0.00003700
H -3.53061300 0.58161200 -0.92646800
H -3.53069700 0.58159900 0.92648600
B9-S0 Cs symmetry, NIMAG=0 E = -287.5200212 a.u. C -0.29319500 -1.89807000 0.00000000
C 0.66770800 -0.92266100 0.00000000
C 0.00000000 0.34191900 0.00000000
C -1.35246300 0.07330000 0.00000000
H -0.20821800 -2.97219600 0.00000000
H 1.73249500 -1.09237500 0.00000000
H -2.40591200 -1.75764500 0.00000000
N -1.51936700 -1.28313500 0.00000000
C 0.58431800 1.67960000 0.00000000
H -0.12891200 2.50063300 0.00000000
C 1.88748200 1.95922300 0.00000000
H 2.63799000 1.17639600 0.00000000
H 2.24099200 2.98225000 0.00000000
H -2.19595600 0.74500900 0.00000000
B9-T1-planar Cs symmetry, NIMAG=2 E = -287.4070017 a.u. C -0.40475900 -1.84230000 0.00000000
C 0.59978900 -0.92824500 0.00000000
C 0.00000000 0.40294100 0.00000000
C -1.41019900 0.17077800 0.00000000
H -0.37144900 -2.91979600 0.00000000
H 1.65315000 -1.15399500 0.00000000
H -2.51634200 -1.62433400 0.00000000
N -1.61544800 -1.17782200 0.00000000
C 0.64221600 1.61876000 0.00000000
H 0.05678300 2.52990200 0.00000000
C 2.13144200 1.73947600 0.00000000
H 2.75890000 0.86091800 0.00000000
H 2.60269000 2.71047300 0.00000000
H -2.22652700 0.87313300 0.00000000
B9-T1-twisted Cs symmetry, NIMAG=0 E = -287.4246100 a.u. C 0.45777700 -1.84101200 0.00000000
C -0.57068800 -0.94263600 0.00000000
C 0.00000000 0.38122300 0.00000000
C 1.38541600 0.20267300 0.00000000
H 0.45346400 -2.91857700 0.00000000
H -1.62398800 -1.17559200 0.00000000
H 2.55663800 -1.55323600 0.00000000
N 1.64005900 -1.13969200 0.00000000
C -0.69864500 1.61394900 0.00000000
H -0.11600400 2.53245900 0.00000000
C -2.15572900 1.69660000 0.00000000
H -2.72021800 1.74927400 0.92578400
H -2.72021800 1.74927400 -0.92578400
H 2.18112700 0.92946300 0.00000000
B10-S0 (same with A10-S0) B10-T1-planar (same with A10-T1-planar) B10-T1-twisted (same with A10-T1-twisted)