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1 Electronic Supplementary Information Peter BOTSCHWINA* and Rainer OSWALD Institut für Physikalische Chemie, Universität Göttingen, Tammannstrasse 6, Göttingen, Germany Otto DOPFER Institut für Optik und Atomare Physik, Technische Universität Berlin Hardenbergstrasse 36, Berlin, Germany Weak interactions in ion-ligand complexes of C 3 H 3 isomers: Competition between H-bound and C-bound structures in c-c 3 H 3 L and H 2 CCCH L (L = Ne, Ar, N 2, CO 2, and O 2 ) 17 tables Tables S1-S13 provide the input for the radial energy profiles which are displayed in Figures 2-5 of the paper. Intramolecular harmonic vibrational wavenumbers for Ne and Ar complexes of c-c 3 H 3 and H 2 C 3 H are listed in Tables S14-S17.
2 TABLE S1. CCSD(T*)-F12a relative energies for neon migration around rigid c- C perpendicular to molecular plane. a θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis A: VQZ-F12(C,H), AV5Z (Ne). Equilibrium structure of c- C : r e (CH) = Å and R e (CC) = Å.
3 TABLE S2. CCSD(T*)-F12a relative energies for in-plane neon migration around rigid c- C. a θ 2 ( ) R opt (Å) E rel (cm -1 ) a Basis A: VQZ-F12(C,H), AV5Z (Ne). Equilibrium structure of c- C : r e (CH) = Å and R e (CC) = Å.
4 TABLE S3. CCSD(T*)-F12a relative energies for neon migration around rigid H 2 C 3 H perpendicular to molecular plane. a θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VQZ-F12(C,H), AV5Z (Ne). Equilibrium structure for H 2 C 3 H : r 1e (CH 2 ) = Å, α e (HCH) = , R 1e (C-C) = Å, R 2e (C C) = Å, and r 2e (CH) = Å.
5 TABLE S4. CCSD(T*)-F12a relative energies for in-plane neon migration around rigid H 2 C 3 H. a θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VQZ-F12(C,H), AV5Z (Ne). Equilibrium structure for H 2 C 3 H : r 1e (CH 2 ) = Å, α e (HCH) = , R 1e (C-C) = Å, R 2e (C C) = Å, and r 2e (CH) = Å.
6 TABLE S5. CCSD(T*)-F12a relative energies for radial N 2 migration around rigid c- C perpendicular to molecular plane. a θ 1 ( ) R opt (Å) E rel (cm -1 ) θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (C, H), AVQZ (N 2 ). Equilibrium structures: a) c- C and R e (CC) = Å; b) N 2 : R e = Å. : r e (CH) = Å
7 TABLE S6. CCSD(T*)-F12a relative energies for in-plane N 2 migration around rigid c- C along a radial path. a θ 2 ( ) R opt (Å) E rel (cm -1 ) θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (C, H), AVQZ (N 2 ). Equilibrium structures: a) c- C R e (CC) = Å; b) N 2 : R e = Å. : r e (CH) = Å and
8 TABLE S7. CCSD(T*)-F12a relative energies for radial N 2 migration around rigid H 2 C 3 H perpendicular to molecular plane. a θ 1 ( ) R opt (Å) E rel (cm -1 ) θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (H 2 C 3 H ), AVQZ (N 2 ). Equilibrium structures: a) H 2 C 3 H : r 1e (CH 2 ) = Å, α e (HCH) = , R 1e (C-C) = Å, R 2e (C C) = Å, and r 2e (CH) = Å; b) N 2 : R e = Å.
9 TABLE S8. CCSD(T*)-F12a relative energies for in-plane N 2 migration around rigid H 2 C 3 H along a radial path. a θ 1 ( ) R opt (Å) E rel (cm -1 ) θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (H 2 C 3 H ), AVQZ (N 2 ). Equilibrium structures: a) H 2 C 3 H : r 1e (CH 2 ) = Å, α e (HCH) = , R 1e (C-C) = Å, R 2e (C C) = Å, and r 2e (CH) = Å; b) N 2 : R e = Å.
10 TABLE S9. CCSD(T*)-F12a relative energies for radial CO 2 migration around rigid c- C perpendicular to molecular plane. a θ 1 ( ) R opt (Å) E rel (cm -1 ) θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (C, H), AVQZ (CO 2 ). Equilibrium structures: a) c- C and R e (CC) = Å; b) CO 2 : R e = Å. : r e (CH) = Å
11 TABLE S10. CCSD(T*)-F12a relative energies for in-plane CO 2 migration around rigid c- C along a radial path. a θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (C, H), AVQZ (CO 2 ). Equilibrium structures: a) c- C : r e (CH) = Å and R e (CC) = Å; b) CO 2 : R e = Å.
12 TABLE S11. CCSD(T*)-F12a relative energies for radial CO 2 migration around rigid H 2 C 3 H perpendicular to molecular plane. a θ 1 ( ) R opt (Å) E rel (cm -1 ) θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (C, H), AVQZ (CO 2 ). Equilibrium structures: a) H 2 C 3 H : r 1e (CH 2 ) = Å, α e (HCH) = , R 1e (C-C) = Å, R 2e (C C) = Å, and r 2e (CH) = Å; b) CO 2 : R e = Å.
13 TABLE S12. CCSD(T*)-F12a relative energies for in-plane CO 2 migration around rigid H 2 C 3 H along a radial path. a θ 1 ( ) R opt (Å) E rel (cm -1 ) θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (C, H), AVQZ (CO 2 ). Equilibrium structures: a) H 2 C 3 H : r 1e (CH 2 ) = Å, α e (HCH) = , R 1e (C-C) = Å, R 2e (C C) = Å, and r 2e (CH) = Å; b) CO 2 : R e = Å.
14 TABLE S13. UCCSD(T*)-F12a relative energies for radial O 2 migration around rigid c- C perpendicular to molecular plane. a θ 1 ( ) R opt (Å) E rel (cm -1 ) θ 1 ( ) R opt (Å) E rel (cm -1 ) a Basis: VTZ-F12 (C, H), AVQZ (O 2 ). Equilibrium structures: a) c- C and R e (CC) = Å; b) O 2 : R e = Å. : r e (CH) = Å
15 Table S14. CCSD(T*)-F12a intramolecular harmonic vibrational wavenumbers (in cm -1 ) for different structures of c- C Ne and for free c- C. a No. of vibration b C s Min 1 C s Min 2 C 2ν Min c- C (a ) (a ) (a 1 ) ( a ) (a ) (a ) (b 2 ) (e ) (a ) (a ) (a 1 ) (e ) (a ) (a ) (a 1 ) ( a ) (a ) (a ) (a 1 ) (e ) (a ) (a ) (b 2 ) (e ) (a ) (a ) (b 2 ) ( a ) (a ) (a ) (b 1 ) (e ) (a ) (a ) (a 2 ) (e ) (a ) (a ) (b 2 ) (e ) (a ) (a ) (a 1 ) 943.3(e ) (a ) (a ) (b 1 ) ( a ) ' 1 ' 1 ' 2 '' 2 a Basis: (T, Q). b Vibrations are ordered according to decreasing wavenumber.
16 Table S15. CCSD(T*)-F12a intramolecular harmonic vibrational wavenumbers (in cm -1 ) for different structures of H 2 C 3 H Ne and for free H 2 C 3 H. a No. of vibration b C s Min 1 C s Min 2 C s planar C 2ν Min H 2 C 3 H (a ) (a ) (a ) (a 1 ) (a 1 ) (a ) (a ) (a ) (b 2 ) (b 2 ) (a ) (a ) (a ) (a 1 ) (a 1 ) (a ) (a ) (a ) (a 1 ) (a 1 ) (a ) (a ) (a ) (a 1 ) (a 1 ) (a ) (a ) (a ) (a 1 ) (a 1 ) (a ) (a ) (a ) (b 1 ) (b 1 ) (a ) (a ) (a ) (b 2 ) (b 2 ) (a ) (a ) (a ) (b 1 ) (b 1 ) (a ) (a ) (a ) (b 2 ) (b 2 ) (a ) (a ) (a ) (b 2 ) (b 2 ) (a ) (a ) (a ) (b 1 ) (b 1 ) a Basis: (T, Q). b Vibrations are ordered according to decreasing wavenumber.
17 Table S16. CCSD(T*)-F12a intramolecular harmonic vibrational wavenumbers (in cm -1 ) for different structures of c- C Ar. a No. of vibration b C s Min 1 C 2ν Min (a ) (a 1 ) (a ) (b 2 ) (a ) (a 1 ) (a ) (a 1 ) (a ) (a 1 ) (a ) (b 2 ) (a ) (b 2 ) (a ) (b 1 ) (a ) (a 2 ) (a ) (b 2 ) (a ) (a 1 ) (a ) (b 1 ) a Basis: (T, Q). b Vibrations are ordered according to decreasing wavenumber.
18 Table S17. Intramolecular harmonic vibrational wavenumbers and shifts (in cm -1 ) for C s and C 2ν structures of H 2 C 3 H Ar. a No. of vibration b C s Min 1 C s Min 2 C s planar C 2ν Min (a ) (a ) (a ) (a 1 ) (a ) (a ) (a ) (b 2 ) (a ) (a ) (a ) (a 1 ) (a ) (a ) (a ) (a 1 ) (a ) (a ) (a ) (a 1 ) (a ) (a ) (a ) (a 1 ) (a ) (a ) (a ) (b 1 ) (a ) (a ) (a ) (b 2 ) (a ) (a ) (a ) (b 1 ) (a ) (a ) (a ) (b 2 ) (a ) (a ) (a ) (b 2 ) (a ) (a ) (a ) (b 1 ) a Basis: (T, Q). b Vibrations are ordered according to decreasing wavenumber.
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