Relationships between dipole moments of diatomic molecules. Department of Physics, Ocean University of China, Qingdao, Shandong , China 2
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1 Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2015 Supplementary Data Relationships between dipole moments of diatomic molecules Shilin Hou 1,2 and Peter F. Bernath 2,* 1 Department of Physics, Ocean University of China, Qingdao, Shandong , China 2 Department of Chemistry and Biochemistry, Old Dominion University, Norfolk, VA 23529, USA * Corresponding author. pbernath@odu.edu Contents Figure S1-S10. Results for each alkali halide molecule from all possible schemes. Page 2- Page 11 Figure S11 Results for GeX (X=O,S,Se,Te). Page 12 Figure S12. Results for the ground states of PbX (X=O,S,Se,Te) Page 13 Figure S13. Results for general molecules from different molecule sets. Page 14 Figure S14. A collection of some results some general molecules from (Δn A,Δn B ) (1,1) schemes. Table S2. Predicted dipole moments from Eqns (3) and (5) for dozens of general molecules. Page 15 Page 16-page 18 Table S3. Dipole moments (in D) for some ground-state molecules. CCSD data are calculated using Gaussian 09 package. Page 19-page 20 Table S4. Data adopted for predicted dipole moments using Eqn (5) for GaCl, InBr, SrCl, SrS, CuCl, and CuBr ground state molecules. Page 21 1 P age
2 Figure S1. LiF & LiCl. The ( n A, n B )=(4,2) result from Eqn (5) for LiCl, and similar results from nine of the LiF schemes are unphysical. 2 P age
3 Figure S2. LiBr & LiI 3 P age
4 Figure S3. KF & NaF. The results from Eqn (5) for ( n A, n B ) = (2,3), (3,2), and (3,3) schemes are unphysical. 4 P age
5 Figure S4. KCl & NaCl 5 P age
6 Figure S5. KBr & NaBr 6 P age
7 Figure S6. KI & NaI 7 P age
8 Figure S7. CsF & RbF 8 P age
9 Figure S8. CsCl & RbCl 9 P age
10 Figure S9. RbBr and CsBr. 10 P age
11 Figure S10. CsI & RbI 11 P age
12 Figure S11. Results for GeX(X=O,S,Se,Te). The results for GeTe from Eqn (5) are unphysical. 12 P age
13 Figure S12. Results for the ground states of PbX (X=O, S, Se, Te). 13 P age
14 Figure S13. Results for general molecules from different molecule sets. The results for BrCl and GeTe are unphysical. This figure also shows that molecules in the same set with larger polar charges have relative smaller errors. 14 P age
15 Figure S14. A collection of some results some general molecules from (Δn A,Δn B ) (1,1) schemes. AgF and AgCl can be seemed as exceptions, since H and Ag are not in the same group (but they have kind of similarity in electron configurations and electronegativities). 15 P age
16 Table S2. Predicted dipole moments from Eqns (3) and (5) for dozens of general molecules. Ref.17 Ref.17 Ref.13 Dipole Dipole (charge=q) (charge=1e) Mole Re/Å Dipole/D q(in e) Eqn(3) (Eqn(3)) % a Eqn(5) (Eqn(5)) % b {AB,AX,BY,XY} (Δn A,Δn B ) SnS SnO PbO SnS PbS (1,1) PbO SnO PbO SnS PbS (1,1) SnO SnO PbO SnS PbS (1,1) PbS SnO PbO SnS PbS (1,1) SnO GeO SnO GeS SnS (1,1) SnS GeO SnO GeS SnS (1,1) GeO GeO SnO GeS SnS (1,1) GeS GeO SnO GeS SnS (1,1) GeO SiO GeO SiS GeS (1,1) SiO SiO GeO SiS GeS (1,1) GeS SiO GeO SiS GeS (1,1) SiS SiO GeO SiS GeS (1,1) SnO SiO SnO SiS SnS (2,1) SnS SiO SnO SiS SnS (2,1) SiO SiO SnO SiS SnS (2,1) SiS SiO SnO SiS SnS (2,1) PbO SiO PbO SiS PbS (3,1) PbS SiO PbO SiS PbS (3,1) SiO SiO PbO SiS PbS (3,1) SiS SiO PbO SiS PbS (3,1) PbO GeO PbO GeS PbS (2,1) 16 P age
17 PbS GeO PbO GeS PbS (2,1) GeO GeO PbO GeS PbS (2,1) GeS GeO PbO GeS PbS (2,1) PbO GeO PbO GeSe PbSe (2,2) PbSe GeO PbO GeSe PbSe (2,2) GeO GeO PbO GeSe PbSe (2,2) GeSe GeO PbO GeSe PbSe (2,2) PbO GeO PbO GeTe PbTe (2,3) PbTe GeO PbO GeTe PbTe (2,3) GeO GeO PbO GeTe PbTe (2,3) GeTe Unphysical - GeO PbO GeTe PbTe (2,3) PbS GeS PbS GeSe PbSe (2,1) PbSe GeS PbS GeSe PbSe (2,1) GeS GeS PbS GeSe PbSe (2,1) GeSe GeS PbS GeSe PbSe (2,1) PbS GeS PbS GeTe PbTe (2,2) PbTe GeS PbS GeTe PbTe (2,2) GeS GeS PbS GeTe PbTe (2,2) GeTe Unphysical - GeS PbS GeTe PbTe (2,2) PbSe GeSe GeTe PbSe PbTe (2,1) PbTe GeSe GeTe PbSe PbTe (2,1) GeSe GeSe GeTe PbSe PbTe (2,1) GeTe Unphysical - GeSe GeTe PbSe PbTe (2,1) InF InF TlF InCl TlCl (1,1) TlCl InF TlF InCl TlCl (1,1) 17 P age
18 TlF InF TlF InCl TlCl (1,1) InCl InF TlF InCl TlCl (1,1) IF BrF IF BrCl ICl (1,1) ICl BrF IF BrCl ICl (1,1) BrF BrF IF BrCl ICl (1,1) BrCl Unphysical - BrF IF BrCl ICl (1,1) LiRb * LiK LiRb NaK NaRb (1,1) LiK LiK LiRb NaK NaRb (1,1) NaRb # LiK LiRb NaK NaRb (1,1) NaK LiK LiRb NaK NaRb (1,1) AgF HF HCl AgF AgCl AgCl HF HCl AgF AgCl HCl HF HCl AgF AgCl HF Unphysical - HF HCl AgF AgCl a %=[Dipole(Eqn (3))-Diploe(exp.)]/Diploe(exp) 100%. b %=[Dipole(Eqn (5))-Diploe(exp.)]/Diploe(exp) 100% * M. Ivanova, A. Stein, A. Pashov, H. Knöckel, and E. Tiemann, The X 1 Σ + state of LiRb studied by Fourier-transform spectroscopy, J. Chem. Phys. 134, (9pp) (2011) # S. Kasahara, T. Ebi, M. Tanimura, H. Ikoma, K. Matsubara, M. Baba, and H. Kato, High-resolution laser spectroscopy of the X 1 Σ + and (1) 3 Σ + states of 23 Na 85 Rb molecule, J. Chem. Phys. 105, (1996) 18 P age
19 Table S3. Dipole moments (in D) for some ground-state molecules. CCSD data are calculated using Gaussian 09 package. 18 All experimental data involved in Eqn (5) are from Ref. 17. AB Exp. 17 CCSD/ G(3df) /D a Eqn (5) /D b Scheme (Δn A,Δn B ) LiCl {LiBr+NaCl-NaBr} (1,1) NaCl {NaBr+LiCl-LiBr} (1,1) KCl {KBr+RbCl-RbBr} (1,1) LiBr {LiCl+NaBr-NaCl} (1,1) NaBr {NaCl+LiBr-LiCl} (1,1) KBr {KCl+RbBr-RbCl} (1,1) BrF {BrCl+IF-ICl} (1,1) NaK {NaRb+LiK-LiRb} (1,1) LiK {LiRb+NaK-NaRb} (1,1) SiS {SiO+GeS-GeO} (1,1) SiO {SiS+GeO-GeS} (1,1) GeO {GeS+SiO-SiS} (1,1) GeS {GeO+SiS-SiO} (1,1) GeSe {GeS+PbSe-PbS} (2,1) IF {ICl +BrF -BrCl} (1,1) ICl {IF +BrCl -BrF} (1,1) LiRb {LiK+NaRb-NaK} (1,1) NaRb {NaK+LiRb-LiK} (1,1) CsBr {CsCl+RbBr-RbCl} (1,1) RbBr {RbCl+KBr-KCl} (1,1) CsCl {CsBr +RbCl-RbBr} (1,1) RbCl {RbBr+KCl-KBr} (1,1) RbI {RbBr+CsI-CsBr} (1,1) CsI {CsBr+RbI-RbBr} (1,1) NaI {NaBr+LiI -LiBr} (1,1) KI {KBr+NaI -NaBr} (1,1) LiI {LiBr+NaI-NaBr} (1,1) InF {InCl +TlF -TlCl} (1,1) TlCl {TlF +InCl -InF} (1,1) TlF {TlCl +InF -InCl} (1,1) InCl {InF +TlCl -TlF} (1,1) SnS {SnO+PbS-PbO} (1,1) PbO {PbS+SnO-SnS} (1,1) 19 P age
20 SnO {SnS+PbO-PbS} (1,1) PbS {PbO+SnS-SnO} (1,1) PbSe {PbS+GeSe-GeS} (2,1) PbTe {PbSe+GeTe-GeSe} (2,1) Average c a =Dipole(CCSD)-Diploe(exp). b =Dipole(Eqn (5))-Diploe(exp). c The mean absolute deviation. 20 P age
21 Table S4. Data adopted for predicted dipole moments using Eqn (5) for GaCl, InBr, SrCl, SrS, CuCl, and CuBr ground state molecules. All experimental data are from Ref. 17 except those indicated. The atomic charges are also presented for references. AB R e /Å µ d /D (Predicted) BY Re/Å µ d /D q(e) AX Re/Å µ d /D q(e) XY µ d /D Re/Å q(e) GaCl InCl GaF InF InBr Tl 81 Br InCl TlCl SrCl a CaCl SrF CaF SrS b BaS SrO BaO CuCl AgF CuF AgCl CuBr AgCl CuCl c ~0.92 AgBr a From Ref. 19. b From Ref. 20. c. Theoretical data from Ref P age
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