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1 Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C. This journal is The Royal Society of Chemistry 2014 Supporting Information Heteroleptic Platinum(II) NHC Complexes with a C^C* Cyclometalated Ligand Synthesis, Structure and Photophysics Alexander Tronnier, a Ute Heinemeyer, b Stefan Metz, b Gerhard Wagenblast, b Ingo Münster b and Thomas Strassner *a a Physikalische Organische Chemie, Technische Universität Dresden, Dresden, Germany, Fax: ; Tel: ; thomas.strassner@chemie.tu-dresden.de b BASF SE, Ludwigshafen, Germany Table of contents: List of Abbreviations S 2 2D NMR Spectra S 3 Solid-State Determination S 11 Photoluminescence Data S 17 Device Details and Performance S 19 Quantum Chemical Calculations S 20 S1

2 List of Abbreviations 2D NMR One-/two-dimensional Nuclear Magnetic Resonance Spectroscopy acac Acetylacetonate B3LYP Becke three-parameter exchange, Lee-Yang-Parr correlation functional BP86 Becke 1988 exchange correction, Perdew86 correlation functional cd Candela CIE Color coordinates, defined by an international commission (CIE Commission internationale de l éclairage) COD 1,5-Cyclooctadiene COSY Homonuclear correlation spectroscopy DFT Density functional theory DMF Dimethylformamide DMSO Dimethyl sulfoxide ECP Effective core potential EQE External quantum yield FMO Frontier molecular orbital HMBC Heteronuclear multiple-bond correlation spectroscopy HOMO Highest occupied molecular orbital HSQC Heteronuclear single-quantum correlation spectroscopy Hz Hertz ILCT Intraligand charge transfer LLCT Ligand-to-ligand charge transfer LUMO Lowest unoccupied molecular orbital MLCT Metal-to-ligand charge transfer M.p. Melting point NHC N-Heterocyclic carbene NOESY Nuclear Overhauser effect spectroscopy OLED Organic light-emitting device/diode PMMA Poly(methyl methacrylate) SOC Spin-orbit coupling TD-DFT Time-dependent density functional theory QY Quantum yield S2

3 2D NMR Spectra N N Pt O O 8 Figure S1. COSY spectrum of complex 8. S3

4 Figure S2. HSQC spectrum of complex 8. S4

5 Figure S3. HMBC spectrum of complex 8. S5

6 Figure S4. NOESY spectrum of complex 8. S6

7 N N Pt O O 9 Figure S5. COSY spectrum of complex 9. S7

8 Figure S6. HSQC spectrum of complex 9. S8

9 Figure S7. HMBC spectrum of complex 9. S9

10 Figure S8. NOESY spectrum of complex 9. S10

11 Solid-State Determination In the following section the solid-state data for 5 8 and 12 are given. Table S1. Crystal data and crystallographic details for 5 7 Complex CCDC # empirical formula C 25 H 22 N 2 O 2 Pt C 30 H 32 N 2 O 2 Pt C 34 H 24 N 2 O 2 Pt formula weight [g/mol] T [K] 198(2) 198(2) 198(2) wavelength [Å] crystal system monoclinic monoclinic trigonal space group P 2 1 /c P 2 1 /c R -3 a [Å] (16) (3) (6) b [Å] (4) (3) (6) c [Å] (3) (16) (18) α [ ] β [ ] (16) (15) 90 γ [ ] U [Å 3 ] (8) (9) 13285(5) Z D calc [Mg/m 3 ] μ(mokα) [mm -1 ] crystal size [mm 3 ] F(000) reflections collected independent reflections 4129 R int = R int = R int = Goodness-of-fit on F R 1 [I>2σ(I)] wr 2 [I>2σ(I)] data / restraints / parameters 4129 / 0 / / 0 / / 0 / 352 S11

12 Table S2. Crystal data and crystallographic details for 8 and 12 Complex 8 12 CCDC # empirical formula C 40 H 36 N 2 O 2 Pt C 41 H 38 N 2 O 2 Pt formula weight [g/mol] T [K] 198(2) 198(2) wavelength [Å] crystal system triclinic triclinic space group P -1 P -1 a [Å] (15) (3) b [Å] (1) (2) c [Å] (12) (19) α [ ] (5) (12) β [ ] (9) (11) γ [ ] (8) (15) U [Å 3 ] (3) (11) Z 2 4 D calc [Mg/m 3 ] μ(mokα) [mm -1 ] crystal size [mm 3 ] F(000) reflections collected independent reflections 6797 R int = R int = Goodness-of-fit on F R 1 [I>2σ(I)] wr 2 [I>2σ(I)] data / restraints / parameters 6797 / 0 / / 0 / 829 S12

13 Figure S9. Molecule pair of complex 5 in the solid state. Figure S10. Molecule pair of complex 6 in the solid state. S13

14 Figure S11. Molecule pair of complex 7 in the solid state. S14

15 Figure S12. Molecule pair of complex 8 in the solid state. S15

16 Figure S13. Molecule pair of complex 12 in the solid state. S16

17 Photoluminescence Data In the following section additional photophysical data for the complexes are given. Figure S14. Absorption spectra for 5 12 and the reference complex 1 as 100% emitter films. S17

18 Figure S15. Normalized emission spectra for 6 12 and the reference complex 1 as 100% emitter films. S18

19 Device Details and Performance Al/LiF O ETL BCP : Cs 2 CO 3 (25 nm) 13 Si Si HBL 13 (5 nm) EML 8 : 13 : 14 (40 nm) 14 = [Ir(dpbic) 3 ] BCP HTL 14 (10 nm) HIL 14 :MoO 3 (10 nm) ITO N N Ir N N Glass 3 Figure S16. Device layout (left) and structure of 13 and 14 (right). ETL = electron-transport layer, HBL = hole-blocking layer, EML = emission layer, HTL = hole-transport layer, HIL = hole-injection layer. BCP = 2,9-dimethyl-4,7-diphenyl-1,10-phenanthroline. Figure S17. Single-matrix device data at different emitter (8) concentrations (5 30%) plotted against the voltage. S19

20 Quantum Chemical Calculations Table S3. Comparison of bond lengths, angles and dihedral angles of 5 from the solid-state determination and DFT calculations (B3LYP/6-31G(d)). DFT Bonds [Å]/Angles [ ] X-ray Singlet Triplet Pt(1)-C(1) 1.947(9) Pt(1)-C(9) 1.990(9) Pt(1)-O(1) 2.070(7) Pt(1)-O(2) 2.037(7) O(1)-Pt(1)-O(2) 88.1(3) C(1)-Pt(1)-C(9) 80.6(4) Pt(1)-C(1)-N(1)-C(8) 3.3(1) N(1)-C(1)-Pt(1)-O(1) 175.6(7) Table S4. Comparison of bond lengths, angles and dihedral angles of 6 from the solid-state determination and DFT calculations (B3LYP/6-31G(d)). DFT Bonds [Å]/Angles [ ] X-ray Singlet Triplet Pt(1)-C(1) 1.933(4) Pt(1)-C(9) 1.991(3) Pt(1)-O(1) 2.100(2) Pt(1)-O(2) 2.037(3) O(1)-Pt(1)-O(2) 88.79(10) C(1)-Pt(1)-C(9) 79.51(16) Pt(1)-C(1)-N(1)-C(8) -7.3(4) N(1)-C(1)-Pt(1)-O(1) (2) Table S5. Comparison of bond lengths, angles and dihedral angles of 7 from the solid-state determination and DFT calculations (B3LYP/6-31G(d)). DFT Bonds [Å]/Angles [ ] X-ray Singlet Triplet Pt(1)-C(1) 1.923(4) Pt(1)-C(9) 1.988(5) Pt(1)-O(1) 2.088(4) Pt(1)-O(2) 2.042(3) O(1)-Pt(1)-O(2) 89.35(13) C(1)-Pt(1)-C(9) 79.90(19) Pt(1)-C(1)-N(1)-C(8) -7.4(4) N(1)-C(1)-Pt(1)-O(1) (3) S20

21 Table S6. Comparison of bond lengths, angles and dihedral angles of 8 from the solid-state determination and DFT calculations (B3LYP/6-31G(d)). DFT Bonds [Å]/Angles [ ] X-ray Singlet Triplet Pt(1)-C(1) 1.923(3) Pt(1)-C(9) 1.985(3) Pt(1)-O(1) 2.074(2) Pt(1)-O(2) 2.041(2) O(1)-Pt(1)-O(2) 89.68(9) C(1)-Pt(1)-C(9) 79.87(13) Pt(1)-C(1)-N(1)-C(8) 2.8(4) N(1)-C(1)-Pt(1)-O(1) 174.7(3) Table S7. Comparison of bond lengths, angles and dihedral angles of 12 from the solid-state determination and DFT calculations (B3LYP/6-31G(d)). DFT Bonds [Å]/Angles [ ] X-ray Singlet Triplet Pt(1)-C(1) 1.950(12) Pt(1)-C(9) 1.983(12) Pt(1)-O(1) 2.074(8) Pt(1)-O(2) 2.062(8) O(1)-Pt(1)-O(2) 89.9(3) C(1)-Pt(1)-C(9) 79.9(5) Pt(1)-C(1)-N(1)-C(8) 0.3(13) N(1)-C(1)-Pt(1)-O(1) (9) Table S8. Data for the wavelength prediction (BP86/6-31G(d)). Complex S-T gap [ev] λ max uncorr. S-T gap corr. λ max corr. [nm] λ max exp. [nm] [ev] [nm] S21

22 Figure S18. Possible isomers of complex 11 (11iso, left) and 12 (12iso, right) in the S0 ground state with cyclometalation to the benzyl ring (B3LYP/6-31G(d)). S22

23 Figure S19. Gaussian shaped absorption spectra and transitions of complex 5 calculated by TD-B3LYP/CPCM (DCM) at the singlet S 0 ground state. Figure S20. Gaussian shaped absorption spectra and transitions of complex 6 calculated by TD-B3LYP/CPCM (DCM) at the singlet S 0 ground state. Figure S21. Gaussian shaped absorption spectra and transitions of complex 7 calculated by TD-B3LYP/CPCM (DCM) at the singlet S 0 ground state. S23

24 Figure S22. Gaussian shaped absorption spectra and transitions of complex 8 calculated by TD-B3LYP/CPCM (DCM) at the singlet S 0 ground state. Figure S23. Gaussian shaped absorption spectra and transitions of complex 9 calculated by TD-B3LYP/CPCM (DCM) at the singlet S 0 ground state. Figure S24. Gaussian shaped absorption spectra and transitions of complex 10 calculated by TD-B3LYP/CPCM (DCM) at the singlet S 0 ground state. S24

25 Figure S25. Gaussian shaped absorption spectra and transitions of complex 11 calculated by TD-B3LYP/CPCM (DCM) at the singlet S 0 ground state. Figure S26. Gaussian shaped absorption spectra and transitions of complex 12 calculated by TD-B3LYP/CPCM (DCM) at the singlet S 0 ground state. S25

26 Figure S27. Frontier molecular orbitals (LUMO+1, LUMO, HOMO, HOMO-1 from top to bottom) of the complexes 5 10 computed on the singlet S 0 ground state (B3LYP/6-31G(d), isovalue = 0.02). S26

27 Figure S28. Frontier molecular orbitals (LUMO+1, LUMO, HOMO, HOMO-1 from top to bottom) of the complexes 11 and 12 computed on the singlet S 0 ground state (B3LYP/6-31G(d), isovalue = 0.02). S27

28 In the following section the singlet S 0 ground state geometries for 5 12 are given (B3LYP/6-31G(d)). Coordinates for the optimized singlet ground state of 5. Pt C C C C H C C H H C N N O C C C C H H H C H H H O H C C C C H C H C H H H C C C C C H C H H H C S28 H H H Coordinates for the optimized singlet ground state of 6. Pt C C C C H C C H H C N N O C C C H C C O H C C C C H C H C H H H C C C C C H C H H H C H

29 H H C H H H C H H H C H H H C H H H C H H H Coordinates for the optimized singlet ground state of 7. Pt C C C C H C C H H C N N O C C C H O H C C C C H C H C H H S29 H C C C C C H C H H H C C C C H C H C H H H C C C C H C H C H H H Coordinates for the optimized singlet ground state of 8. Pt C C C C H C C H H C N N O C C C H O

30 H C C C C H C H C H H H C C C C C H C H H H C C C C C C H H C C C C C C H H C H H H C H H H C H H H C H H H C H S30 H H C H H H Coordinates for the optimized singlet ground state of 9. Pt C C C C H C C H H C N N O C C C H O H C C C C H C H C H H H C C C C C H C H H H C C C C C

31 C C C C C C C C H H H C H H H C H H H C H H H C H H H C H H H C H H H C H H H H H Coordinates for the optimized singlet ground state of 10. Pt C C C C H C C H H C S31 N N O C C C H O H C C C C H C H C H H H C C C C C H C H C C C C C C H H C C C C C C H H C H H H C H H H C H H H

32 C H H H C H H H C H H H C C C H C H H H Coordinates for the optimized singlet ground state of 11. Pt C C C C H C C H H C N N O C C C H O H C C C C C C H C H H H C S32 C C C H C H C H H H H H C H H H C H H H Coordinates for the optimized singlet ground state of 12. Pt C C C C H C C H H C N N O C C C H O H C C C C C C H C H H H C

33 C C C C C H H C C C C C C H H C H H H C H H H C H H H C H H H C H H H C C C C H C H C H H H H H C H H H In the following section the T 1 triplet state geometries for the complexes 5 12 are given, which were used for the wavelength prediction (BP86/6-31G(d)). S33

34 Coordinates for the optimized triplet state of 5. Pt C C C C H C C H H C N N O C C C C H H H C H H H O H C C C C H C H C H H H C C C C C H C H H H C H H H S34 Coordinates for the optimized triplet state of 6. Pt C C C C H C C H H C N N O C C C H C C O H C C C C H C H C H H H C C C C C H C H H H C H H H C H H H C H

35 H H C H H H C H H H C H H H Coordinates for the optimized triplet state of 7. Pt C C C C H C C H H C N N O C C C O H C C C C H C H C H H H C C C C C H C H S35 H H C C C C C C H H C C C C C C H H H H H H H H H Coordinates for the optimized triplet state of 8. Pt C C C C H C C H H C N N O C C C H O H C C C C H C H

36 C H H H C C C C C H C H H H C C C C C C H H C C C C C C H H C H H H C H H H C H H H C H H H C H H H C H H H S36 Coordinates for the optimized triplet state of 9. Pt C C C C H C C H H C N N O C C C H O H C C C C H C H C H H H C C C C C H C H H H C C C C C C C C C C C C

37 C H H H C H H H C H H H C H H H C H H H C H H H C H H H C H H H H H Coordinates for the optimized triplet state of 10. Pt C C C C H C C H H C N N O C C C H S37 O H C C C C H C H C H H H C C C C C H C H C C C C C C H H C C C C C C H H C H H H C H H H C H H H C H H H C H H

38 H C H H H C C C H C H H H Coordinates for the optimized triplet state of 11. Pt C C C C H C C H H C N N O C C C H C H H H C H H H O H C C C C C H C H H H C S38 H H C C C C H C H C H H H Coordinates for the optimized triplet state of 12. Pt C C C C H C C H H C N N O C C C H O H C C C C C C H C H H H C C C C C C H H

39 C C C C C C H H C H H H C H H H C H H H C H H H C H H H C C C C H C H C H H H H H C H H H In the following section the triplet state geometries for the complexes 5 12 are given, which were used for the spin density calculations (B3LYP/6-31G(d)). S39

40 Coordinates for the optimized triplet state of 5. Pt C C C C H C C H H C N N O C C C C H H H C H H H O H C C C C H C H C H H H C C C C C H C H H H C H H H S40 Coordinates for the optimized triplet state of 6. Pt C C C C H C C H H C N N O C C C H C C O H C C C C H C H C H H H C C C C C H C H H H C H H H C H H H C H

41 H H C H H H C H H H C H H H Coordinates for the optimized triplet state of 7. Pt C C C C H C C H H C N N O C C C H O H C C C C H C H C H H H C C C C C H C S41 H H H C C C C H C H C H H H C C C C H C H C H H H Coordinates for the optimized triplet state of 8. Pt C C C C H C C H H C N N O C C C H O H C C C C H C H

42 C H H H C C C C C H C H H H C C C C C C C C C C C C C H H H C H H H C H H H C H H H H H H H C H H H C H H H S42 Coordinates for the optimized triplet state of 9. Pt C C C C H C C H H C N N O C C C H O H C C C C H C H C H H H C C C C C H C H H H C C C C C C C C C C C C

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