This journal is The Royal Society of Chemistry 23 Tuning the colour and efficiency in OLEDs by using amorphous or polycrystalline emitting layers. P. Brulatti, V. Fattori, S. Muzzioli, S. Stagni, P. P. Mazzeo, D. Braga, L. Maini, S. Milita and M. Cocchi Electronic Supplementary Information Electrochemistry The redox properties of the target Pt(II) complexes were investigated by cyclic voltammetry. Unfortunately, the solubility of Pt(ppy)(2-PTZ) in CH 2 Cl 2, which is one of the preferred solvents for electrochemistry, is rather low, while the fluorinated analogue Pt(F 2 ppy)(2-ptz) proved almost completely insoluble also in DMSO. Even though this feature limit the significance of the obtained results, it was possible to obtain a voltammetric curve for the complex Pt(ppy)(2PTZ) in CH 2 Cl 2 by using a glassy carbon (GC) working electrode coupled to a Platinum counter and in the presence of a saturated calomelane electrode (SCE) as the reference. In the region of the positive potentials, a Pt(II)-based and electrochemically and, likely, chemically irreversible process that is roughly centered at.9 V is observed. Relative to reductions, the voltammetric wave consist of one electrochemically irreversible process centered at -.8 V that is assigned to the formation of a ligand (ppy or 2-PTZ)-based radical anion..3x -5.25x -5.2x -5.5x -5.x -5 i / A.5x -5 -.5x -5 -.x -5 -.5x -5 -.2x -5.25.5.75..25.5 E / V
This journal is The Royal Society of Chemistry 23.25x -.25x -.5x -.75x i / A -.x -.25x -.5x -.75x -.2x -.225x -2. -.75 -.5 -.25 -. -.75 -.5 -.25 E / V Figure S. Experimental - Cyclic voltammetries were carried out using a Autolab Type III potentiostat with computer control and data storage via GPES Manager software. Solutions of concentration mm in CH 2 Cl 2 were used, containing [Bu 4 ][BF 4 ] as the supporting inert electrolyte. A three-electrode assembly was employed, consisting of a Glassy Carbon (GC) working electrode, platinum wire counter electrode and saturated calomelane (SCE) reference electrode. Solutions were purged for 5 min with solvent-saturated nitrogen gas with stirring, prior to measurements being taken without stirring.
This journal is The Royal Society of Chemistry 23 OLED configuration Pt(ppy)(2-PTZ) Pt(F 2 ppy)(2-ptz) Pt F Pt Vacuum level CH 3 CH 3 LUMO TCTA : Pt complex 2.3 2.3 2.9 F 2.8 t-bu t-bu O O O ITO 4.9 TPD : PC TCTA Pt complex 5.4 5.6 5.7 7 nm 3 nm TAZ 6.4 LiF.5nm 4.3 Al HOMO Energy (ev) nm 3 nm Figure S2. Architecture of the LEDs manufactured, and molecular structures of the materials used. These are completed with energy level diagram shown for understanding the exciton and electronic traffic within the devices. The highest occupied molecular orbital (HOMO) obtained for each material corresponds to its ionization potential. The lowest unoccupied orbital (LUMO) is equal to the molecular electronic affinity. The Fermi level positions for ITO and Al electrode contacts are added for completion. The positions of all the levels are indicated by the numbers in electronvolts relative to the vacuum level at energy zero. HOMO and LUMO levels (ev) as calculated from redox potentials.
This journal is The Royal Society of Chemistry 23 Transient Decay Analysis (a).% Pt(ppy)(2-PTZ) in PMMA.% Pt(F 2 ppy)(2-ptz) in PMMA =48 nm τ = 6.6 µs 2 3 4 =47 nm τ= 8. µs 2 3 4 5 % Pt(ppy)(2-PTZ) in TCTA (b) % Pt(F 2 ppy)(2-ptz) in TCTA =58 nm =58 nm τ =.4 µs [7%] τ = 3.8 µs τ 2 = 3. µs [3%] 3 6 9 2 5 8 2% Pt(ppy)(2-PTZ) in TCTA (c) 2 4 6 8 2% Pt(F 2 ppy)(2-ptz) in TCTA =65 nm τ =.7 µs [3%] =62 nm τ 2 = 3.5 µs [87%] τ =.4 µs 2 4 6 8 2 4 % Pt(ppy)(2-PTZ) 45 (d) 2 4 6 8 % Pt(F 2 ppy)(2-ptz) 8 3 5 τ rise =7. ns 6 4 τ rise = ns =75 nm τ =.7 µs 5 5 time (ns) =75nm τ =.5 µs 2 5 5 2 time (ns) 2 3 4 5 2 3
This journal is The Royal Society of Chemistry 23 Figure S3. Room temperature transient PL decays from both [4 wt% Pt complex :TCTA] blends (a), from both [ wt% Pt complex :TCTA] blends (b), from both [2 wt% Pt complex :TCTA] blends (c) and from neat films of both Pt complexes (d) on the microsecond time scale after excitation using light pulses of duration ns at λ exc = 373 nm. Also shown is the response time of the dimer phosphorescence from the neat films on a decimal nanosecond scale (inset) detected at = 75 nm. Open circles represent the experimental data and solid lines are decay fits. Singlephoton IBH model 5 counter were employed for the time resolved luminescence measurements. X ray diffraction Intensity () 2 8 6 4 2 5 5 2 25 3 35 2Theta ( ) Figure S4. Diffractogram of the starting bulk Pt(ppy)(2-PTZ). The powder is crystalline, the sharp peak at 2 θ= 6.3 is due to the sample holder.
This journal is The Royal Society of Chemistry 23 Intensity () 2 5 5 5 5 2 25 3 35 2Theta ( ) Figure S5. Diffractogram of the starting bulk Pt(F2ppy)(2-PTZ). Intensity () 2 5 5 5 5 2 25 3 35 4 2Theta ( ) Figure S6. Comparison of the diffractograms of: the as-deposited Pt(F2ppy)(2-PTZ) thin film (blue line), the thin film after heating at 6 C for 3 minutes (green line) and the starting crystalline powder (red line). The as-deposited Pt(F2ppy)(2-PTZ) thin film presents a strong peak at d=.6 Å which is not present in the starting material, suggesting the formation of a new form. Upon
This journal is The Royal Society of Chemistry 23 heating at 6 C the film converts into the bulk phase which can be easily detected by its colour change (from light yellow into pink) and confirmed by the presence of several peaks which correspond the starting powder structure.