Investigation into the mechanism of photo-mediated RAFT polymerization involving the reversible photolysis of the chain-transfer agent

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Electronic Supplementary Material (ESI) for Polymer Chemistry. This journal is The Royal Society of Chemistry 2017 Investigation into the mechanism of photo-mediated RAFT polymerization involving the reversible photolysis of the chain-transfer agent Benjamin Cabannes-Boué, Qizhi Yang, Jacques Lalevée, Fabrice Morlet-Savary and Julien Poly* Supporting Information I - Synthesis and characterization of methyl 2-((9H-carbazole-9-carbonothioyl)thio)-2- methylpropanoate (DTC) 1) Synthesis Materials Carbazole (Sigma-Aldrich; 95 %), carbon disulfide (CS 2 ; Sigma-Aldrich; 99.9 %), methyl α- bromoisobutyrate (Sigma-Aldrich; 99 %) and sodium hydroxide (NaOH; Sigma-Aldrich; 97 %) were used as received. Experimental procedure In a flask of 500 ml, 4.00 g of NaOH (1.00.10-1 mol) were dissolved under stirring in 250 ml of dimethylsulfoxide. Carbazole (16.7 g; 1.00.10-1 mol) was then added and the mixture was stirred for 1 h. The solution became brown. Then, CS 2 (6.0 ml; 1.0.10-1 mol) was added to the mixture which was stirred during 2.5 h, taking a red color. Finally, methyl α-bromoisobutyrate (13 ml; 1.0.10-1 mol) was added. The solution was stirred during 24 h before being poured in 1 L of distilled water. The suspension was divided in 3 portions of ~400 ml. For each portion, 4 extractions with 100 ml each of dichloromethane were performed, before the organic phases were gathered and washed 4 times with 100 ml of distilled water (the 4 th aqueous phase was transparent). The solvent was evaporated and the product was recrystallized in methanol (MeOH). Total yield after purification: 42 %. 2) 1 H NMR Spectrum Figure S1. 1 H NMR spectrum of DTC

II - Polymerization tests by conventional thermal RAFT using DTC 1) Polymerization procedures Synthesis of a PS 149.5 mg of DTC (4.35 10-1 mmol, 1 eq.) and 4530 mg of S (100 eq.) were added in this order into a dried Schlenk flask. The solution was thoroughly deoxygenated by three freeze-pump-thaw cycles. The flask was filled with nitrogen gas and placed in an oil bath maintained at 110 C for 24 h under magnetic stirring. Solvent was then evaporated under vacuum. Synthesis of a PMMA 10.2 mg of AIBN (0.15 eq.), 142.1 mg of DTC (4.14 10-1 mmol, 1 eq.), 2070.5 mg of MMA (50 eq.) and dioxane (5.00 ml) were added in this order into a dried Schlenk flask. The solution was thoroughly deoxygenated by three freeze-pump-thaw cycles. The flask was filled with nitrogen gas and placed in an oil bath maintained at 70 C for 7 h under magnetic stirring. Solvent was then evaporated under vacuum. Synthesis of a PBA 8.2 mg of AIBN (0.15 eq.), 113.6 mg of DTC (3.30 10-1 mmol, 1 eq.), 2120.4 mg of BA (50 eq.) and dioxane (5.00 ml) were added in this order into a dried Schlenk flask. The solution was thoroughly deoxygenated by three freeze-pump-thaw cycles. The flask was filled with nitrogen gas and placed in an oil bath maintained at 80 C for 6 h under magnetic stirring. Solvent was then evaporated under vacuum. Synthesis of PNVC 3.6 mg of AIBN (0.25 eq.), 29.8 mg of DTC (8.6 10-2 mmol, 1 eq.), 839.2 mg of NVC (50 eq.) and dioxane (2.00 ml) were added in this order into a dried Schlenk flask. The solution was thoroughly deoxygenated by three freeze-pump-thaw cycles. The flask was filled with nitrogen gas and placed in an oil bath maintained at 80 C for 24 h under magnetic stirring. Solvent was then evaporated under vacuum. 2) Characterization by SEC M n (g/mol) M w (g/mol) Đ = M w / M n DP n PS 5.20 10 3 5.48 10 3 1.05 47 PMMA 1.29 10 4 1.49 10 4 1.16 126 PBA 6.81 10 3 7.56 10 3 1.11 50 PNVC 4.82 10 3 5.90 10 3 1.22 23 Table S1. Results of the preliminary syntheses realized with DTC under thermal conditions

III - Effect of light intensity a b c Figure S2. Kinetic monitoring of the photo-mediated RAFT polymerization of BA using a blue LED (0.9 W, λ em,max = 465 nm). a. SEC chromatograms (RI detector). b. Polymerization kinetics. c. Evolution of number average molecular weight (M n ) and dispersity (Đ = M w /M n ) with conversion; line: theoretical molecular weight. [BA] 0 /[DTC] 0 = 120; Dioxane/BA: 3/1 in volume

IV - Kinetic modeling of a reversible photolysis The kinetic scheme can be represented as follows: h P-X* k d P-X k k r P + X With PX being the dormant species (macrocta), PX* the corresponding excited state generated under irradiation, P the propagating species (carbon-centered radical) and X the thiocarbonylthiyl (sulfur-centered radical). Making the approximation that the light source is monochromatic, the rate of disappearance of PX due to light irradiation is: ( d[px] dt )hν = I A PX abs A With I abs being the absorbed intensity, A the total absorbance and A PX the absorbance due to PX only. Considering the establishment of a steady state, the following relations are obtained: Steady state approximation applied to the dormant species at the ground state: d[px] A PX = I dt abs A k[px ] k r [P ][X ] 0 Steady state approximation applied to the dormant species at the excited state: d[px ] dt = I abs A PX A k[px ] k d [PX ] 0 Steady state approximation applied to the active species: d[p ] = k dt d [PX ] k r [P ][X ] 0 These relations lead to the following equation, governing the reversible photolysis process: I abs A PX A φ d = k r [P ][X ]

Where the quantum yield of photodissociation is introduced: k d φ d = k d + k The law of conservation of matter can be summarized as follows: PX PX* P X Initially: C 0 Equilibrium: C 0.[1 - (x + y)] C 0.y C 0.x C 0.x With C 0 being the initial concentration of the CTA. The 2 following approximations can be then introduced: A PX The concentration of PX* is negligible (short-lived excited state): x y Only the absorptions of PX and X are considered (which implies no other absorbing species): A = PX [PX] PX [PX] i [i] PX [PX] + X [X ] i The following equation is thus obtained: I abs.φ d ( C 2 0.k = 1 + X r PX x 1 x) x2 If we assume that (only a low fraction of active species): 1 x The equation becomes: I abs.φ d ( C 2 0.k = 1 + X x) r PX x2 And finally, expressing I abs as a function of the absorbance A and incident intensity I 0 : I 0.(1 10 A ).φ d ( C 2 0.k = 1 + X x) r PX x2

V - Reinitiation efficiency Chain-extension with BA starting from a PBA macrocta synthesized by conventional thermal RAFT (RI chromatogram after 3 h of reaction): a The comparison of the areas of the peaks corresponding to the chain-extended product PBA-b- PBA and to the residual PBA macrocta, considering a same dn/dc, enables the estimation of the residual fraction of PBA precursor: 3.5 %. Chain-extension with BA starting from a PS macrocta synthesized by conventional thermal RAFT (RI chromatogram after 3 h of reaction): b The comparison of the areas of the peaks corresponding to the block copolymer PS-b-PBA and to the residual PS macrocta, considering their respective dn/dc values, enables the estimation of the residual fraction of PS precursor: 9.4 %. For the PS, the dn/dc value used was 0.185 ml/g. For the PS-b-PBA copolymer, an average value was calculated considering the number average degree of polymerization of each block (PS block: 43; PBA block: 131): dn/dc = 0.091 ml/g.

VI - Effect of the wavelength a b c Figure S3. Kinetic monitoring of the photo-mediated RAFT polymerization of BA using a green LED (3 W, λ em,max = 525 nm). a. SEC chromatograms (RI detector). b. Polymerization kinetics. c. Evolution of number average molecular weight (M n ) and dispersity (Đ = M w /M n ) with conversion; line: theoretical molecular weight. [BA] 0 /[DTC] 0 = 120; Dioxane/BA: 3/1 in volume

VII Chain-end fidelity a b c Figure S4. Kinetic monitoring of the photo-mediated RAFT polymerization of BA using a blue LED (3 W, λ em,max = 472 nm) starting from a PBA (M n = 4.10 10 3 g.mol -1 ; Đ = 1.16) synthesized by photomediated RAFT as a macrocta. a. SEC chromatograms (RI detector). b. Polymerization kinetics. c. Evolution of number average molecular weight (M n ) and dispersity (Đ = M w /M n ) with conversion; line: theoretical molecular weight. [BA] 0 /[PBA] 0 = 200; Dioxane/BA: 3/1 in volume