Abstract:Bifunctional molecules that combine independent push-pull fluorophores and azo photochromes have been synthesized to create fluorescent structures upon light-induced migration in neat thin films. Their photochromic and emissive properties have been systematically investigated and interpreted in light of those of the corresponding model compounds. Fluorescence lifetimes and photoisomerization and fluorescence quantum yields have been determined in toluene solution. Kinetic analyses of the femtosecond transient … Show more
“…In solvents like tetrahydrofuran (THF), dimethylformamide (DMF), ethyl acetate (AcOEt) or methanol, the solutions appeared orange with a band centered at 436–439 nm as commonly reported for azo derivatives due to ππ* charge transfer transitions involving the aminophenylazo unit (Figure a, Figure S1), and confirmed by TDDFT calculations at a B3LYP/6‐31G++(2d, 2p) level in THF to account for non‐covalent H‐bond interactions of AzoHBP with the solvent molecules (Figure S2). The second higher‐energy band located in the UV range around 330–340 nm can be ascribed to intramolecular charge transfer within the biphenylamino branches by analogy with previous compounds …”
Section: Methodssupporting
confidence: 57%
“…The second higherenergy band located in the UV range around 330-340 nm can be ascribed to intramolecular charget ransfer within the biphenylaminob ranches by analogy with previous compounds. [19] When using toluene, AzoHBP hardly dissolved at early times. In the course of time, the solution turned bright orange and UV/Vis absorption spectroscopy revealed the rise of two bands at 341 and 431 nm ( Figure S3 a).…”
“…In solvents like tetrahydrofuran (THF), dimethylformamide (DMF), ethyl acetate (AcOEt) or methanol, the solutions appeared orange with a band centered at 436–439 nm as commonly reported for azo derivatives due to ππ* charge transfer transitions involving the aminophenylazo unit (Figure a, Figure S1), and confirmed by TDDFT calculations at a B3LYP/6‐31G++(2d, 2p) level in THF to account for non‐covalent H‐bond interactions of AzoHBP with the solvent molecules (Figure S2). The second higher‐energy band located in the UV range around 330–340 nm can be ascribed to intramolecular charge transfer within the biphenylamino branches by analogy with previous compounds …”
Section: Methodssupporting
confidence: 57%
“…The second higherenergy band located in the UV range around 330-340 nm can be ascribed to intramolecular charget ransfer within the biphenylaminob ranches by analogy with previous compounds. [19] When using toluene, AzoHBP hardly dissolved at early times. In the course of time, the solution turned bright orange and UV/Vis absorption spectroscopy revealed the rise of two bands at 341 and 431 nm ( Figure S3 a).…”
“…We set the excitation wavelength to 305 nm for ns and 310 nm for fs transient absorption measurements. The details of the experimental setup were reported previously 29,30 and are briefly shown in the ESI. † Fig.…”
“…Such a film thickness allowed for reduced adhesion effects of the azo layer with the glass substrate known to impair photomigration, [ 17 ] and yielded absorbance around 0.5, allowing for illumination throughout the azo thin films and not only by the upper surface. The fact that both E and Z isomers closely absorb [ 34 ] makes the photomigration more efficient since both isomers could be excited at 488 nm, near their absorption maximum. Under structured polarized light irradiation, push–pull azo materials undergo considerable mass transport according to mechanisms that keep being debated between optical, [ 35 ] entropy‐driven elastic, [ 36 ] or mechanical effects, [ 37 ] to form surface relief gratings (SRGs).…”
Photochromic azo materials have stirred considerable interest for their ability to mechanically respond to polarized light through large photoinduced migration and orientation processes. In order to apprehend the microscopic dynamics behind the extensive mass transport occurring under interferential illumination, two azo compounds differing by their propensity to form hydrogen bonds are synthesized and processed as nondoped glassy thin films. Interferential irradiation using polarization and intensity patterns reveals fully distinct responses. Regular nanometer‐high surface relief gratings transform into micrometer superstructures with an amplitude ten times higher than the initial film thickness when using the latter polarization. Systematic comparisons between the azo materials in terms of thermal properties, photochromism in solution and in the solid state, and photomigration are carried out. The progressive formation of superstructures is ascribed to two successive processes. The first one relates to fast photoinduced migration due to the impinging structured light, and the second one is promoted by slower thermally activated “zig‐zag”‐like diffusion and Z‐E thermal relaxation, which in turn requests high orientational mobility of the azo compounds and causes large nanomechanical changes. Such studies should provide novel structural guidelines in terms of material fluidity to rapidly achieve highly structured and rewritable materials at low light irradiance.
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