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Wavelength-optimized Two-Photon Polymerization Using Initiators Based on Multipolar Aminostyryl-1,3,5-triazines

Two-photon induced polymerization (2PP) based 3D printing is a powerful microfabrication tool. Specialized two-photon initiators (2PIs) are critical components of the employed photosensitive polymerizable formulations. This work investigates the cooperative enhancement of two-photon absorption cross sections (σ2PA) in a series of 1,3,5-triazine-derivatives bearing 1-3 aminostyryl-donor arms, creating dipolar, quadrupolar and octupolar push-pull systems. The multipolar 2PIs were successfully prepared and characterized, σ2PA were determined using z-scan at 800 nm as well as spectrally resolved two-photon excited fluorescence measurements, and the results were compared to high-level ab initio computations. Modern tunable femtosecond lasers allow 2PP-processing at optimum wavelengths tailored to the absorption behavior of the 2PI. 2PP structuring tests revealed that while performance at 800 nm is similar, at their respective σ2PA-maxima the octupolar triazine-derivative outperforms a well-established ketone-based quadrupolar reference 2PI, with significantly lower fabrication threshold at exceedingly high writing speeds up to 200 mm/s and a broader window for ideal processing parameters.

2PA chromophores (even dendritic and polymeric 2PA active compounds) are favorable as electronic coupling between the branches leads to a cooperative enhancement that can cause a rise of σ 2PA 10 . The heterocyclic system 1,3,5-triazine is strongly electron deficient, so it is an excellent electronic acceptor group, and it has three carbon atoms to which branching substituents can be attached to create dipolar-, quadrupolar-, and octupolar push-pull-systems. Detailed structural analyses of star shaped 1,3,5-triazine-based compounds were carried out to investigate the planarity of the system. X-ray structure analyses of the one-and two-branched counterparts and a computer model of the three-branched compound revealed a highly planar conformation of the π-systems 11 . Furthermore, derivatives of heterocycles that contain pyridine-type nitrogen atoms often exhibit low fluorescence quantum yields 12 . This is desirable for 2PIs as fluorescence is a common loss channel, competing with the initiation of polymerization. The recently developed ketone-based 2PI M2CMK (Fig. 1) takes advantage of carbonyl moieties as electronic acceptor groups that ensure low fluorescence and is used in this work as a reference material 12,13 . The 2PA-behavior of 1,3,5-triazine derivatives has been investigated before; however, their application as 2PIs, especially regarding high writing speeds up to over 100 mm/s, has not been demonstrated so far. Previous studies show that 1,3,5-triazine derivatives bearing 1,4-phenylenevinylene arms with terminal dialkylamino-groups (aminostyryl-1,3,5-triazines) exhibit relatively high 2PA that strongly increases in a non-linear fashion with the number of branches 11,14,15 . These factors make branched systems containing a triazine core element promising 2PI-candidates, so that in this work a series of multipolar aminostyryl-1,3,5-triazines ( Fig. 1) was prepared to investigate their relevant photophysical properties and particularly their efficiency regarding the application as 2PIs.

Results
Synthesis. The molecules BTrz, 2BTrz, and 3BTrz ( Fig. 1) based on the 1,3,5-triazine acceptor form a series of di-, quadru-, and octupolar molecules, respectively, that were synthesized to investigate their suitability as 2PIs. Previous investigations of similar series regarding their 2PA behaviour employed methyl-and ethyl-groups as substituents on the terminal amino-groups 14,15 . As high solubility of 2PIs in polymerizable resin mixtures is crucial for the 2PP process, dibutylamino-groups were used as solubility promoting electronic donor groups in this work to circumvent the limited solubility often associated with highly planarized aromatic π-systems.
The required precursor 2,4,6-trimethyl-1,3,5-triazine (Trz) was prepared according to literature 16 from commercially available ethyl acetimidate hydrochloride, which is first converted to the free base and then trimerized under the influence of catalytic amounts of glacial acetic acid. The three increasingly branched aminostyryl triazine derivatives were then obtained analogous to literature 14 by subsequently reacting the three methyl groups of Trz with 4-(dibutylamino)benzaldehyde (DBA) in a Knoevenagel-type condensation under alkaline catalysis using potassium hydroxide in methanol (Fig. 2).
For BTrz only rather low yields of around 10% could be obtained even with a molar ratio of 2:1 for Trz:DBA. This is presumably because BTrz, due to additional resonance stabilization of intermediate carbanions, is more reactive than Trz towards condensation reactions on the methyl groups. Thus considerable amounts of 2BTrz as well as intermediate highly polar addition products are formed despite the unfavorable molar ratios of the starting materials.  2BTrz and 3BTrz were isolated in yields of 62% and 23% respectively from a reaction mixture with a molar ratio of 1:3.5 for Trz:DBA.
Photophysical properties. The basic relevant one-and two-photon photophysical properties of BTrz, 2BTrz, and 3BTrz as well as the reference M2CMK in THF are summarized in Table 1.
One Photon Spectra. Figure 3 shows the electronic absorption and emission spectra of BTrz, 2BTrz and 3BTrz in THF. All three samples show a pronounced lowest energy absorption band slightly above 400 nm. The extinction coefficient of this band scales with the number of branches and the values are in good agreement with those published for a series of similar compounds 11 . The lowest energy absorption band of 2BTrz and 3BTrz is slightly shifted to lower energies (by 1200 cm −1 ) with respect to BTrz. In addition, this band shows a pronounced shoulder at higher energy for 2BTrz, which is absent for 3BTrz. These findings are in line with previous reports on a similar series of di-, quadru-and octupolar donor-acceptor systems 17 and can be similarly rationalized using a Frenkel exciton model for the interactions among the branches. All three samples exhibit structureless emission spectra with a Stokes shift of almost 4000 cm −1 , indicating significant charge-transfer character in the excited state. The emission quantum yields for 2BTrz and 3BTrz amount to 0.2, thus being by almost a factor of 4 and 100 larger than those for BTrz and M2CMK, respectively. Whether the nonradiative deactivation processes, accounting for the major portion of the population decay, are due to internal conversion back to the ground state, or intersystem crossing to energetically accessible triplet states, will be discussed in a forthcoming publication.
Two-photon absorption cross sections, σ 2PA . A strong non-linear dependence on the number of branches was observed for the σ 2PA measured by z-scan at 796 nm. Doubling the number of branches from one branch in BTrz (60 GM) to two branches in 2BTrz (244 GM) leads to a 4.1-fold cross section for the latter compound. However, adding a third branch in 3BTrz (275 GM) only leads to a slight increase (4.6-fold the value of BTrz) of the cross section compared to 2BTrz (Fig. 4).
A qualitatively similar picture is obtained from two-photon excited fluorescence (2PEF) measurements, which allow for monitoring a large spectral range of technical interest (680 to 1000 nm). The fact that the σ 2PA values at 796 nm obtained from the two different methods differ slightly (cf. Table 1), may be attributed to the difference in sample concentration of almost 3 orders of magnitude, as required by the different methods. In addition, it is well known that absorption based techniques may be prone to complications like e.g. disturbing excited state absorption, etc 18,19 . Fluorescence based techniques on the other hand are prone to larger errors, when the fluorescence quantum yields are very small (as e.g. for M2CMK) 20 . Fig. 4 shows a comparison of the one-and two-photon cross sections as a function of wavelength. For dipolar BTrz both spectra are virtually identical in terms of bandshape,   with the maximum close to 800 nm. The situation completely changes for 2BTrz and 3BTrz, which both show strong two-photon maxima at significantly lower wavelengths than the one-photon maxima. While for 2BTrz this maximum exactly shows up at 800 nm, it is shifted by almost 50 nm to the blue for 3BTrz. Thus, whereas the two-photon cross section maxima scale with increasing branch number as expected from calculations (vide infra), the cross section at 800 nm is almost the same for the two multipolar samples. Figure 5 shows the relative (i.e. normalized with respect to the number of branches) enhancement of 2BTrz and 3BTrz with respect to BTrz.
In line with literature 17 , a significant enhancement for quadrupolar 2BTrz and octupolar 3BTrz is observed in the red part of the spectrum. The enhancement of octupolar 3BTrz in the blue part of the spectrum is significantly more pronounced than that for quadrupolar B2Trz. Contrary to the results from the aforementioned refs 3,17 , BTrz shows an "enhancement" below 1 for the spectral range where BTrz has its maximum. Calculated one-photon (black columns) and two-photon allowed transition wavelengths (red columns), are shown as stick-spectra (degenerate or near-degenerate transitions are presented as a single transition). All calculated results (f and σ 2PA from Table 2) were red-shifted by 3500 cm −1 and scaled with a single constant factor to match the experimental data for BTrz. Note that the 2PA stick spectra in black were offset by 6 nm from the 1PA peaks for clarity of presentation.  Computational investigation. The molecular structures of the methyl analogues of the molecules considered here (MTrz, 2MTrz, 3MTrz), were optimized in THF solution using density functional theory (DFT) and the M06-2X functional 21 . The resulting structures are almost perfectly planar, suggesting strong π-conjugation effects along the whole molecule connecting the amino groups to the triazine ring. Excitation energies, as well as oneand two-photon absorption strengths, computed using the ab-initio ACD(2) method 22,23 in THF solution, are presented in Table 2. The data reflects the experimental results of Table 1 well, with the exception that the absorption maxima are consistently shifted to somewhat higher energies (by approximately 3500 cm −1 ). In the case of MTrz, the lowest excited state possesses delocalized charge transfer (CT) character in which electron density shifts from the amino group through the side chain into the triazine ring. In the case of 2MTrz (3MTrz) two (three) such states are present, one for each side chain. While the interactions of these states could be quantified by the use of essential state models 24,25 , here we will discuss the spectra on a qualitative level. In the case of 2MTrz, two states with non-vanishing one-photon absorption are computed, in agreement with the fact that a shoulder of the main peak is seen in the absorption spectrum at around 27000 cm −1 (Fig. 3). The lower energy state possesses the stronger one-photon absorption strength. According to a three-state essential state model 25 , this state then serves as an intermediate state for the enhanced two-photon absorption of the higher energy state.
In the case of 3MTrz the situation is somewhat more involved. In this case, approximate C 3h symmetry is present and the states transform as the irreducible representations of this point group. Accordingly, there are two intense quasi-degenerate states of E' symmetry and a third A' state, which is one-photon forbidden. This combination leads to only one peak in the linear absorption spectrum, in agreement with Fig. 3. In analogy to 2MTrz the dark state possesses the largest two-photon absorption strength. In summary, the results show that moving from MTrz to 2MTrz qualitatively changes the mode of two-photon absorption resulting in an increase by more than a factor of three, while only a smaller modification occurs when proceeding to 3MTrz.
2PP structuring tests. In literature, several methods have been used to quantitatively test 2PI performance.
Single-line writing is well suited to test resolution limits 26 , while printing of more complex shapes at different laser intensities and writing speeds gives a more detailed and practically relevant picture regarding the performance of 2PP as a 3D microfabrication technique. Since the absorption maxima of 2PIs can only be roughly controlled by chromphore design and tunable fs-pulsed NIR-laser systems have been commercially available for some time 27 , in this work the influence of adjusting the laser wavelength to the σ 2PA -maxima of the 2PIs (Table 1 and Fig. 4) was also investigated. Thus arrays of defined woodpile-structures were produced varying the laser power (4-22 mW for low energy segment and 50-140 mW for high energy segment) and writing speed (20-200 mm/s) at 800 nm (the wavelength most commonly used with commercial Ti:sapphire fs-lasers) as well as the laser wavelength corresponding to the σ 2PA -maxima, using formulations containing the 2PIs in a mixture of acrylate resins (ETA/TTA = 1:1). To take into account the different size of the delocalized π-systems and maintain comparability, 2BTrz and the reference M2CMK were dissolved at 5 µmol 2PI/g resin, while BTrz was used at 2-fold and 3BTrz at 0.66-fold concentration. While the crystalline compounds 3BTrz and M2CMK required the addition of acetone as a co-solvent for dissolution (removed in vacuo before processing), BTrz and 2BTrz were dissolved far easier by the acrylates mixture.
Laser scanning microscopy (LSM) images of the polymerized woodpile-structures were judged visually and divided in four different quality classes (Fig. 6A), indicating excellent structures with fine hatch-lines in green, good structures with thicker hatch-lines and/or small defects in yellow, structures of inacceptable quality due to holes and exploded regions caused by overexposure in red, and structures that were distorted, incomplete or collapsed due to underexposure in blue. For 2PP 3D printing applications, ideal processing windows (green and yellow color codes) over a broad range of parameters are desired, as well as low laser power fabrication thresholds that allow splitting of the initial laser beam for parallel processing at high feed rates for high throughput in mass production, and high laser power overexposure thresholds for thermally induced decomposition of the material 28 . Figure 6B highlights the virtues of 2PP as a 3D printing technique and demonstrates that structures with complex geometry, delicate features and overhangs can be produced using the novel triazine 2PI 2BTrz at impressive writing speeds up to 200 mm/s.  Figure 7 visualizes the processing windows of the 2PIs. The data represent the percentage of structures falling into a certain quality class that were obtained by varying writing speeds from 20 to 200 mm/s in 20 mm/s steps, and laser powers from 4-22 mW in 2 mW steps to assess low energy performance and from 50-140 mW in 10 mW steps to assess high energy performance respectively. Table 3 lists the individual threshold laser powers for    the fabrication of green class structures at the highest tested writing speed, as well as first red class (overexposed) structures at the lowest tested speed. At 800 nm, 3BTrz has a processing window similar to reference M2CMK, with a 20 mW higher overexposure threshold, but also more yellow class structures. Compared to the latter, 2BTrz (that is already at its 2PA maximum at 800 nm) has a smaller ideal processing window, manifesting in a slightly higher fabrication threshold as well as a lower overexposure threshold. Despite the adjustment of 2PI concentration to compensate the reduced size of the π-system, BTrz apparently produces significantly fewer radicals compared to the other 2PIs, so that no ideal structures could be obtained in the low energy segment, and no overexposure was observed in the high energy segment. Even though only a 15 nm increase of the laser wavelength was required to print at the 2PA maximum of BTrz, the overall performance was most drastically affected by the wavelength shift compared to the other 2PIs. At the same time, the ideal processing window at the 2PA maximum was the smallest of the tested 2PIs. Both 3BTrz and M2CMK produce radicals more efficiently at their respective 2PA maxima of 750 nm and 760 nm, resulting in both lower fabrication and overexposure thresholds. Overall, at its 2PA maximum 3BTrz has the broadest ideal processing window of all tested compounds, with a fabrication threshold of 12 mW (14 mW for M2CMK at 760 nm) and an overexposure threshold of 120 mW (100 mW for M2CMK at 760 nm).

Discussion
A series of multipolar aminostyryl-1,3,5-triazine two-photon initiators (2PIs) with one (dipolar), two (quadrupolar), and three (octupolar) styryl donor arms, BTrz, 2BTrz, and 3BTrz, was successfully prepared and evaluated in comparison to the well-established quadrupolar benzylidene ketone based reference M2CMK. While the one-photon absorption and emission maxima were similar both within the triazine series and compared to the reference, the fluorescence quantum yields of the triazine series were 1-2 orders of magnitude larger than for the ketone based system. The triazines displayed high two-photon absorption cross sections (σ 2PA ) similar to the reference 2PI, both in z-scan and two-photon excited fluorescence (2PEF) based measurements, and a marked cooperative enhancement of 2BTrz compared to the dipolar analogue that flattened again for the octupolar system. This was also in accordance with computations performed in this study. The use of dibutylamino-donor groups ensured excellent solubility and processability of the 2PIs in the acrylate-based resin used for two-photon polymerization (2PP) based 3D printing. At 800 nm, a common operation wavelength for 2PP printers employing commercial fs-pulsed Ti:sapphire lasers, the ideal processing windows and overall performance of 2BTrz and 3BTrz were similar to the reference M2CMK, while BTrz required much higher laser powers to be active, even though the 2PI concentration was adjusted to account for the smaller delocalized π-system. By tuning the laser wavelength to the σ 2PA -maxima determined via 2PEF-spectroscopy, all investigated systems showed a marked increase in sensitivity, i.e. thresholds for fabrication of ideal structures as well as thermally induced decomposition of the formulation were lowered. Interestingly, and despite a significantly lower absolute value of σ 2PA at its maximum compared to M2CMK, 3BTrz exhibited a larger ideal processing window at the optimum wavelength. Thus, the study demonstrated that besides the choice and design of the employed 2PI, optimizing the laser wavelength is a valuable step to increase efficiency and performance of 2PP based 3D printing.

Materials. Ethyl acetimidate hydrochloride and 4-(dibutylamino)benzaldehyde (DBA) were purchased from
Sigma-Aldrich and used without further purification. The solvents and other reagents were purchased from Sigma Aldrich, Fluka and Merck and were dried and purified by standard laboratory methods. Trimethylolpropane triacrylate (TTA, Genomer 1330) and ethoxylated-(20/3)-trimethylolpropane triacrylate (ETA, Sartomer 415) were received as a gift from Rahn and Sartomer, respectively. Thin layer chromatography analysis was performed on silica gel 60 F 254 aluminium sheets from Merck. Column chromatography was performed by preparative MPLC using a Buechi Sepacore Flash System (Buechi pump module C-605, Buechi control unit C-620, Buechi UV-Photometer C-635 with peak detection set at λ = 295 nm, Buechi fraction collector C-660). Glass and polyethylene columns were used, packed with Silicagel 60 on VWR silica gel 60 (0.040-0.063 mm particle size).
The preparation and analysis of the photosensitive compounds and formulations was conducted in an orange light lab. The windows and fluorescent lamps were covered in adhesive foils or coated so that light with a wavelength < 520 nm was cut off.
Synthesis. 2,4,3,. Prepared according to literature 16  The reaction mixture magnetically stirred under argon for 120 h at 60 °C. Workup analogous to BTrz,  UV/Vis-spectroscopy. Absorption spectra were measured on a Cary 50 spectrometer, whereas emission spectra were recorded on a FluoroMax-4 (Horiba Scientific). All emission spectra were corrected for the wavelength dependent sensitivity of the detector using a set of secondary emissive standards 29 . Emission quantum yields were obtained using coumarin 30 and coumarin 153 in MeCN 30,31 , as well as rhodamine 6G in methanol as reference standards 32 .
Open aperture z-scan. An amplified Ti:sapphire laser system (Femtopower Compact Pro) was used for the open aperture z-scan measurement to determine 2PA cross sections. A detailed description of the experimental setup and the fitting equations used can be found elsewhere 33 . Rhodamine B in MeOH was used as reference to verify the reproducibility of the measurements. All investigated compounds were prepared as 10 mM solutions in spectroscopic grade THF. The solutions were measured in a 0.2 mm thick flow cell in a non-recycling volumetric flow of 4 mL/h. The excited volume is therefore refreshed approximately every 100 pulses, which approximately corresponds to 10 times for each z-position, which was found to be sufficient. The measurements were carried out at different pulse energies. At higher energies a signal of the pure solvent appears and the solvent will contribute to the effective nonlinear absorption and even thermal effects are more likely to influence the measurement. Care had to be taken to collect the whole transmitted laser energy using a large diameter and short focal length lens. Additionally, a proper Gaussian beam profile in time and space is essential for the analysis.
2PEF-cross section measurements. 2PA cross sections were also determined via two-photon excitation spectra using a set-up similar to the one described in literature by Makarov et al. 34 . In detail, the output of an optical parametric amplifier (TOPAS-Prime, Light Conversion), which is seeded by a femtosecond Ti:Sapphire regenerative amplifier (Spitfire, Spectra Physics), in combination with a frequency mixer unit (NirUVis, Light Conversion) is used as excitation source. The excitation intensity is adjusted using a combination of a broadband zero-order halfwaveplate and a Glan-Taylor polarizer, and the polarization set to vertical. The beam is slightly focused by a lens (f = 20 cm), which is placed 14 cm before the sample. The pump power is monitored using a powermeter (Thorlabs PM100A) equipped with a thermal sensor (Thorlabs S302C) behind the sample. The fluorescence is focused onto the entrance slit of a monochromator (0.25 m Cornerstone, Oriel, grating 74166 Newport) equipped with a multi-pixel photon-counter avalanche photodiode detector (Hamamatsu S-10362-11-050U) using a spherical mirror (Ø = 75 mm, f = 150 mm). The output signal is preamplified (SR240, Stanford Research Systems), processed with a gated boxcar-integrator and averager module (SR250, SRS), digitized (SR245, SRS) and recorded on a computer.
The two-photon cross-section at a given wavenumber, σ 2PA ( ν ), was calculated as follows 34 :~σ Here I x (ν , λ obs,x ) is the (two-photon-induced) fluorescence intensity at excitation wavenumber ν  and observation wavelength λ obs for either sample or reference (x ∈ {s,r}). c x and φ x ′(λ obs ) are the concentration and differential fluorescence quantum yield (at the corresponding observation wavelengths) of sample and reference.
The 2PA spectra were measured relative to rhodamine 6G in methanol and fluorescein in water at pH 11 35 . Solutions of the investigated compounds were prepared in THF with concentrations in the range from 3•10 −6 to 2•10 −5 mol/L (the maximum low energy absorption was approx. 0.5). Pump pulse energies were in the range from 1 to 3 µJ. Computational Details. Geometry optimizations were performed at the DFT/M06-2X 21 level of theory using the 6-31 + G* basis set 36 . Solvent effects were included through the conductor-like polarizable continuum model 37 using values of 7.4257 and 1.971216 for the static and optical dielectric constants, respectively. Excitation energies were computed using the ab-initio algebraic diagrammatic construction method to second order ADC(2) 22,23 . Two-photon absorption strengths were evaluated by a sum-over-states expression evaluated in the intermediate state representation [38][39][40] . Excited state solvation was included by a perturbative linear-response approach in the nonequilibrium limit 41 . All calculations were carried out employing the Q-Chem 4.3 program package 42 .
2PP structuring tests. The details of the 2PP microfabrication setup were reported previously 43 . For the present work a tunable femtosecond NIR-laser (MaiTai eHP DeepSee, Spectra-Physics) was used at various wavelengths, with a pulse duration of 70 fs after the microscope objective (32×/0.85, water immersion) used to focus the beam into the sample. The prism pulse compressor position was optimized for every wavelength to ensure a 70 fs pulse in the sample. The peak intensities for the used objective and 1 mW of laser power for a sech² shaped pulse are calculated according to Zipfel et al. 44 44 . This corresponds to approximately 571,000 voxel/s at 200 mm/s. By using a line and layer spacing of half the FWHM the throughput of the system can be estimated with 0.11 mm³/h. To facilitate high-speed structuring a combination of sample positioning via a motorized stage and a galvanometer scanner was used. The in-house developed software controls the complete setup. The structuring process was monitored in real time with a CMOS-camera mounted behind the dichroic mirror in the beam path. The samples for 2PP tests were prepared by casting about 30 µL of a liquid formulation (2PI dissolved at concentrations of 3.3 µmol 2PI/g resin (3BTrz), 5 µmol 2PI/g resin (M2CMK, 2BTrz) or 10 µmol 2PI/g resin (BTrz) in a 1:1 mixture of trimethylolpropane triacrylate (TTA, Genomer 1330) and ethoxylated-(20/3)-trimethylolpropane triacrylate (ETA, Sartomer 415), 3BTrz and M2CMK had to be pre-dissolved in acetone that was removed in vacuo before processing) onto the glass substrate of a µ-dish (35 mm diameter with glass bottom, high version, Ibidi GmbH, Martinsried, Germany) that had been functionalized with methacrylate groups by cleaning and activation with a 4:1 mixture of conc. H 2 SO 4 and H 2 O 2 (30% in water), then using 3-(trimethoxysilyl)propyl methacrylate (Sigma Aldrich) according to literature 45 . Arrays of defined woodpile test structures (lateral dimension: 30 × 30 µm, 3 µm hatch-distance, 0.5 µm layer-distance, 25 layers) were written into the monomer formulation by means of 2PP. After polymerization, the unpolymerized resin was removed by repeated soaking in Isopropanol. For time efficient visual assessment of structure quality, laser scanning microscopy (Zeiss LSM 700 and ZEN11 software for evaluation, detailed images of the structures are provided in the Supplementary information) imaging was employed, taking advantage of the autofluorescence of residual 2PIs in the polymer structures and averaging the signal from stacks of multiple scanned layers to visualize internal defects of structures that would remain hidden in electron microscopy images. The complex polyhedron model was obtained analogous to the woodpile arrays at 100 mW power and 200 mm/s writing speed, with the rinsed structure dried, sputtered with gold and images taken using a FEI Philips XL30 scanning electron microscope with EDX detection.