Zinc Donor–Acceptor Schiff Base Complexes as Thermally Activated Delayed Fluorescence Emitters

: Four new zinc(II) Schiff base complexes with carbazole electron donor units and either a 2,3-pyrazinedicarbonitrile or a phthalonitrile acceptor unit were synthesized. The donor units are equipped with two bulky 2-ethylhexyl alkyl chains to increase the solubility of the complexes in organic solvents. Furthermore, the effect of an additional phenyl linker between donor and acceptor unit on the photophysical properties was investigated. Apart from prompt ﬂuorescence, the Schiff base complexes show thermally activated delayed ﬂuorescence (TADF) with quantum yields up to 47%. The dyes bearing a phthalonitrile acceptor emit in the green–yellow part of the electromagnetic spectrum and those with the stronger 2,3-pyrazinedicarbonitrile acceptor—in the orange–red part of the spectrum. The emission quantum yields decrease upon substitution of phthalonitrile with 2,3-pyrazinedicarbonitrile and upon introduction of the phenyl spacer. The TADF decay times vary between 130 µ s and 3.5 ms at ambient temperature. The weaker phthalonitrile acceptor and the additional phenyl linker favor longer TADF decay times. All the complexes show highly temperature-dependent TADF decay time (temperature coefﬁcients above − 3%/K at ambient conditions) which makes them potentially suitable for application as molecular thermometers. Immobilized into cell-penetrating RL-100 nanoparticles, the best representative shows temperature coefﬁcients of − 5.4%/K at 25 ◦ C that makes the material interesting for further application in intracellular imaging.


Introduction
Temperature is one of the key parameters in daily life, industry and scientific research, and is quantified with temperature sensors.Commonly used temperature sensors can be divided into several groups, depending on which temperature-dependent physical parameter is measured: volume in a liquid-filled glass thermometer, electrical resistance in a resistance thermometer or voltage in case of a thermocouple, to mention the most common types.Despite being highly useful, these readily available sensors are not suitable for a number of important applications.Particularly, they cannot be used for measurements in very small objects such as (microfluidic) chips and living cells because their spatial resolution is limited to around 10 µm [1].Luminescent temperature probes [1][2][3][4][5] not only overcome the above limitation, but also allow 2D and 3D mapping of temperature distribution via imaging techniques.
Purely organic dyes and metal complexes that emit thermally activated delayed fluorescence (TADF) have been extensively investigated in the last decade in context of application in OLED technology [27,28].Although optical temperature sensing with the help of TADF emitters was demonstrated a while ago [29,30], only recently have molecular thermometers on their basis attracted significant attention.Sensors utilizing TADF-emitting carbon dotbased nanocomposite [31], polymers based on 1,8-naphthalimide [32], anthraquinone and dicyanobenzene -derived [33] organic dyes, as well as Pt(II), Pd(II) and Zn(II) complexes with benzoporphyrins [34,35] have been reported.
Previously, we presented a new group of TADF emitters based on Zn(II) complexes with Schiff bases [36].These dyes rely on an abundant metal and, in this respect, are comparable to metal-free TADF emitters.On the other hand, they feature particularly high molar absorption coefficients in the visible part of electromagnetic spectrum (39,000-75,000 M −1 cm −1 ) and are also characterized by high temperature sensitivity of the TADF decay time at ambient temperature (~−3.5%/K for polymer-immobilized dyes).Among the two dyes investigated, the one with the carbazole electron donor featured a significantly higher ratio of TADF to prompt fluorescence and several-fold-shorter decay times compared to the analogue utilizing the dialkylaniline donor group, but, unfortunately, it also possessed poor solubility in organic solvents.Thus, it is of considerable interest to investigate a broader palette of the new emitters and improve the solubility of the dyes in organic solvents and polymers to minimize potential aggregation issues.
In this work, we present four Zn(II) Schiff base complexes that include a combination of a carbazole donor with two different acceptor units and optionally include a phenyl linker (Figure 1).It will be shown that the nature of the acceptor unit and presence of the linker strongly influence the photophysical properties of the dyes, whereas the temperature sensing characteristics are barely affected by the modifications.
Chemosensors 2022, 10, x FOR PEER REVIEW 2 of 16 Purely organic dyes and metal complexes that emit thermally activated delayed fluorescence (TADF) have been extensively investigated in the last decade in context of application in OLED technology [27,28].Although optical temperature sensing with the help of TADF emitters was demonstrated a while ago [29,30], only recently have molecular thermometers on their basis attracted significant attention.Sensors utilizing TADF-emitting carbon dot-based nanocomposite [31], polymers based on 1,8-naphthalimide [32], anthraquinone and dicyanobenzene -derived [33] organic dyes, as well as Pt(II), Pd(II) and Zn(II) complexes with benzoporphyrins [34,35] have been reported.
Previously, we presented a new group of TADF emitters based on Zn(II) complexes with Schiff bases [36].These dyes rely on an abundant metal and, in this respect, are comparable to metal-free TADF emitters.On the other hand, they feature particularly high molar absorption coefficients in the visible part of electromagnetic spectrum (39,000-75,000 M −1 cm −1 ) and are also characterized by high temperature sensitivity of the TADF decay time at ambient temperature ( −3.5%/K for polymer-immobilized dyes).Among the two dyes investigated, the one with the carbazole electron donor featured a significantly higher ratio of TADF to prompt fluorescence and several-fold-shorter decay times compared to the analogue utilizing the dialkylaniline donor group, but, unfortunately, it also possessed poor solubility in organic solvents.Thus, it is of considerable interest to investigate a broader palette of the new emitters and improve the solubility of the dyes in organic solvents and polymers to minimize potential aggregation issues.
In this work, we present four Zn(II) Schiff base complexes that include a combination of a carbazole donor with two different acceptor units and optionally include a phenyl linker (Figure 1).It will be shown that the nature of the acceptor unit and presence of the linker strongly influence the photophysical properties of the dyes, whereas the temperature sensing characteristics are barely affected by the modifications.

Measurements
1 H and 13 C-APT NMR spectra of the intermediates were recorded on a 300 MHz spectrometer and the 1 H and 13 C spectra NMR spectra of the Zn(II) Schiff base complexes on a 500 MHz instrument from Bruker (www.bruker.com(24 February 2022)) (Figures S7-S24).The residual signal of the deuterated solvent was used as an internal standard.High-resolution mass spectra of the Zn(II) Schiff bases (Figures S30-S33) were recorded on the matrix-assisted laser desorption/ionization time-of-flight mass spectrometer (MALDI-TOF MS) Micromass MALDI micro MX from Waters (www.waters.com(24 February 2022)).Mass spectra for reaction monitoring and characterization of intermediates (Figures S25-S29) were acquired on an Expression CMS L compact mass spectrometer from Advion (www.advion.com(24 February 2022)) with an APCI (atmospheric-pressure chemical ionization) source and quadrupole mass analyzer (range 10-2000 m/z).
Spectral properties were measured in precision cuvettes from Hellma Analytics (www.hellma-analytics.com(24 February 2022)).UV-Vis spectra were recorded on a CARY 50 UV-Vis spectrophotometer from Varian (www.agilent.com(24 February 2022)) in 10 mm cuvettes made of optical glass.Luminescence spectra were recorded on a Fluorolog-3 luminescence spectrometer (www.horiba.com(24 February 2022)) equipped with a NIRsensitive R2658 photomultiplier from Hamamatsu.The measurements were performed in a quartz cuvette equipped with an 80 mm long tube (10 mm pass-length, Type 221).Deoxygenation of toluene solutions was performed by bubbling high-purity nitrogen (99.99999% purity) from Linde Gas (www.linde-gas.com(24 February 2022)) through the solution for at least 20 min.In order to record the spectra of dyes in PS, the foils were placed diagonally in a quartz glass precision cuvette (10 mm) filled with a 5 w% aqueous Na 2 SO 3 solution that additionally contained a catalytic amount of CoCl 2 .
Luminescence decay times were measured using a spectraLED (λ = 456 nm) excitation source from Horiba on Fluorolog-3 spectrometer equipped with a DeltaHub module (Horiba).Data analysis was performed on DAS-6 Analysis software from Horiba using a mono-, bi-or tri-exponential fit.Average decay times (τ) of bi-and tri-exponential decays were calculated from the individual lifetimes (τ x ) and their amplitudes (B x ) according to: Absolute quantum yields of prompt fluorescence (Φ prompt ) in toluene and PS were measured under aerated conditions on a Fluorolog-3 spectrometer equipped with an integrating sphere Quanta-phi.Absolute quantum yields of delayed fluorescence (Φ DF ) were calculated according to: where A deoxy and A air are the areas under the emission spectra acquired under deoxygenated and air-saturated conditions, respectively.It was assumed that due to the long decay times, the TADF emission is almost completely quenched at air-saturated conditions.Examples of the spectra under deoxygenated and air-saturated conditions measured in toluene and PS can be found in Supporting Information (Figures S1-S3).
Temperature was adjusted by using a Cary SPV-1X0 Single Cell Peltier Accessory Peltier element from Varian in combination with a F12-ED refrigerated/heating circulator from Julabo (www.julabo.com(24 February 2022)).
Temperature calibration curves were fitted via an Arrhenius type model [37]: where k 0 is the temperature-independent decay rate for the excited-state deactivation, k 1 is a pre-exponential factor, k B is the Boltzmann constant, ∆E is the energy gap between the first singlet and first triplet state, and T is the absolute temperature.

Preparation of Dye-Polymer Films
Dye (1 wt% in respect to the polymer) and polystyrene (10 wt% in respect to the solvent) were dissolved in chloroform to obtain a "cocktail".The "cocktails" were knifecoated on a dust-free PET support with a wet film thickness of 25 µm and dried for half an hour at room temperature.In case of polymer films, incorporating dye-adduct with pyridine, pyridine (100-fold excess compared to the mass of the dye) was added to the "cocktail" and the foils were dried one day in a drying chamber at 70 • C.

Fiber-Optic Setup
A sensor spot was stamped out of a dye/PS PET foil (1 wt% dye) and fixed with a metal cap on a 1 mm optical fiber.The fiber was connected to a custom version of Firesting phase fluorometer from PyroScience (www.pyroscience.com(24 February 2022)) that was equipped with a blue LED for the excitation.The tip of the fiber was held in a doublewalled glass bottle filled with an aqueous 5 w% Na 2 SO 3 solution.The temperature was adjusted by a Julabo F25-ME refrigerated/heating circulator and measured by an external PT-100 resistance thermometer.

Water-Dispersible Nanoparticles
A "cocktail" was prepared by dissolving dye (0.5 wt% with respect to the polymer) and RL-100 (0.2 wt% with respect to the solvent) in acetone/THF (9+1 v/v) and addition of pyridine (100-fold excess compared to the mass of the dye).Water (3 times the volume of the "cocktail") was quickly added to the "cocktail" under vigorous stirring and the organic solvents were removed under reduced pressure.Residues of pyridine were removed by dialysis.
For temperature calibration, 2 mL of particle dispersion (~0.4 mg/mL) were added to 1 mL PBS puffer (10 mM, pH = 7.4) in a cuvette.The dispersion was deoxygenated by addition of 30 mg glucose monohydrate and traces of glucose oxidase.

Synthesis
The Zn(II) Schiff base complexes consist of a carbazole donor moiety and either a 2,3-pyrazinedicarbonitrile or a phthalonitrile acceptor moiety.The carbazole units bear two 2-ethylhexyl chains which significantly increase the solubility of the complexes compared to the previously reported t-butyl substituted derivative [36].The alkyl-substituted carbazole 1 is conveniently prepared in two steps from commercially available 9H-carbazole following a literature method [38].Starting from compound 1, the carbazole-substituted hydroxybenzaldehyde precursor 6 and its phenyl extended analogue 4 are synthesized in two and four steps, respectively (Figure 2a).In a last step, the Zn(II) Schiff base complexes are formed in a one-pot procedure [40][41][42] from the corresponding diamine, zinc acetate dihydrate and the precursors 4 or 6 (Figure 2b).
The Zn(II) Schiff base complexes consist of a carbazole donor moiety and either a 2,3pyrazinedicarbonitrile or a phthalonitrile acceptor moiety.The carbazole units bear two 2-ethylhexyl chains which significantly increase the solubility of the complexes compared to the previously reported t-butyl substituted derivative [36].The alkyl-substituted carbazole 1 is conveniently prepared in two steps from commercially available 9H-carbazole following a literature method [38].Starting from compound 1, the carbazole-substituted hydroxybenzaldehyde precursor 6 and its phenyl extended analogue 4 are synthesized in two and four steps, respectively (Figure 2a).In a last step, the Zn(II) Schiff base complexes are formed in a one-pot procedure [40][41][42] from the corresponding diamine, zinc acetate dihydrate and the precursors 4 or 6 (Figure 2b).

Photophysical Properties
Figure 3 shows absorption and emission spectra of the four complexes in toluene.The complexes bearing the phthalonitrile acceptor (ZnPH-Cz and ZnPH-Ph-Cz) absorb in the blue part and emit in the green-yellow of the electromagnetic spectrum (Figure 3a).The absorption and emission spectra of ZnPH-Cz are almost identical to those of Zn-2 [36], which bears tert-butyl groups instead of 2-ethylhexyl substituents (Table 1).A pronounced bathochromic shift of absorption and emission spectra is observed upon substitution of phthalonitrile with 2,3-pyrazinedicarbonitrile (Figure 3b), which is a significantly stronger electron acceptor than phthalonitrile [43].These dyes (ZnPZ-Cz and ZnPZ-Ph-Cz) show the absorption maxima in the green part of the spectrum and emit red light.The molar absorption coefficients are slightly higher for the dyes with 2,3-pyrazinedicarbonitrile acceptor compared to the corresponding compounds based on phthalonitrile (Table 1).Introduction of phenyl spacer decreases molar absorption coefficients

Photophysical Properties
Figure 3 shows absorption and emission spectra of the four complexes in toluene.The complexes bearing the phthalonitrile acceptor (ZnPH-Cz and ZnPH-Ph-Cz) absorb in the blue part and emit in the green-yellow of the electromagnetic spectrum (Figure 3a).The absorption and emission spectra of ZnPH-Cz are almost identical to those of Zn-2 [36], which bears tert-butyl groups instead of 2-ethylhexyl substituents (Table 1).A pronounced bathochromic shift of absorption and emission spectra is observed upon substitution of phthalonitrile with 2,3-pyrazinedicarbonitrile (Figure 3b), which is a significantly stronger electron acceptor than phthalonitrile [43].These dyes (ZnPZ-Cz and ZnPZ-Ph-Cz) show the absorption maxima in the green part of the spectrum and emit red light.The molar absorption coefficients are slightly higher for the dyes with 2,3-pyrazinedicarbonitrile acceptor compared to the corresponding compounds based on phthalonitrile (Table 1).Introduction of phenyl spacer decreases molar absorption coefficients by ~30%.Notably, in both systems, the UV absorption of the dyes with linker is strongly enhanced.
phenyl linker show slightly broader emission spectra.This effect can be explained by more restricted rotation between the donor and acceptor units in case of the dyes bearing no spacer which favors sharper emission bands [43].Unfortunately, substitution of phthalonitrile with 2,3-pyrazinedicarbonitrile also results in significant decrease of the luminescence quantum yields, both for prompt fluorescence and TADF (Table 1).The effect is milder in case of the phthalonitrile acceptor (ZnPH-Ph-Cz), but is much more pronounced for the dye bearing 2,3-pyrazinedicarbonitrile ZnPZ-Ph-Cz that shows poor prompt and delayed fluorescence in solution (Table 1).The TADF decay times, measured in anoxic toluene, vary between 144 µ s and 1040 µ s (Table 1) and are non-monoexponential, with the exception of ZnPH-Cz (Figure S4).The shortest decay times were obtained for ZnPZ-Cz and ZnPZ-Ph-Cz, which bear the stronger 2,3-pyrazinedicarbonitrile acceptor (Table 1).As can be seen, the TADF decay   The emission spectra of the dyes with 2,3-pyrazinedicarbonitrile acceptor (ZnPZ-Cz and ZnPZ-Ph-Cz) are significantly broader (FWHM of 2860 and 3870 cm −1 , respectively) than for the corresponding dyes bearing phthalonitrile acceptor (FWHM of 2380 and 2830 cm −1 for ZnPH-Cz and ZnPH-Ph-Cz, respectively).It is also evident that the dyes with phenyl linker show slightly broader emission spectra.This effect can be explained by more restricted rotation between the donor and acceptor units in case of the dyes bearing no spacer which favors sharper emission bands [43].Unfortunately, substitution of phthalonitrile with 2,3-pyrazinedicarbonitrile also results in significant decrease of the luminescence quantum yields, both for prompt fluorescence and TADF (Table 1).The effect is milder in case of the phthalonitrile acceptor (ZnPH-Ph-Cz), but is much more pronounced for the dye bearing 2,3-pyrazinedicarbonitrile ZnPZ-Ph-Cz that shows poor prompt and delayed fluorescence in solution (Table 1).
The TADF decay times, measured in anoxic toluene, vary between 144 µs and 1040 µs (Table 1) and are non-monoexponential, with the exception of ZnPH-Cz (Figure S4).The shortest decay times were obtained for ZnPZ-Cz and ZnPZ-Ph-Cz, which bear the stronger 2,3-pyrazinedicarbonitrile acceptor (Table 1).As can be seen, the TADF decay times are increased upon introduction of phenyl linker.The observed effects may be explained by an increased energy gap between first singlet and triplet state (∆E ST ) upon introduction of the linker [43].Particularly, the energy of the singlet state is increased due to less efficient separation between HOMO (usually located on the donor unit) and LUMO (usually located on the acceptor unit), and the triplet state is reduced in energy by conjugation extending effects [43].

Properties of Immobilized Dyes
Polystyrene was used as a model matrix for evaluation of the photophysical properties of the new dyes in a rigid environment since immobilization of dyes is essential for many applications, varying from sensors to OLEDs.Photophysical properties of the immobilized emitters are summarized in Table 2.All four emitter-polymer materials were characterized as with and without additional pyridine.The pyridine coordinates on the free axial positions of the zinc metal center and is supposed to prevent the emitters from aggregation.Immobilization only slightly affects the absorption and emission spectra.However, both the TADF decay times and the quantum yields are strongly affected by immobilization.The TADF decays of all four complexes (with and without pyridine) are nonmonoexponential (Figure S4).For immobilized ZnPH-Cz and ZnPZ-Cz, the decay times are comparable to those obtained in toluene solution.On the other hand, the dyes with phenyl spacer (ZnPH-Ph-Cz and ZnPZ-Ph-Cz) show 3-4-fold increase of the decay times upon immobilization.This is a drawback with respect to potential applications as molecular thermometers since the longer decay times favor higher cross-sensitivity of the materials to molecular oxygen.Interestingly, coordination of pyridine results in decrease of TADF decay times in case of phthalonitrile-based emitters ZnPH-Cz/Py and ZnPH-Ph-Cz/Py, whereas the opposite effect is observed for the 2,3-pyrazinedicarbonitrile-based emitters ZnPZ-Cz/Py and ZnPZ-Ph-Cz/Py.
Without additional pyridine, only ZnPH-Cz shows acceptable quantum yields of the delayed fluorescence, whereas for other dyes, TADF efficiency is moderate to poor.In contrast, all emitters with coordinated pyridine show an increase in both prompt and TADF quantum yields (up to 47% for ZnPH-Cz/Py).For ZnPH-Cz/Py and ZnPH-Ph-Cz/Py the TADF is by far more efficient than prompt fluorescence emission.The pyridine-coordinated emitter ZnPH-Cz/Py, apart from good solubility, shows excellent photophysical properties in rigid matrix that makes it the most promising candidate for practical applications.
Figure 4 exemplifies the effect of temperature of the TADF decay time for ZnPH-Cz and ZnPH-Cz/Py in polystyrene matrix.The dependencies for the other complexes can be found in Supporting Information (Figures S5 and S6).Evidently, the TADF decay times strongly decrease with temperature which is the prerequisite for the application of the emitters as molecular thermometers with self-referenced decay time read-out.Interestingly, structural modifications have almost no effect on the temperature sensitivity.In fact, the temperature coefficients for all the dyes including previously reported Zn-2 vary in a very narrow range (from −3.2 to −3.7%/K at 25 • C, Table 2).Such temperature coefficients are very high and exceed those for most of the reported molecular thermometers and thermographic phosphors [36].
strongly decrease with temperature which is the prerequisite for the application of the emitters as molecular thermometers with self-referenced decay time read-out.Interestingly, structural modifications have almost no effect on the temperature sensitivity.In fact, the temperature coefficients for all the dyes including previously reported Zn-2 vary in a very narrow range (from −3.2 to −3.7%/K at 25 °C, Table 2).Such temperature coefficients are very high and exceed those for most of the reported molecular thermometers and thermographic phosphors [36].

Polymer-Based Sensor Materials
In order to evaluate potential applicability of the dyes, the most promising candidate ZnPH-Cz/Py was evaluated in two different sensor formats: a fiber-optic sensor and nanoparticles.In the first format, the dye was embedded in a polystyrene layer coated on a transparent polyethylene terephthalate support.The sensor foil was fixed on the tip of an optical fiber and readout was performed with a custom version (excitation with a blue LED excitation source) of a commercially available phase fluorometer (Firesting, PyroScience).Figure 5 shows the measured phase shift of three temperature cycles between 20 °C and 50 °C acquired in anoxic solutions.The sensor shows reproducible performance and good resolution, but also demonstrates an important limitation of the frequency-domain read-out: due to significant contribution of prompt fluorescence (30%, Table 2), the measured phase angle is significantly lower than, e.g., for phosphorescent dyes with the same excited state decay time.Clearly, the most serious limitation of the sensor is that it operates in the anoxic environment but different approaches (e.g., using oxygen scavengers [36]) may be feasible to overcome this problem.

Polymer-Based Sensor Materials
In order to evaluate potential applicability of the dyes, the most promising candidate ZnPH-Cz/Py was evaluated in two different sensor formats: a fiber-optic sensor and nanoparticles.In the first format, the dye was embedded in a polystyrene layer coated on a transparent polyethylene terephthalate support.The sensor foil was fixed on the tip of an optical fiber and readout was performed with a custom version (excitation with a blue LED excitation source) of a commercially available phase fluorometer (Firesting, PyroScience).Figure 5 shows the measured phase shift of three temperature cycles between 20 • C and 50 • C acquired in anoxic solutions.The sensor shows reproducible performance and good resolution, but also demonstrates an important limitation of the frequency-domain read-out: due to significant contribution of prompt fluorescence (~30%, Table 2), the measured phase angle is significantly lower than, e.g., for phosphorescent dyes with the same excited state decay time.Clearly, the most serious limitation of the sensor is that it operates in the anoxic environment but different approaches (e.g., using oxygen scavengers [36]) may be feasible to overcome this problem.
Nanoparticles for potential application in intracellular measurements have also been prepared.ZnPH-Cz/Py was embedded in commercially available Eudragit RL-100 polymer.RL-100 nanoparticles bear positively charged quaternary ammonium groups on their surface, have an average size of ~30 nm, and efficiently stain a variety of cells that enable intracellular measurements [44].They are usually prepared by a common precipitation technique [45].In short, the dye and the polymer are dissolved in a water miscible organic solvent (usually acetone), followed by addition of water under vigorous stirring and removal of the organic solvent under reduced pressure.
For characterization, the oxygen from the aqueous particle dispersion was removed by glucose and glucose oxidase.PBS buffer was added to avoid potential degradation of ZnPH-Cz/Py in acidic environment that would otherwise be generated by formation of gluconic acid during the enzymatic reaction.Anoxic puffer systems that are known from super-resolution microscopy [46] can be used if the material is further applied for intracellular temperature measurements.
Excitation and emission spectra (Figure 6a) indicate a slight hypsochromic shift compared to polystyrene.Remarkably, the TADF decay times in the nanoparticles increase by about 2-fold (25 • C) compared to polystyrene (Figure 6b).Favorably for optical temperature measurement, the temperature sensitivity is also further enhanced to −5.4%/K at 25 • C. A possible explanation for the longer TADF decay times and higher sensitivity could be the more hydrophilic environment which affects the donor and acceptor orientation, as well as the charge distribution of the dye.effect may be further explored in future to prepare more sensitive bulk optodes and fiber-optic sensors on the basis of the nanoparticles.Nanoparticles for potential application in intracellular measurements have also been prepared.ZnPH-Cz/Py was embedded in commercially available Eudragit RL-100 polymer.RL-100 nanoparticles bear positively charged quaternary ammonium groups on their surface, have an average size of ~30 nm, and efficiently stain a variety of cells that enable intracellular measurements [44].They are usually prepared by a common precipitation technique [45].In short, the dye and the polymer are dissolved in a water miscible organic solvent (usually acetone), followed by addition of water under vigorous stirring and removal of the organic solvent under reduced pressure.
For characterization, the oxygen from the aqueous particle dispersion was removed by glucose and glucose oxidase.PBS buffer was added to avoid potential degradation of ZnPH-Cz/Py in acidic environment that would otherwise be generated by formation of gluconic acid during the enzymatic reaction.Anoxic puffer systems that are known from super-resolution microscopy [46] can be used if the material is further applied for intracellular temperature measurements.
Excitation and emission spectra (Figure 6a) indicate a slight hypsochromic shift compared to polystyrene.Remarkably, the TADF decay times in the nanoparticles increase by about 2-fold (25 °C) compared to polystyrene (Figure 6b).Favorably for optical temperature measurement, the temperature sensitivity is also further enhanced to −5.4 %/K at 25 °C.A possible explanation for the longer TADF decay times and higher sensitivity could be the more hydrophilic environment which affects the donor and acceptor orientation, as well as the charge distribution of the dye.This effect may be further explored in future to prepare more sensitive bulk optodes and fiber-optic sensors on the basis of the nanoparticles.

Conclusions
In conclusion, four new Zn(II) Schiff base complexes combining a carbazole based electron donor and two different electron acceptors and optionally an additional phenyl linker were prepared.The absorption and emission spectra show significant bathochromic

Figure 2 .
Figure 2. Synthesis of the dye precursors (a) and the Zn(II) Schiff base complexes (b).

Figure 2 .
Figure 2. Synthesis of the dye precursors (a) and the Zn(II) Schiff base complexes (b).

Figure 4 .
Figure 4. Temperature dependency of TADF decay times for ZnPH-Cz (a) and for ZnPH-Cz/Py (b) immobilized in PS matrix acquired in deoxygenized solution.In each temperature calibration cycle, three decay time measurements were made at each temperature.The calibration cycle was repeated three times.

Figure 4 .
Figure 4. Temperature dependency of TADF decay times for ZnPH-Cz (a) and for ZnPH-Cz/Py (b) immobilized in PS matrix acquired in deoxygenized solution.In each temperature calibration cycle, three decay time measurements were made at each temperature.The calibration cycle was repeated three times.

Figure 6 .
Figure 6.Excitation (solid lines) and emission (dashed lines) spectra (a) and temperature dependency of TADF decay times (b) for ZnPH-Cz/Py immobilized in RL-100 nanoparticles acquired under anoxic conditions.For the temperature dependency measurements, two calibration cycles were performed.In each cycle, three decay time measurements were made at each temperature.The inset shows a photographic image of the particle dispersion (0.4 mg/mL) under UV irradiation.

Figure 6 .
Figure 6.Excitation (solid lines) and emission (dashed lines) spectra (a) and temperature dependency of TADF decay times (b) for ZnPH-Cz/Py immobilized in RL-100 nanoparticles acquired under anoxic conditions.For the temperature dependency measurements, two calibration cycles were performed.In each cycle, three decay time measurements were made at each temperature.The inset shows a photographic image of the particle dispersion (0.4 mg/mL) under UV irradiation.

Table 1 .
Photophysical properties of Zn(II) Schiff base complexes in toluene at 25 °C.

Table 2 .
Photophysical properties of Zn(II) Schiff base complexes with and without pyridine in rigid polystyrene matrix at 25 • C.