Open Access Article
Christoph
Staudinger
,
Johanna
Breininger
,
Ingo
Klimant
and
Sergey M.
Borisov
*
Institute of Analytical Chemistry and Food Chemistry, Graz University of Technology, Stremayrgasse 9, 8010, Graz, Austria. E-mail: sergey.borisov@tugraz.at
First published on 8th February 2019
New aza-BODIPY pH indicators with spectral properties modulated solely by photoinduced electron transfer (PET) are presented. The pH sensitive hydroxyl group is located in the meta-position of a phenyl substituent with respect to the aza-BODIPY core, which eliminates the conjugation to the chromophore. The new dyes show reversible “on”–“off” fluorescence response upon deprotonation of the receptor but no changes in the absorption spectrum, which is in contrast to state-of-the-art indicators of the aza-BODIPY family. This eliminates potential changes in the efficiency of the inner filter effect and Förster resonance energy transfer (FRET) and makes the new dyes suitable acceptors in light harvesting systems used for ratiometric pH imaging. The introduction of electron-withdrawing or electron-donating groups into the receptor results in a set of indicators suitable for measurements from physiological (pH 7) to very alkaline (pH 13) conditions. The new sensors are particularly promising for monitoring of pH changes in concrete, as was recently shown elsewhere.
Materials utilized for optical pH sensing include fluorescent indicators belonging to different chromophore classes (fluoresceins,18 rhodamines,19,20 perylenes,21,22 1,4-diketopyrrolo-pyrroles,23 HPTS,24,25 BODIPYs26–30 and aza-BODIPYs).3,29,31–35 Most of these dyes respond to pH changes in the near neutral and acidic ranges, enabling numerous applications in biology, medicine, environmental monitoring and biotechnology. In contrast, fluorescent indicators responding under alkaline conditions are comparably rare.22,36–38 Notably, sensing in the alkaline range is of primary interest in such fields as the paper industry, waste water treatment, leather processing, and metal mining and finishing, and during microbial production involving alkaliphiles.37 It is also of utmost importance for corrosion prediction and detection in steel-reinforced concrete structures, since the lifetime of these materials strongly depends on the internal pH. Whereas the pH values in concrete typically vary from 12.5 to 13.5 in the initial period, the medium becomes less alkaline with time but should stay above 10 to enable passivation of the steel components.38 Here durable and low-cost materials for pH sensing are of the highest interest.39,40
Reported fluorescent sensors for the alkaline range possess several limitations such as comparably short absorption and emission wavelengths in the case of coumarin38 and BODIPY36,37 chromophores and high hydrophobicity in the case of perylene dyes.22 Tetraaryl-aza-BODIPYs represent a particularly interesting class of fluorescent dyes showing absorption and emission in the red/NIR part of the spectrum, high molar absorption coefficients and extreme photostability.3,31 The applications of these dyes go well beyond classical sensing and imaging34,41,42 and include photothermal43 and photodynamic44 tumor therapy, photoacoustic imaging45–47 and energy conversion.48,49 With respect to optical pH sensing, aza-BODIPYs based on aromatic amines responding to pH under acidic conditions33 and those based on substituted phenols with a broader range of available pKa values31 have been reported. Importantly, deprotonation of the phenol receptor (or the amine) in the para-position with respect to the aza-BODIPY core not only results in fluorescence quenching due to acceptor-excited photoinduced electron transfer (PET)50 but also it is accompanied by a strong bathochromic shift of the absorption spectrum indicating additional intramolecular charge transfer (ICT) mechanisms.3 Although such behavior is usually not critical for most applications, it definitely results in a more complex sensor behavior. First, the pH dependent absorption of the indicators affects the magnitude of the inner filter effect which depends on the dye concentration and the thickness of the sensor foil. Second, in a multi-component system (consisting, e.g., of a pH indicator and a reference dye), both luminescence enhancement of the second component (due to lower absorption of the indicator at the excitation wavelength) and luminescence quenching (due to the inner-filter effect caused by the deprotonated form of the indicator) are possible. Third, since the absorption spectrum of the non-emissive deprotonated form of the indicator shows very good overlap with the emission spectrum of the protonated form and the concentration of the indicator in the sensor is fairly high (1–5 mM), quenching via Förster resonance energy transfer (FRET) is favored. Evidently, purely PET-based dyes make it possible to overcome the above limitations. Moreover, they would be attractive for application in light-harvesting systems for overcoming the limitation of the small Stokes shifts, typical of fluorescent dyes. For the latter, excitation at the maximum of the absorption band is virtually impossible since the excitation and emission light cannot be fully separated. In the light-harvesting system, excitation is performed at the absorption maximum of the energy donor with subsequent energy transfer to the acceptor. This allows the utilization of the high molar absorption coefficients of the donor and results in large effective Stokes shifts. The enhancement of the sensor brightness allows the production of thinner sensing layers with faster response times.
Herein we present 5 new aza-BODIPY pH indicator dyes which are decorated with a hydroxyl group in the meta-position of an aryl substituent. This receptor group is responsible for fluorescence quenching via the PET effect but neither induces the pH dependency of the absorption spectra nor negatively affects the fluorescence quantum yields. Due to electronic separation of the OH group from the electron-withdrawing core, the new dyes feature significantly higher pKa values compared to the state-of-the-art aza-BODIPY indicators and cover the pH range from ∼7 to 13. One of the indicators almost ideally matches the physiologically relevant conditions and the pH of seawater, whereas the other representatives are attractive for monitoring pH in concrete39,40,51 and studies of alkaliphilic bacteria.52
Absorption measurements were performed using a Cary 50 UV-VIS spectrophotometer from Varian, Palo Alto, USA (http://www.varianinc.com). Emission and excitation spectra were recorded on a Fluorolog® 3 Spectrofluorometer from Horiba Scientific (http://www.horiba.com) equipped with an R2658 photomultiplier tube from Hamamatsu (http://www.hamamatsu.com) or on an F-7000 fluorescence spectrophotometer from Hitachi (http://www.hitachi-hightech.com). 100-OS precision cuvettes from Hellma Analytics with a light path of 10 mm were used (http://www.hellma-analytics.com). The fluorescence quantum yields were determined relative to dibutoxy aza-BODIPY dye (Φ = 36% in chloroform).53
The pH sensing behavior of the dyes was investigated by diluting a THF stock solution (0.5 mg mL−1) with EtOH and subsequently mixing the resulting solution with a buffer in a ratio of 1
:
1. The concentration of the dyes in the final solution was ∼1.5 × 10−6 M. The pH response of the dyes physically entrapped in hydrogel D4 was investigated in glass cuvettes (1 cm path length) with the foils positioned diagonally. The cuvettes were filled with buffers and washed with water after each pH buffer change.
The pH sensors utilizing the Dual Lifetime Referencing (DLR) technique were read out using a Firesting compact phase fluorometer from Pyroscience GmbH (http://www.pyroscience.com) and the measurement set-up described previously.54 The planar foils were cut into circles and mounted on the distal end of a 1 m plastic optical fiber (Ratioplast, http://www.ratioplast.com) with the help of a home-made adaptor. The modulation frequency, LED intensity and integration time were set at 3 kHz, 80% and 16 ms, respectively. The sensors were submerged in a buffer containing 10 mM phosphate and 2 mM borate with an ionic strength of approximately 150 mM (adjusted by the addition of sodium chloride). The pH of the solution was adjusted between 5 and 12 (with steps of 0.4 pH units) by the addition of hydrochloric acid and sodium hydroxide (both 300 mM).
The imaging experiments were conducted using an AD-130GE RGB + NIR camera from JAI (http://www.jai.com). A high power yellow LED array with 12 LEDs (“12× OSRAM Oslon SSL 80 gelb Rund-Platine”) with a passive cooler and a lens array with an emission angle of 30° (all obtained from LED-Tech.de Optoelectronics (http://www.led-tech.de)) was used as the excitation source. A combination of emission filters (a foil filter (“026 bright red”) from LEE filters (http://www.leefilters.com) and an RG640 glass filter from Hoya (http://www.hoyafilter.com)) was mounted in front of the camera lens. The sensor material was glued to the bottom of a plastic Petri dish and submerged in the buffers during the measurements. The measurement times were 2000 ms and 600 ms for the RGB and NIR channels, respectively. The images were recorded with 12 bit color depth per channel.
Calibration curves and apparent pKa values were obtained by fitting the plot of fluorescence intensity vs. pH with the Boltzmann sigmoid:
![]() | (1) |
:
CH 3
:
1), the solution was partitioned between DCM and aqueous NaHCO3 solution (3 × 25 mL) and dried over sodium sulfate. The solvent was removed under reduced pressure. The crude product was purified by column chromatography (silica-gel, DCM
:
CH 3
:
1, detection by TLC with DCM
:
CH 3
:
1 and UV/VIS spectroscopy) and recrystallization from MeOH to yield red-purple crystals.
Yield: 26.1 mg (55%).
MS (MALDI): 729.3868 (calculated: 729.3557).
1H NMR (300 MHz, chloroform-d): δ = 8.04 (t, J = 7.9 Hz, 6H), 7.61 (s, 1H), 7.50 (d, J = 7.5 Hz, 1H), 7.30 (d, J = 7.8 Hz, 1H), 7.06–6.90 (m, J = 8.0 Hz, 8H), 6.86 (d, J = 7.4 Hz, 1H), 5.06 (s, 1H), 4.13–3.90 (m, 6H), 1.88–1.70 (m, 6H), 1.51 (dd, J = 14.9, 7.4 Hz, 6H), 0.99 (t, J = 7.3 Hz, 9H).
13C APT NMR (76 MHz, chloroform-d): δ = 161.83, 161.44, 160.73, 159.26, 156.72, 155.91, 145.83, 144.78, 143.58, 141.34, 134.28, 131.83, 131.54, 131.01, 129.76, 125.12, 124.23, 123.94, 121.49, 118.24, 117.44, 116.42, 116.01, 114.83, 77.16, 67.97, 31.35, 19.38, 13.98.
Yield: 25.8 mg (39%), red crystals.
MS (MALDI): 763.2911 (calculated: 763.3168).
1H NMR (300 MHz, chloroform-d): δ = 8.19–7.98 (m, J = 18.0, 8.9 Hz, 6H), 7.39–7.28 (m, J = 13.0, 6.9 Hz, 2H), 7.17–7.07 (m, 2H), 7.05–6.93 (m, 5H), 6.87 (d, J = 8.7 Hz, 2H), 5.84 (s, 1H), 4.03 (dt, J = 12.5, 6.3 Hz, 6H), 1.88–1.71 (m, J = 7.8, 5.7 Hz, 6H), 1.57–1.47 (m, J = 15.0, 7.5 Hz, 6H), 1.00 (t, J = 7.3 Hz, 9H).
13C APT NMR (76 MHz, chloroform-d): δ = 162.06, 161.42, 160.80, 160.40, 155.51, 152.15, 146.41, 144.96, 144.00, 138.75, 132.20, 131.97, 131.60, 130.85, 127.23, 125.77, 124.80, 124.27, 123.82, 121.77, 119.60, 117.60, 116.11, 114.84, 77.16, 67.96, 31.37, 19.38, 13.97.
Yield: 41.3 mg (63%), green crystals.
MS (MALDI): 671.1675 (calculated: 671.1368).
1H NMR (300 MHz, chloroform-d): δ = 8.20–7.95 (m, 6H), 7.35 (d, J = 5.7 Hz, 2H), 7.15 (s, 1H), 7.08–6.97 (m, J = 10.8, 4.0 Hz, 5H), 6.91 (d, J = 8.4 Hz, 2H), 3.89 (d, J = 3.2 Hz, 9H).
Yield: 36.9 mg (53%), purple metallic crystals.
MS (MALDI): 639.1469 (calculated: 639.1959).
1H NMR (300 MHz, chloroform-d): δ = 8.16–7.97 (m, 6H), 7.09–6.82 (m, 10H), 3.96–3.78 (m, 9H).
13C APT NMR (76 MHz, chloroform-d): δ = 162.56, 161.68, 161.44, 161.30, 155.61, 152.16, 149.69, 146.58, 146.40, 144.55, 140.68, 140.43, 132.10, 131.49, 130.89, 130.10, 124.98, 124.53, 123.97, 122.12, 118.02, 117.13, 117.01, 114.48, 114.37, 114.26, 111.47, 111.15, 77.16, 55.54.
Yield: 66.4 mg (98%), purple metallic crystals.
MS (MALDI): 645.2808 (calculated: 645.2617).
1H NMR (300 MHz, chloroform-d): δ = 8.17–8.00 (m, J = 8.6, 3.5 Hz, 6H), 7.79 (d, J = 1.8 Hz, 1H), 7.64 (dd, J = 8.4, 1.7 Hz, 1H), 7.49 (t, J = 7.3 Hz, 2H), 7.42 (d, J = 7.0 Hz, 1H), 7.07–6.87 (m, 7H), 5.64 (s, 1H), 4.05 (t, J = 6.4 Hz, 2H), 3.97 (s, 3H), 3.89 (s, 3H), 1.86–1.74 (m, J = 14.5, 6.6 Hz, 2H), 1.56 (s, 2H), 0.99 (t, J = 7.3 Hz, 3H).
![]() | ||
| Fig. 1 Synthetic route to the new aza-BODIPY dyes. Intermediates with indices belong to the respective dye. | ||
000 L mol−1 cm−1, a typical value for this dye class. The fluorescence quantum yield is about 25%, except for indicator 5 whose Φ is ∼2-fold lower. Fluorescence decay times show the same trend with values of ∼2.6 ns for indicators 1–4 and only ∼1.5 ns for indicator 5. The most important structural difference between indicators 1–4 and indicator 5 is the methoxy group in the o-position to the hydroxyl group. This provides the possibility of hydrogen bonding between these two groups and might cause a reduction in quantum yield and fluorescence lifetime. The brightness of the dyes is therefore significantly higher than that of the previously reported purely PET-based aza-BODIPY dye with a meta-hydroxyl group in the “lower” phenyl ring (Φ of 10%).3
![]() | ||
| Fig. 2 pH dependence of absorption (solid lines) and emission spectra (dashed lines) of indicator 3 (a) and the state-of-the-art hydroxy-aza-BODIPY pH indicator31 (c) in hydrogel D4; (b) and (d) show the pH equilibria for the respective dyes. | ||
| Compound | λ abs, nm | λ em, nm | ε, M−1 cm−1 | Φ, % | τ, ns | pK′a b |
pK′a c |
|---|---|---|---|---|---|---|---|
| a Protonated form of the dyes. b Determined in solution in EtOH/H2O (1/1). c Determined in a Hydromed D4 sensor foil in a concentration of 0.2 w%. d Dye solubility is insufficient for the titration. | |||||||
| 1 | 696 | 720 | 83 200 |
24 | 2.54 | n.d.d | 11.7 |
| 2 | 696 | 721 | 85 400 |
27 | 2.69 | 11.1 | 10.8 |
| 3 | 695 | 721 | 80 700 |
26 | 2.56 | 7.8 | 7.5 |
| 4 | 694 | 720 | 73 300 |
27 | 2.67 | 10.3 | 10.3 |
| 5 | 698 | 722 | 90 000 |
14 | 1.57 | n.d.d | 11.6 |
The fluorescence response of the new dyes to pH is typical of the “on”–“off” indicators (Fig. S2 of the ESI,†Fig. 3b). Generally, the pKa values (Table 1) are significantly higher than those for the state-of-the-art aza-BODIPY dyes with conjugated phenol and the same substitution character. The relatively high pKa values of the new dyes can be explained by the electronic decoupling of the hydroxyl group from the electron withdrawing core of the dye. Interestingly, the apparent pKa for dye 1 is even higher than that for phenol (pKa = 9.99).57 This may be explained by the fairly hydrophobic character of the chromophore creating a microenvironment where the more polar anionic form is less stabilized than the uncharged form. Indicator 2, which is decorated with a single chlorine atom in the ortho-position towards the hydroxyl group, features only a slightly lower pKa value (Table 1). Two fluorine atoms located in the ortho and para-positions towards the hydroxyl group further decrease the pKa value by about 1 unit. As can be seen, the effect of two chlorine atoms in the ortho-position towards the hydroxyl group (indicator 3) is much stronger (pKa = 7.8), making this indicator promising for measurements under physiological conditions in marine environment due to pKa almost ideally matching the pH of seawater. On the other hand, indicators 1, 2, 4 and 5 are expected to be promising for imaging of pH on concrete surfaces51 and the investigation of alkaliphilic bacteria.52 In fact, we recently demonstrated high potential of the new sensors for monitoring the pH dynamics in concrete.39,40 The dyes can also be used as essential components for the preparation of broad range pH sensors (usually obtained by mixing multiple pH indicators).31 Notably, only a few aza-BODIPY indicators have been reported with similarly high pKa values and they require higher synthetic effort31 or are no longer fluorescent and can only be used as absorption based indicators.58
![]() | ||
| Fig. 3 Structures with apparent pKa values (a) and titration curves (b) of the new aza-BODIPY indicators immobilized in polyurethane hydrogel D4. | ||
Table 2 compares the properties of fluorescent pH indicators used in sensors for measurements in highly alkaline media. As can be seen, only BODIPYs28 and aza-BODIPYs (this work) have so far allowed for the fine-tuning of the pKa value and the dynamic range of the sensors. Compared to the former, the new dyes show about 150 nm bathochromically shifted absorption and emission spectra, which is beneficial for application in environments with high autofluorescence and scattering but also for in vivo measurements.
| Dye-class | Matrix | λ max abs/exc, nm | λ max em, nm | pK′a | Comment | Ref. |
|---|---|---|---|---|---|---|
| Coumarin | Cross-linked 1,4-bis(acryloyl)piperazine | 370 | 470 | 11.9 | Short wavelength absorption and emission | 38 |
| BODIPY | Polyurethane hydrogel D4 | 523 | 532 | 11.44 | Comparably short wavelength of absorption and emission | 37 |
| BODIPY | Polymeric hydrogel | 502 | 508 | 10.8 | Comparably short wavelength of absorption and emission | 36 |
| BODIPY | Polyurethane hydrogel D4 | 522–540 | 537–550 | 0.5–12.83 | Comparably short wavelength of absorption and emission | 28 |
| Perylene | Polyurethane hydrogel D4 | 586 | 595 | 10.56 | Extremely limited tuneability of the pKa | 22 |
| Perylene | Polyurethane hydrogel D4 | 650 | 662 | 10.15 | Extremely limited tuneability of the pKa | 22 |
| Aza-BODIPYs | Polyurethane hydrogel D4 | 694–698 | 720–722 | 7.5–11.7 | Tuneable pKa, NIR absorption and emission, high photostability; excellent spectral compatibility with robust reference materials | This work |
In order to overcome the limitations of fluorescence intensity measurement, we prepared pH sensor materials which rely on the Dual Lifetime Referencing (DLR) technique. This method relies on the use of a second emitter with a much longer luminescence decay time (micro- or millisecond time domain). It enables a robust read-out independent of the intensity of the excitation light and sensitivity of the photodetector and compensates for some variation in the thickness of the sensor foil. Similar to the previously reported aza-BODIPY indicators, the new dyes are spectrally compatible with the robust inorganic emitters Egyptian Blue55 and Cr-GAB.59 In fact, the sensors prepared on the basis of dyes 3 and 4 and Egyptian blue as a reference material were excellently suitable for robust referenced read-out with a compact phase fluorometer (Fig. S3 of the ESI†). The resolution of these sensors estimated from the standard deviation of the measured phase angle (∼0.11°) was 0.003 pH units when measured close to the apparent pKa of the sensors. Clearly, this referencing scheme can also be applied for the other dyes of the series.
State-of-the-art para-substituted-hydroxy aza-BODIPY indicators are not ideal for this concept as the efficiency of energy transfer depends on the overlap of the absorption and emission spectra of the donor and the acceptor, respectively. A strong bathochromic shift in the absorption of the acceptor upon deprotonation (see Fig. 2a) results in reduced FRET efficiency and a “turn on” effect of the donor, which reduces the dynamics of the sensor.
Fig. 4a depicts the composition of the light harvesting system which relies on the pH-insensitive tetraphenyl aza-BODIPY as an energy donor and indicator 3 as an acceptor. Importantly, the absorption spectrum of 3 is bathochromically shifted by approximately 40 nm due to the electron donating ether groups (see Fig. S4 of the ESI†), thus ensuring excellent spectral overlap between the emission of the donor and the absorption of the acceptor. The protonated indicator can indeed be efficiently excited via energy transfer from the donor (Fig. 4b). The corresponding emission spectra (Fig. 4c) of the materials clearly show that the light harvesting concept leads to a strong signal enhancement (∼3.4 fold) of the fluorescence of the pH indicator. The energy transfer is very efficient since only a small amount of residual donor fluorescence is visible. In basic media (Fig. 4d and e), the fluorescence emission of the acceptor is completely quenched. In contrast, the residual fluorescence of the donor remains constant (Fig. 4e, peak at 690 nm). Furthermore, no “turn on” of donor emission is visible upon deprotonation of the indicator. Therefore, even a simple long-pass emission filter (e.g. at 700 nm) makes it possible to collect almost the entire fluorescence from the indicator. The strong signal enhancement can either be used to prepare thinner and faster responding sensor films or to obtain sensors with better signal-to-noise ratios. Additionally, the residual fluorescence from the donor is also very useful for referencing purposes.
![]() | ||
| Fig. 4 Enhancement of the fluorescence properties of the pH sensor via light harvesting. Chemical structures of the employed donor (tetraphenyl aza-BODIPY) and acceptor (indicator 3) (a). Excitation (b, d) and emission (c, e) spectra at pH 5 (b, c) and pH 10 (d, e) for the sensor material employing light harvesting (green) and for the corresponding sensor materials containing only the donor (red) and only the acceptor (blue). The concentrations of the dyes are given in wt% with respect to the polymer. The spectra were recorded with sensor foils of approximately 3 μm sensor layer thickness in the right angle mode. The emission intensities are normalized to the emission intensity of the pure donor for every plot. The absorption spectra of the sensor foil are depicted in Fig. S1 in the ESI.† | ||
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c9an00118b |
| This journal is © The Royal Society of Chemistry 2019 |