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BODIPY-coelenterazine conjugates as self-illuminating substrates for NanoLuc

Valeska Viereckt a, Frank Abendroth a, Alexander Schauerte b, Marina Gerhard b, Crispin Lichtenberg a, Dmitri Kosenkov cd and Olalla Vázquez *ae
aDepartment of Chemistry, Marburg University, Marburg, Germany. E-mail: olalla.vazquez@staff.uni-marburg.de
bDepartment of Physics and Materials Science Center, Marburg University, Marburg, Germany
cPrinceton Precision Health (PPH), Princeton University, Princeton, USA
dLewis-Sigler Institute for Integrative Genomics, Princeton University, Princeton, USA
eCentre for Synthetic Microbiology (SYNMIKRO), University of Marburg, Marburg, Germany

Received 9th November 2024 , Accepted 3rd March 2025

First published on 3rd March 2025


Abstract

We report how the conjugation of coelenterazine (CTZ) to BODIPY retains its activity as a versatile substrate for luciferase-type enzymes opening the possibility of taking advantage of BODIPY's fluorescent properties and capacity to generate singlet oxygen. Bioluminescence imaging-guided photodynamic therapy or 1O2-triggered drug release are potential applications of these conjugates.


Bioluminescence—light emission by living organismsis a powerful tool for studying biological processes because it relies on enzymes, enabling high sensitivity and biocompatibility.1 Consequently, bioluminescent systems are widely used in detection.2,3 Beyond cell tracking and reporter assays, the current bioluminescence toolkit has led to pioneering probes capable of monitoring metabolites at the point of care,4 radiometric sensors,5,6 uncaging inducers,7 signal-transduction triggers8 and photosensitiser activators.9 In many of them, the light generated from luciferase-type substrates drives bioluminescence resonance energy transfer (BRET), facilitating longer-wavelength emissions and internal activation by self-illumination. BRET reduces heat conversion and photobleaching and allows prolonged homogenous measurements,10,11 minimising the challenges associated with external excitation. Recent BRET systems involved engineered small luciferases linked to fluorescent or phototoxic proteins,12 like KillerRed13 and miniSOG,14 for either tunable emissions15 or singlet oxygen (1O2) production in cancer therapy.16 While genetically encoded tools are valuable, dye-substrate conjugates can enhance BRET by reducing the donor-to-acceptor distance. Besides, their smaller size should also minimise physiological interference and offer a simpler implementation. Along these lines, significant efforts have been devoted to synthesising derivatives of the luciferase-type substrate coelenterazine (CTZ).17 Unlike conventional D-luciferin, CTZ does not require ATP for activation. To improve optical performance, modifications of CTZ18–21 and dye conjugates19 were reported. Surprisingly, to our knowledge, BODIPY-CTZ conjugates remain unexplored despite their spectral overlap (Fig. 1) and the excellent spectroscopic properties of these fluorophores. Of note, BODIPY can easily turn into effective photosensitisers by halogenation,22 which gives versatility to these potential BRET probes. Herein, we designed novel substrates for the semisynthetic enzyme NanoLuc (NLuc).23 NLuc outperforms traditional luciferase enzymes in brightness, stability and size. In 2015, NLuc's potential was further expanded by the development of its split version, NanoBiT.24 NanoBiT consists of an optimised 18 kDa fragment LgBiT and high-affinity peptide HiBiT (Kd = 700 pM). Since BRET efficiency depends on donor–acceptor proximity and dipole orientation, we envisioned conjugates with different linker lengths (3 & 5) and the halogenated analogues (4 & 6).
image file: d4cc05979d-f1.tif
Fig. 1 Top: Evidence of BRET by luminescence and absorbance spectral overlap. Down: Chemical structure of the aim BODIPY-CTZ probes as NLuc substrates.

Two synthetic routes were explored for the CTZ core (Scheme 1). For conjugates with the expected longer linker (5 & 6), CTZ 9 was obtained by a Horner–Wadsworth–Emmons olefination.25 Subsequent acetylation with excess of acetic anhydride increased the precursor's stability. For the shorter-linker conjugates (3 & 4), the synthesis hinged on a palladium-catalyzed Hartwig–Buchwald N-arylation of chloropyrazine 10 with α-amino ester 11 yielding the key intermediate N-arylester 12.26 This was then converted into the O-acetylated CTZ 14via an in situ-generated acid salt. The latter procedure (Scheme 1B) was more economical and easily scalable. Finally, the O-acetylated CTZ 13 and 14 were conjugated to the corresponding BODIPY moieties via NHS ester formation. Conveniently, the coupling reaction also led to hydrolysis of the O-acetyl group. The resulting conjugates 3–6 were stored under N2 atmosphere in the dark at −80 °C to avoid CTZ decomposition.


image file: d4cc05979d-s1.tif
Scheme 1 (A) Synthesis of long BODIPY- (5) and 2I-BODIPY-CTZ (6) conjugates: (a) (1) TMG, MeOH, rt, 2 h; (2) NaBH4, DCM/MeOH 1[thin space (1/6-em)]:[thin space (1/6-em)]1, rt, 1 h; 27%; (b) Ac2O, rt, 2 h; 99%; (c) succinic anhydride, Pd(PPh3)4, PhSiH3, DMF, rt, 45 min; 83%; (d) (1) NHS, DIC, THF, rt, 45 min; (2) 15/16, NMM, THF, rt, 1 h; 25% for 5; 27% for 6. (B) Synthesis of short BODIPY- (3) and 2I-BODIPY-CTZ (4) conjugates: (e) Cs2CO3, Pd(OAc)2, BINAP, MeCN, 60 °C, 12 h; 76%; (f) (1) NaOH, THF, rt, 16 h; (2) Ac2O, THF, rt, 2 h; 38%; (g) for 3: (1) NHS, DIC, THF, rt, 2.5 h; (2) 17, NMM, THF, rt, 2.5 h; 37%; for 4: (1) NHS, DIC, THF, rt, 2.5 h; (2) 18, NMM, DMF, rt, 1.5 h; 42%.

Once synthesized, we investigated the ability of the conjugates to generate 1O2 under irradiation using 1,3-diphenylisobenzofuran (DPBF) as a trap27 and compared the results to the unconjugated photosensitizer 2 (Table SR1, SR2 and Fig. SR1, SR2, ESI). As expected, both conjugates displayed comparable photosensitizing capacity. Interestingly, 2, which lacks CTZ, surpassed them by ∼33%. To confirm that this difference was not due to a decrease in available 1O2 by reacting with the susceptible CTZ core, we added up to 277 eq of CTZ-400a (1) to 2 (Fig. SR3, ESI). Although 1 slightly decreased the rate of DPBF consumption, the conjugates 4 and 6 still displayed the slowest kinetics. Of note, CTZ hardly absorbed at 517 nm (Fig. SR4 and SR5, ESI). Next, we examined whether the conjugation impacted the fluorescence of the non-halogenated analogues 3 and 5 (Fig. SR6, SR7 and Table SR3, ESI). As before, fluorescence was lower for the conjugates 3 (ΦF = 0.243) and 5 (ΦF = 0.269) than for BODIPY without CTZ 22 (ΦF = 0.604).

To investigate these photochemical behaviours, we conducted excitation energy transfer modelling based on Förster resonance energy transfer (FRET) theory,28 as implemented in the PyFREC software29 and ab initio molecular models. In our FRET modelling (Tables SR4 and SR5, ESI), we assumed that the excitation energy of 2I-BODIPY is transferred via a FRET mechanism from the 2I-BODIPY donor to the CTZ acceptor. This FRET interaction facilitates photoexcitation energy transfer, which ultimately reduces the energy available for 1O2 production or fluorescence emission. This is also evident from the experimentally measured fluorescence lifetimes, where the lifetime of BODIPY-CO2H (4.581 ± 0.030 ns) slightly decreases upon the addition of CTZ, dropping to 4.367 ± 0.032 ns for 1[thin space (1/6-em)]:[thin space (1/6-em)]10 BODIPY-CO2H-to-CTZ concentrations. Additionally, short and long conjugates 3 and 5, which feature covalently bound CTZ groups, exhibit even shorter lifetimes 3.617 ± 0.048 ns and 3.819 ± 0.041 ns, respectively. The decreased energy available for these processes is a direct result of the efficient FRET mechanism. Furthermore, although conjugate 6 (and 5) has a donor–acceptor distance longer by approximately 30% compared to shorter conjugates, the mutual orientation factor of the donor and acceptor groups is ∼4–6 times more favourable in the longer conjugates 6 (and 5) (Table SR5 and Fig. 2, ESI). This orientation factor contributes to faster computed FRET rates in these shorter conjugates (Table SR5, ESI), which is likely an overestimation because modelling is based on one static minimal energy molecular geometry while an ensemble of molecular geometries exists in solution. Despite that experimentally, both short and long conjugates exhibit similar quantum yields, suggesting that the longer distance in conjugate 6 is offset by less favourable orientation factors in conjugate 4, likely due to the higher rigidity of the shorter linker. Finally, lower fluorescence lifetimes and higher FRET efficiencies were found for 3 and 5 (Table S1, Fig. S1–S6, Table SR3 and Fig. SR7, ESI).


image file: d4cc05979d-f2.tif
Fig. 2 Although the short 2I-BODIPY-CTZ (4) conjugate has a shorter donor–acceptor distance (dDA) than the long 2I-BODIPY-CTZ (6), the mutual orientation factor (Θ) of the transition dipole moments (red and blue arrows) is less favourable for FRET. This trend also holds for 3 and 5 (see Table SR5, ESI).

While direct BRET modelling is beyond this work's scope, we applied FRET theory to explore possible mechanisms of energy transfer for the BRET model. Although our FRET model does not yield absolute BRET rates, its distance- and orientation-dependent factors are analogous to those of BRET. Our modelling suggests that if the BRET excitation donor is (an oxidized form of) CTZ with the BODIPY moiety acting as the acceptor, then, again, a longer conjugate should result in more optimal donor–acceptor alignment and a faster BRET rate compared to the shorter conjugate (Table SR5, ESI).

Next, we explored if NanoBiT could oxidize the conjugates to generate light. We first verified LgBiT-HiBiT enzymatic activity using CTZ-400a (1) (Fig. SR8, ESI).26 Gratifyingly, both non-halogenated conjugates (3 and 5) produced detectable light but less than 1 (Fig. 3A). Consistent with our calculations, the long conjugate 5 exhibited a faster BRET rate and higher bioluminescence than the shorter one 3, possibly due to the more rigid, shorter linker chain in conjugate 3 and/or its molecular interactions. As previously reported for the conversion of CTZ derivatives by NLuc,26 the kinetics of 5 were best described by the substrate-inhibition model (Fig. SR9, ESI), displaying the highest signal with a characteristic flash-type bioluminescence. In contrast, the standard Michaelis–Menten model provided the best fit for 3. To evaluate whether the observed bioluminescence can activate the attached BODIPY via BRET, we recorded luminescence in the presence of LgBiT and HiBiT (Fig. 3B). BRET was detected for 5 (λmax = 518 nm) but not for 3 (λmax = 458 nm), which aligns with our kinetics studies.


image file: d4cc05979d-f3.tif
Fig. 3 (A) Km of 3 and 5 using LgBiT-HiBiT. Mean value of three independent measurements after 5 min of substrate addition. (B) Luminescence spectra of 3 and 5 at 14.8 μM in 50 mM Tris pH = 7.5, 150 mM NaCl, 0.005% Igepal CA-630 and 0.1 g L−1 BSA. (C) 1O2 detection using 25 μM Si-DMA, 12.5 μM of 5 or 6.8 μM of 6 in 10 mM phosphate buffer (pH 7.4), 100 mM NaCl, 20% glycerol. ****p < 0.0001.

Encouraged by the BRET efficiency of 5 and the ability of the conjugates 4 and 6 to produce 1O2 under irradiation (Table 1), we investigated if their bioluminescence could yield detectable 1O2. Several challenges arose: (i) reduced ΦΔ due to CTZ conjugation; (ii) solubility limitations (up to 50 μM); (iii) CTZ instability in solubilizing organic solvents; (iv) inherent difficulty in 1O2 detection. Initially, we tested NLuc-expressing cells with our conjugates. Unfortunately, the toxicity was modest without differences between halogenated and non-halogenated conjugates (Fig. SR10 and SR11, ESI). Singlet oxygen sensor green (SOSG) and electron paramagnetic resonance (EPR) analysis with 4-OH-TEMP were unsuitable due to the intrinsic requirements of our system, i.e., emission-spectrum overlap, photosensitizer concentrations >1 μM and physiological conditions (pH < 8). However, the far-red probe Si-DMA31 displayed a statistically significant response with 6, using almost half of 5 concentration (Fig. 3C and Fig. SR12, ESI). Interestingly, the enzyme alone appeared to interact with Si-DMA, increasing its fluorescence (Fig. SR13 ESI,Kd = 17.5 ± 5.0 μM) but not with bovine serum albumin (BSA).

Table 1 1O2 quantum yields (ΦΔ) in MeOH relative to erythrosine B (ΦΔ = 0.62)30 using a LED source (λem = 517 nm)
Compound I a 517 nm, 5.4 μM k [s−1 10−3] Φ Δ
a k reaction constant of 1O2 generation via DPBF decomposition. b Mean value of three independent measurements with errors ≤± 9%. Ia = absorbance.
2I-BODIPY-CO2H (2) 0.476 ± 0.020 32.6 ± 1.48 0.719
Short 2I-BODIPY-CTZ (4) 0.418 ± 0.022 19.4 ± 0.32 0.490
Long 2I-BODIPY-CTZ (6) 0.399 ± 0.020 18.1 ± 2.36 0.476


We thank Prof. Tallarek and Dr Thomas Roider (photometry); Prof. Koert (infrared spectroscopy); Prof. Hideg and Dr Carmielli (EPR); Marburg University for financial support.

Data availability

The supporting data are provided in the ESI.

Conflicts of interest

There are no conflicts to declare.

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Footnote

Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4cc05979d

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