Open Access Article
Spyros Letsiosab,
Giovana Carrasco
b,
Martin Lee
b,
Mateen Wagietc,
Marta Madureira
c,
Marley Samways
c,
Zaid Khan
b,
Valerie G. Brunton†
b,
Olivera Grubisha†
c and
Alison N. Hulme†
*a
aEaStChem School of Chemistry, University of Edinburgh, Edinburgh, EH9 3FJ, UK. E-mail: Alison.Hulme@ed.ac.uk
bCancer Research UK Scotland Centre (Edinburgh), Institute of Genetics & Cancer, University of Edinburgh, Edinburgh, EH4 2XR, UK
cUCB, Slough, UK
First published on 30th April 2026
Proteolysis Targeting Chimeras (PROTACs) are heterobifunctional molecules, emerging as a promising class of drugs. Amongst their structural components, the linker moiety plays a pivotal role in modulating their biological activity and physicochemical properties. Current PROTAC design strategies involve utilising shorter and more rigid linkers to limit the number of possible conformations within the ternary complex. We hypothesised that employing a short diyne spacer as the linker between the two ligands could generate highly potent PROTACs. Here, we report a series of diyne-bearing, low nanomolar BRD4 degraders recruiting the CRL4CRBN E3 ligase complex. As well as providing highly-active degraders, the Raman-active diyne moiety also enables the label-free visualisation of intracellular drug uptake at low micromolar concentrations via stimulated Raman scattering (SRS) microscopy. This work demonstrates the potential of diyne-based PROTAC linkers for both drug development and to address a key challenge within the field in understanding the cellular uptake mechanisms and intracellular localisation of PROTACs.
Recent advances in the field have shown that the linker not only connects the POI and E3 ligase ligands, but also strongly influences degradation activity and overall PROTAC efficacy.6 By introducing modifications to the linker, such as altering the length, composition or rigidity, the physicochemical, pharmacokinetic (PK) and pharmacodynamic (PD) properties can be optimised.6–9 Notably, limiting the number of possible ternary complex conformations by using shorter linkers or increasing linker rigidity can enhance the stability of the ternary complex.10 These adjustments ease computational analysis by limiting the complex's degrees of freedom, and also help maintain a lower molecular weight.6,10 However, each protein system is unique, and developing a potent PROTAC can be a lengthy process that may require testing linkers of different length and rigidity. Therefore, advances in the field often referred to as “linkerology” are required to optimise PROTAC linker design.9 We sought to evaluate the use of a rigid 4-atom diyne to overcome some of the current limitations in PROTAC linker development.
While significant progress has been made in PROTAC design strategies, high-resolution imaging of PROTACs that would yield useful insights on their intracellular localisation and mode of action remains underexplored. In recent years, stimulated Raman scattering (SRS) microscopy has emerged as a powerful new tool for label-free drug imaging.11–15 It offers valuable insights into the uptake and trafficking of (bio)molecules and aids selection of those with the most favourable drug-like properties. Among various functional groups, alkynes have been extensively employed as bioorthogonal Raman labels, generating signals within the cell-silent region of Raman spectra (1800–2800 cm−1).16,17 Advances in the design and development of alkyne-based Raman probes have significantly driven progress in this area.18–20 To date, the bisarylbutadiyne (BADY) moiety, which produces a strong signal at approximately 2200 cm−1, has been among the most successful Raman labels for drug imaging applications, due to its strong signal intensity and stability (Fig. 1a).21,22
In this study, we set out to design and synthesise a series of PROTACs that targeted the bromodomain and extra-terminal domain (BET) family proteins BRD2, BRD3, and BRD4. BRD4, in particular, has been one the most well investigated protein targets in PROTAC development.23–25 By coupling the aromatic rings of both the POI and E3 ligase ligands to a rigid 4-atom diyne linker, thus mimicking the BADY Raman probe, we sought to generate PROTACs that would produce an intense vibrational signal in the cell-silent region. By exploiting this feature, we planned to track the uptake of our PROTACs directly using SRS microscopy, and visualise their intracellular localisation at the low micromolar concentrations that are typical of drug screening assays, while confirming effective degradation activity under imaging conditions. If successful, this approach would provide the first high-resolution visualisation of PROTACs without the need to modify their structure to attach a label, offering new insights into PROTAC behaviour.
Two PROTACs were designed using the para position of the phenyl group of (+)-JQ1 as the exit vector. LS1 and LS2 (Fig. 1b) were obtained by linking the alkyne derivative of (+)-JQ1 to a bromo-alkyne derivative of lenalidomide (12) or of 1 (19) via Cadiot–Chodkiewicz coupling, with a yield of 63% and 33%, respectively for this key step (see Schemes S1–S4 for synthesis).34 To obtain PROTACs using the ester moiety as the exit vector (Fig. 1b), bisarylbutadiyne (BADY) derivatives of the CRBN ligands were synthesised with a methylamine handle at the meta and para positions respectively (Scheme S5). These CRBN binders were then coupled to the acid derivative of (+)-JQ1 via amide bond formation to yield LS3 and LS4 in 47% and 59%, respectively (Scheme S6). Milligram quantities of LS1–LS4 were obtained for biological testing in ≥95% purity, as determined by LC-MS analysis (see SI for chromatograms).
To further characterise the most efficacious PROTACs, LS1 and LS2, and to assess whether they preferentially degrade BRD4, the prototypic member of the BET family, HeLa cells were treated with 30 nM of either LS1 or LS2 for 6 h, followed by quantitative whole-cell proteome analysis (Fig. 1e). Results indicated that LS1 most significantly downregulated BRD4, while LS2 equally downregulated BRD2, BRD3, and BRD4.
BRD4 forms puncta at super-enhancers, which are large nuclear phase-separated condensates that drive high levels of transcription.37 We used high content confocal imaging, to visualise nuclear BRD4 puncta and to determine the effect LS1 and LS2 PROTACs have on them.38 HeLa cells were treated with compounds, immunostained and BRD4 puncta were identified and counted as distinct fluorescent spots in the nucleus (Fig. S3). After 24 h treatment with a range of PROTAC concentrations, LS1 and LS2 demonstrated a reduction in the number of BRD4 puncta, with maximum efficacy achieved at ∼100 nM, and DC50 values of 35 nM and 36 nM, respectively. LS4 achieved a partial effect, and demonstrated a DC50 of 98 nM (Fig. 2c, d and Fig. S4a). Importantly, both LS1 and LS2 were over 5 times more potent than MZ1 (DC50 = 200 nM) and had comparable potency to CRBN recruiting BRD4 PROTAC ARV825 (DC50 = 33 nM) (Fig. 2d and Fig. S4b), underscoring the potential of diyne linkers in BRD4 PROTAC development.24 Time-dependent BRD4 degradation was confirmed using high-content imaging after treatment with 150 nM of ARV825, LS1, and LS2, or 300 nM of MZ1 and LS4 (Fig. 2e and Fig. S5). All PROTACs led to a decrease of BRD4 puncta, indicative of BRD4 degradation in cell nuclei over time, with more than a 50% decrease observed after 24 h. Interestingly, the rate of degradation observed in this assay was slower compared to the western blot analysis, a phenomenon previously observed.38
We next investigated the mechanism of BRD4 degradation by LS2. Treatment of HeLa cells with 0.03 µM LS2 for 4 h effectively degraded BRD4 (Fig. 2f). Pre-treatment with the proteasome inhibitor MG132 or the neddylation inhibitor MLN4924 completely rescued BRD4 from degradation by LS2 (Fig. 2f).39 Additionally, introducing an excess of CRBN ligand, lenalidomide, provided some protection against BRD4 degradation. This was also confirmed using the immunofluorescence assay where co-treatment with MG132 abolished degradation by LS1 or LS2 (150 nM) (Fig. 2g and Fig. S6). These data demonstrate that the PROTACs degrade BRD4 via the ubiquitin-proteasome system in a CRBN-dependent manner.
36 ligand conformations were generated with equally spaced diyne dihedral angles. The BRD4 and CRBN proteins were then aligned onto each ligand conformer, rejecting any alignments which resulted in significant clashes between BRD4 and CRBN. Our analysis revealed that LS1's structural rigidity restricts BRD4-CRBN interfaces, with only 4 viable conformations out of 36. In contrast, LS2 which is less conformationally restricted, allowed for 23 conformations, highlighting the impact of structural restriction on protein alignment. Further refinement using molecular dynamics yielded a stable structure, with a representative snapshot of the BRD4(BD1):LS1:CRBN ternary complex, shown in Fig. 3a. These findings underscore the ability of diyne linkers to generate efficacious BRD4 PROTACs.
To monitor dissociation kinetics on ternary complexes we performed a Surface Plasmon Resonance (SPR) assay.41 When examining ternary complex formation within biophysical assays, a commonly used term is the “cooperativity” factor (α).36 This factor is defined as the ratio of binary over ternary dissociation constants (α = KD binary/KD ternary). When α > 1, cooperativity is positive, indicating enhanced ternary complex affinity. While not essential for PROTAC activity, gathering evidence suggests that stable ternary complexes with positive cooperativity can aid in PROTAC design.41
The SPR assay served to assess whether or not either LS1 or LS2 would create the appropriate multifaceted complex, consisting of BRD4BD1:PROTAC:CRBN, which is the required intermediate for ubiquitin transfer.7 Our assay involved pre-mixing the PROTAC with near-saturating concentrations of BRD4BD1 and then perfusing this complex solution to a pre-captured CRBN protein on the SPR chip surface (Fig. 3b). LS1 generated a KD response of 426 nM with a half-life of t1/2 = 120 s, whilst in binary study format, the KD for CRBN binding of LS1 was found to be 1320 nM (Fig. 3c, S7 and Table 1 and Table S1). Therefore, LS1 demonstrated positive cooperativity with an α value of 3.1. Further SPR studies confirmed that LS2 also facilitated ternary complex formation, with a KD response of 58 nM and a half-life of t1/2 = 81 s. In binary assay format, LS2 produced a KD of 1810
nM (Fig. 3c, Table 1 and Table S1), giving an α value of 31.1, indicating impressively positive cooperativity. These results suggest that the new diyne linker format adopted for both LS1 and LS2, despite its rigidity and short length, has the ability to form stable ternary complexes with promising dissociation kinetics. Positive control BRD4 PROTAC ARV825 having a flexible linker, was also utilised in this assay to provide comparison. It generated a KD response of 188 nM with a half-life of t1/2 = 244 s, and an α value of 3.6 comparable to that of LS1 (Table 1).
| Compound | KD (nM) | kon (M−1 s−1) × 105 | koff (s−1) | t1/2 (s) | α |
|---|---|---|---|---|---|
| a For a detailed analysis of the binary complex results against BRD4BD1, BRD4BD2 and CRBN, see Table S1. SPR values were derived from fitted kinetic data: dissociation constant (KD = koff/kon), and cooperativity (α = KD binary (CRBN)/KD ternary). (ARV825 & LS1: n = 2 independent experiments, LS2: n = 1). | |||||
| ARV825 | 188 | 0.21 | 0.0034 | 244 | 3.6 |
| LS1 | 426 | 0.18 | 0.0084 | 120 | 3.1 |
| LS2 | 58 | 1.47 | 0.0085 | 81 | 31.2 |
To further study the intracellular localisation of LS1, we used multi-modal imaging. HeLa cells were simultaneously treated with LS1 (10 µM) and ER-tracker Blue-White (1 µM) to mark endoplasmic reticulum. Imaging showed that LS1 co-localised with ER-tracker (Fig. 4c, Pearson's coefficient: r = 0.83). For comparison, (+)-JQ1-pBADY and lenalidomide-BADY molecules were synthesised (see SI for synthesis). After SRS imaging both compounds demonstrated a similar localisation as LS1, mainly accumulating to the lipid rich region surrounding the nucleus (Fig. S8b, c). These findings align with previous imaging studies of (+)-JQ1 having amide-bound BADY and of 80S ribosome inhibitor anisomycin tagged with the BADY moiety.21,22 In contrast, when cells were incubated with the BADY probe (1 µM), it mainly accumulated within lipid droplets in the cytoplasm (Fig. S9). This indicates that the BADY probe itself does not direct the molecules toward the endoplasmic reticulum (ER). To provide comparison, the autofluorescence properties of the pomalidomide-bearing BRD4 PROTAC ARV825 were exploited to visualise its distribution within HeLa cells (Fig. S10a and b). Despite ARV825 containing a flexible PEG linker, its intracellular localisation was similar to that of LS1, and it was shown to be mainly localised within the ER of the cells (Fig. S10c). Taken together, these data suggest that our new linker moiety is not the driving factor behind the ER accumulation of our molecule. However, further studies will be required to fully elucidate these findings.
SRS microscopy offers the advantage that signal intensity is directly proportional to sample concentration.44,45 However, quantifying absolute intracellular concentrations with SRS can be challenging due to variations in signal intensity across cells.
We first demonstrated the linear relationship between LS1 concentration and Raman intensity through SRS imaging of LS1 in DMSO at various concentrations (Fig. S11a). By quantifying the intracellular concentration of LS1 in individual cells, we estimated the concentration range within cells (Fig. S11b). Quantification showed a stepwise increase in intracellular LS1, with 50- to 200-fold enrichment compared to treatment concentrations.
Although BRD4 is exclusively nuclear, LS1 predominantly localises to the endoplasmic reticulum (ER).22,38 Upon further examination, a weak nuclear LS1 signal was observed at a treatment concentration of 10 µM. A line profile of SRS intensity across a cell revealed a 3.5-fold increased nuclear intensity compared to background, while the cytoplasmic signal showed approximately a 5.5-fold increase in intensity (Fig. S12a and b). Additionally, hyperspectral imaging of the nuclear region revealed a weak on-resonance peak of LS1, further validating its presence within the nucleus (Fig. S12c and d). We also established that there was no unwanted degradation of the diyne vibrational motif in LS1 in the presence of intracellular nucleophiles such as glutathione (Fig. S13).19,22 Importantly, even after 4 h of treatment with 1 µM and 10 µM of LS1, more than 50% and 75% of BRD4 remained, respectively (Fig. S14). This indicates that the weak nuclear LS1 signal is not due to target protein degradation. Our previous results demonstrate that 10 µM and 1 µM concentrations of LS1 can efficiently degrade BRD4 after 24 h. Therefore, the nuclear levels of LS1 are sufficient to engage the target protein and degrade it via the UPS (Fig. 2a and c).
Intriguingly, proteasomal inhibition induces nucleolar aggregates containing ubiquitin and nucleoplasmic proteosome target proteins.46 Fig. 2g shows that treatment with 20
µM MG132 for 12 h results in intranuclear BRD4 puncta approximately three times higher than in untreated cells. To enhance nuclear LS1 signal, we blocked the proteasome again with MG132 (20 µM) for 16 h before incubation with LS1. Notably, after proteasomal inhibition, LS1 localised not only in the ER but also within these nucleolar aggregates (Fig. 4d). Importantly, when BADY was added, it was not detected in the nucleolar aggregates (Fig. S15a), suggesting that the presence of LS1 is due to its binding to BRD4 and CRBN. Treatment with (+)-JQ1-pBADY and lenalidomide-BADY also showed a signal within the nucleolar aggregates, however, the signal intensity was much weaker compared to LS1 (Fig. S15b, c). A possible explanation is that both BRD4 and CRBN proteins are present in the aggregates, leading to higher quantities of LS1.
Biological characterisation of our PROTACs, LS1–LS4, revealed that those having the linker attached at the para position of (+)-JQ1, LS1 and LS2, are particularly potent and rapid degraders of BRD4. LS1 and LS2 can achieve over 90% BRD4 degradation, and were shown to have DC50 values of 35 nM and 36 nM, respectively using a high-content confocal imaging assay. Mechanistic investigations confirmed that these PROTACs induce CRBN-dependent degradation via the UPS.
It has been previously reported that structurally constrained PROTAC linkers can enhance selectivity against BRD4 by limiting the number of accessible interprotein interactions.27 Interestingly, our quantitative whole-cell proteome analysis shows that despite the high conformational restriction of LS1 and LS2, both can significantly degrade BRD4, as well as BRD2 and BRD3. However, LS1 appears more selective for BRD4 compared to BRD2 and BRD3, suggesting that its higher conformational restriction results in increased selectivity. In contrast, LS2 shows no preference, which may be due to its more flexible structure.
SPR binding studies confirmed the formation of a stable, ternary complex, between BRD4BD1 and CRBN in the presence of LS1 or LS2. Notably, this complex exhibited positive cooperativity, with α values of 3.1 and 31.1, for LS1 and LS2, respectively. Understanding the cooperativity of PROTAC ternary complexes can provide crucial insights into their stability, potentially aiding in rational PROTAC design.41
Additionally, our computational model of the BRD4(BD1):LS1:CRBN ternary complex provided a structural hypothesis for ternary complex formation, while also demonstrating how the linker is predicted to be placed within the ternary complex. LS1 and LS2, to our knowledge, are the first known PROTACs with completely rigid and linear linkers. Their structural restriction provides an entropic advantage compared to flexible linker bearing PROTACs, allowing only rotational movement around the linker axis and significantly reducing potential conformations. Their structure together with our reported data make them attractive for in silico ternary complex structure predictions. Similar types of linkers could aid future drug design strategies by significantly reducing the uncertainty of linker protein interactions.
Utilising imaging technologies to directly track drugs can provide crucial information on intracellular drug localisation, identify mechanisms of drug resistance and guide modifications to improve cellular entry enhancing the success rate of drug candidates.15 It complements information provided by protein-tagging technologies that can track real-time degradation and recovery profiles for individual target proteins.47 Although, fluorescently labelled PROTACs have been utilised to demonstrate their mechanism of cellular uptake, the resolution provided by these is poor and the intracellular distribution of the PROTACs themselves remains largely unknown.48 Our SRS imaging data demonstrate that the label-free PROTAC LS1 can be visualised within cells at the low micromolar concentrations typically used in drug screening assays, and at which degradation activity has been confirmed. Unexpectedly, LS1 was observed mainly within the ER of the cells. Spectral analysis of SRS images revealed a weak nuclear signal for LS1, likely due to target engagement. Interestingly, ARV825, which lacks the rigid diyne moiety, was also co-localised within the ER of the cells, suggesting that the ER accumulation of LS1 is not driven by the linker's structure.
By exploiting the quantitative nature of SRS microscopy, we were able to measure the relative intracellular concentrations of LS1 within individual cells. After treatment with 1 µM of LS1, we observed approximately a 200-fold enrichment, however, at 10 µM, the enrichment decreased to 50-fold. Advancing this approach could be valuable for assessing drug permeability across cell membranes in the future.
Our findings demonstrate that a 4-atom, linear PROTAC linker, which cannot bend to fit the protein–protein interface, can be utilised to generate potent PROTACs while allowing for the formation of a stable ternary complex. These molecules are the first PROTACs, to our knowledge, that can be directly imaged using SRS microscopy in real time within live cells at biologically relevant concentrations and without the need for external probe attachment. This innovative approach not only enhances our understanding of PROTAC distribution but could also provide insights into drug localisation in resistant cell lines, as well as aid in studying the kinetics and mechanisms of uptake across various cell lines. We anticipate that future application of these linkers in PROTAC development will enable the targeting of novel proteins for both drug discovery and diagnostic purposes.
Cells were washed once with ice-cold PBS and lysed for 5
min at 4 °C with RIPA buffer (50 mM Tris-HCl, pH 7.4, 150 mM NaCl, 1% w/v Triton X-100, 0.5% w/v sodium deoxycholate, 0.1% w/v SDS; all from Sigma-Aldrich) supplemented with protease (0.4% v/v) and phosphatase (2% v/v) inhibitors (Sigma-Aldrich). After centrifugation (13
300g for 10 min at 4 °C) the protein concentration of the supernatant was quantified with Pierce™ BCA protein assay (23
227, Thermo Fischer Scientific) based on the manufacturer's instructions. Samples were prepared by 5 min incubation at 95 °C with NuPage™ LDS sample buffer (NP0007, Thermo Fisher Scientific). Proteins were separated according to size with Mini-Protean® TGX Precast gels with 20–30 µg protein per well and transferred to a PVDF membrane (Bio-Rad). The membrane was then blocked for 1 h with 5% milk TBS-T at room temperature, before incubating with primary antibodies at 4 °C overnight. The following primary antibodies were used: BRD2 (1
:
2000, Abcam, ab139690), BRD3 (1
:
200, Abcam, ab50818), BRD4 (1
:
1000, Thermo Fischer Scientific, A301-985A-T). Membranes were then washed with TBS-T three times and incubated for 1 h at room temperature with secondary anti-rabbit IgG HRP-linked antibody (1
:
3000, Cell Signalling Technology, 7074P2) or anti-mouse IgG HRP-linked antibody (1
:
3000, Cell Signalling Technology, 7076P2). After three TBS-T washes, the membrane was then incubated with Clarity Western ECL blotting substrate (Bio-Rad) or with SuperSignal™ West Femto Maximum Sensitivity Substrate (Thermo Fischer Scientific) and visualised using a ChemiDoc imaging system (Bio-Rad). All antibodies were diluted in 5% milk TBS-T.
:
500, Abcam, ab128874) and incubated overnight at 4 °C. After washing three times with PBS, cells were incubated with fluorescent secondary antibody (Alexa Fluor 647, 1
:
1000, Thermo Fischer Scientific, A-21447), Alexa Fluor 568 phalloidin (1
:
10
000, Thermo Fischer Scientific, A12380) and NucBlue Fixed Cell ReadyProbes Reagent (2 drops per mL, Thermo Fischer Scientific, R37606) for 2 h at room temperature. All antibodies, phalloidin and NucBlue were diluted in blocking buffer. Images were acquired using Opera Phenix High Content Screening System (PerkinElmer). Images were processed and analysed using a pipeline to detect BRD4 puncta spots in live nuclei (Harmony v5.2).
The pellet was lysed in 5% SDS, 100 mM Tris pH 8.5, 1
mg
mL−1 chloroacetamide, 1.5 mg mL−1 Tris(2-carboxyethyl)phosphine. The lysate was sonicated using SoniPrep 150 (MSE) for 30 seconds and then heated at 95 °C for 30 min. The lysate was bound to MagReSyn® HILIC (Resyn Biosciences) beads and processed on KingFisher.49 Bound lysate was washed in acetonitrile followed by ethanol and the proteins were digested in 50 mM triethylammonium bicarbonate (TAEB) containing 1 µg trypsin. The resulting peptides were desalted using a C18 column.
The peptides were loaded onto 25 cm Aurora Columns (IonOptiks, Australia) and separated by nanoscale C18 reverse-phase liquid chromatography using an UltiMate 3000 RSLC nano system coupled online to an Orbitrap Fusion Lumos Tribrid mass spectrometer (Lumos) (all Thermo Fisher Scientific). HPLC buffers: 0.5% acetic acid in HPLC-grade water (buffer A); 0.5% acetic acid in HPLC-grade acetonitrile (buffer B) were prepared. HPLC method was programmed as follows: gradient increased from 5% to 30% buffer B in 70 min. The mass spectrometer was operated in DIA mode, acquiring a MS 350–1650 Da at 120k resolution followed by MS/MS on 45 windows with 0.5 Da overlap (200–2000 Da) at 30k with a NCE setting of 28.
Since the initial structures were generated by rigid-body alignment, we then relaxed the complexes. First, any protein sidechains involved in heavy atom clashes were removed and then re-modelled using the Schrödinger Protein Preparation Workflow.50 We then sought to use the OpenMM molecular dynamics (MD) software engine to further relax these complexes.51 In order to ensure a gradual relaxation for each structure, the solvated system was first minimised with harmonic restraints (10 kcal mol−1 Å−2 force constant) applied to all protein/ligand heavy atoms. The restraints were then removed on the protein sidechain atoms, and the system was re-minimised. This process was repeated to remove the restraints from the protein backbone atoms, and then finally from the ligand atoms. Each of these minimised structures was then simulated for 50 ns of MD, with structures saved every 0.5 ns (the first 10 ns of simulation was discarded as equilibration). Additional details around these MD simulations can be found in the Supporting Information. The structure shown in Fig. 3a was selected as a representative snapshot of these structural ensembles, as it showed the lowest median RMSD to all other simulation frames. This RMSD was calculated based on the BRD4 Cα atoms, after having aligned the CRBN backbone.
s, flow rate 10 µL min−1). The anti-GST antibody (30 µg mL−1, in running buffer), was then amine-coupled to the sensor chip surface, followed by deactivation using 1 M ethanolamine. Next, the sensor chip was equilibrated in running buffer (1% DMSO, HBS-P+ (1×)). GST tagged CRBN (1 µg mL−1, in running buffer) was then anti-GST antibody captured to the required density (100 RU).
:
1 with a solution of 50 µM of BRD4BD1 or BRD4BD2 in running buffer, to prepare a final solution of 400 µL of 1 µM compound and 25 µM of bromodomain respectively. The complex was then serially diluted in running buffer containing 2 µM of bromodomain (4-point 2-fold serial dilution, 1 µM to 62.5 nM concentration of compound, and 25 µM to 3.44 µM concentration of bromodomain). Solutions were injected individually in multi-cycle kinetic format (contact time 400 s, flow rate 30 µL min−1, dissociation time 600 s) using a stabilisation period of 60 s and syringe wash (50% DMSO) between injections.Images were captured using a custom-designed multi-modal microscope setup. A picoEmerald S laser system (APE, Berlin, Germany) supplied a tunable pump laser (700–990 nm, 2 ps, 80 MHz repetition rate) alongside a spatially and temporally combined Stokes laser (1032 nm, 2 ps, 80 MHz repetition rate). The output beams were directed into the scanning unit of an Olympus FV1000MPE microscope through a series of dielectric mirrors and guided into an Olympus XLPL25XWMP N.A. 1.05 objective lens using a 690 nm short-pass dichroic mirror (Olympus). For SRS measurements, the Stokes beam was intensity modulated using a 20 MHz EoM integrated into the picoEmerald S. Forward scattered light was gathered with another 25× Olympus XLPL25XWMP N.A. 1.05 objective lens, with Stokes light being filtered out using a Chroma ET890/220 m filter. A telescope focused this light onto an APE silicon photodiode, linked to an APE lock-in amplifier set with a 20 µs time constant. The lock-in amplifier signal was transmitted to an Olympus FV10-Analog unit. Laser powers post-objective reached 20–100 mW for the pump laser and 50–400 mW for the Stokes laser. Images were recorded at resolutions of 512 × 512 or 1024 × 1024 pixels with a pixel dwell time ranging from 4 to 20 µs, by averaging 2–4 times, utilising Olympus's FluoView FV10-ASW scanning software. Image analysis and processing were carried out using ImageJ 1.53c.
To eliminate background processes in SRS images of alkynes, off-resonance images were captured by tuning the pump wavelength 2 nm (∼30 cm−1) away from the on-resonance image. These were then subtracted from the on-resonance image using ImageJ's ‘Image Calculator’ function. ImageJ also facilitated adjustments to brightness and contrast, as well as the assignment of false colours and scale bars.
Footnote |
| † These authors jointly supervised this work. |
| This journal is © The Royal Society of Chemistry 2026 |