Introduction

Room temperature phosphorescence (RTP) of organic materials with persistent emissions can mitigate the interference from environmental self-luminescence. Moreover, the organic matter often has advantages of low toxicity and good biocompatibility1,2,3,4,5,6,7,8,9,10. Therefore, constructing organic RTP materials would benefit tissue imaging, tumor diagnosis, and drug tracking10,11,12,13,14,15. To date, most phosphorescent materials have poor biological tissue permeability because the wavelengths of their emission spectra are short (less than 580 nm)9,16,17,18,19,20,21,22,23,24,25,26. This only means phosphors provide good imaging in shallow regions of an organism. Constructing near-infrared phosphorescent materials has gained some urgency. Although some red RTP materials such as boron fluoride, carbazole, and naphthalene diimides have been developed, those with wavelengths exceeding 650 nm are rare27,28,29,30,31,32. Moreover, presumably limited by the energy gap law, phosphorescence lifetimes of these red RTP materials are very short and not conducive for bioimaging (Fig. 1a and Supplementary Fig. 1).

Fig. 1: Design concept of the guest/host system.
figure 1

a Problems in constructing ultralong near-infrared RTP materials b Phosphorescence performance distribution of RTP materials. c Strategy used in this work for constructing ultralong near-infrared RTP materials.

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Establishing ultralong-lifetime RTP materials with long-wavelength emission inevitably means lowering the lowest triplet (T1) level of the material. However, lower T1 levels bring two major obstacles to phosphorescence. One of the obstacles is that lower T1 increases the band gap between S1 and T1 (ΔEST), which is not conducive to intersystem crossing (ISC) of excitons. The other obstacle is that a lower T1 level easily causes excitons to be consumed non-radiatively, resulting in a significant reduction in lifetime and intensity of phosphorescence (Fig. 1b). Therefore, assuming materials already have low T1, improving the ISC capability of excitons and suppressing the non-radiative transitions of excitons are key in achieving ultralong-lifetime near-infrared/NIR phosphorescence. Recently, guest–host materials have gradually attracted more attention33,34,35,36,37,38,39,40, because the host molecules can inhibit the non-radiative transition of the guest energy in the guest–host system41,42,43,44,45,46. Additionally, several research results have shown that there is a synergy of energy between host and guest molecules, which can assist the guest molecules to transfer the excited state energy effectively38,39,40,41,42. Therefore, the guest–host system provides a new strategy for the construction of organic RTP materials with long-wavelength emissions and long lifetimes.

With that in mind, we tried to construct ultralong-lifetime near-infrared RTP materials employing a guest–host doped strategy. The pyrene derivatives with high conjugation are regarded as guests. Their high conjugation can reduce the T1 levels of the molecules, thereby ensuring that the resultant materials undergo long-wavelength phosphorescence. The benzophenone (BPO) compound is chosen as the host matrix, which can act as two roles. One role is associated with assisting transfers of guest excitons; the other role is associated with restricting the motion of the guest molecules, thereby suppressing the non-radiative transition of guest excitons (Fig. 1c). The results show that the designed guest–host materials have strong red afterglow visible to the naked eye. By increasing the degree of conjugation of the guest molecules, phosphorescence wavelengths of the guest–host materials are red-shifted from 600/657 nm to 681/732 nm. More importantly, our newly developed guest–host materials have long phosphorescence lifetimes of 102–324 ms. To the best of our knowledge, this is the first RTP material with both long-wavelength (>700 nm) and long lifetime (>100 ms) simultaneously. Comparative experiments of the molten state and the crystalline state prove that the host matrix restricts the motion of guest molecules is a necessary condition for the doped system to have phosphorescence emission. Molecular dynamics (MD) simulations further show that between host and guest there is a strong interaction that suppresses non-radiative transitions of guest excitons. Moreover, experimental results also confirm that host molecules exhibit synergies with guest molecules in excited states. As a proof-of-concept, the materials were used for precise mapping of lymph nodes and labeling of armpit tumors with high signal-to-background ratios (SBR) of 55 and 43, respectively. The long wavelengths help to reduce scattering from tissue and long lifetimes further mitigate the interference from autofluorescence in bioimaging. Thus, phosphorescent materials with both kinds of properties can provide more unambiguous imaging of tumors.

Results

Synthesis and photophysical properties

The guest molecules are based on the pyrene unit, to which adding anisole or N,N-dimethylaniline groups on one or both sides through the Suzuki reaction increases the molecular conjugation (Fig. 2a and Supplementary Fig. 2). The five guests show good solubility in chloroform, tetrahydrofuran, and dimethyl sulfoxide. The molecular structures and purities of the target compounds were confirmed by NMR spectroscopy, single-crystal X-ray diffraction, and high-performance liquid chromatography (Supplementary Figs. 3,  4). As guest conjugation increases, the maximum absorption peaks are red-shifted from 343 to 378 nm (Supplementary Fig. 5a), and the corresponding fluorescence peaks are also red-shifted from 381 to 467 nm (Supplementary Fig. 5b). The host BPO was purchased directly from a commercial supplier and used without further processing. BPO has a low melting point (48 °C) and stable subcooling states and thus the guest molecules can be dispersed in the host using the melt-casting method (The detailed process is in the supplementary information). Because the concentration of the guest molecules is very important in determining the RTP properties of the guest–host materials, we first prepared a series of Py/BPO guest–host materials with different guest–host molar ratios (1:50–1:50000) to optimize the luminescence performance. The phosphorescence quantum yields of 1:50, 1:100, 1:500, 1:1000, 1:5000, 1:10000, and 1:50000 are 3.3, 5.5, 7.8, 9.2, 6.8, 5.1, and 3.6%, respectively. The delayed emission spectra further shows that doped material with the guest–host molar ratio of 1:1000 has the strongest phosphorescence intensity (Supplementary Fig. 7), which is in accordance with our previous work39,40,41,42. Four other guest–host materials (MOPy/BPO, MAPy/BPO, DMOPy/BPO, and DMAPy/BPO, Fig. 2a) with a guest–host molar ratio of 1:1000 were prepared, and the luminescence characteristics of the guest–host systems were systematically investigated.

Fig. 2: Photoluminescence properties of the guest–host system.
figure 2

a Molecular structures of the guest and host molecules. b Fluorescence (top) and phosphorescence (down) images of the guest–host materials. c Phosphorescence spectra of host–guest materials. Excitation wavelength: 380 nm; Delayed time: 1 ms. d Phosphorescence decay curves of guest–host materials. Excitation wavelength: 380 nm.

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Five guest–host materials show blue to cyan fluorescence under the excitation source (Fig. 2b) and the maximum emission peaks of the guest–host materials are red-shifted from 416 to 483 nm as guest conjugation increases (Table 1 and Supplementary Fig. 8). Importantly, after finishing the irradiation, with the exception of DMAPy/BPO, the other four guest–host materials have visible to the naked eye a deep red afterglow for ~3 s that reveal the RTP properties (Fig. 2b). Delayed spectra further show that the guest–host materials have two phosphorescence peaks, which are fine structures that arise from energy level vibrations. Similarly, with increasing guest conjugation, the phosphorescence peaks of the guest–host materials are red-shifted from 657 to 732 nm or 600 to 681 nm (Table 1 and Fig. 2c). That is, the guest–host materials produce deep-red or even near-infrared phosphorescence emissions and belong to a group that produces phosphorescence with the longest wavelengths to date. The Commission Internationale de l’Eclairage coordinates further indicate that the guest–host materials have a very deep phosphorescent color (0.63, 0.35; 0.64, 0.34; 0.65, 0.33; 0.69, 0.30; 0.70, and 0.29) (Supplementary Fig. 9). Unlike most red RTP materials which have short phosphorescence lifetimes, the phosphorescence lifetimes of this guest–host system are 102–324 ms (Table 1 and Fig. 2d). Moreover, the guest–host materials have satisfactory luminous intensities, the phosphorescence quantum efficiency being in the range 4.2–9.2% (Table 1). The above results fully prove that, with the guest–host doped strategy, we have developed a group of ultralong-lifetime near-infrared RTP materials. As we know that the stability of materials will greatly affect practical applications. To verify the stability of the doped materials, Py/BPO and MAPy/BPO were chosen to soak in water for 24 h, and two materials still have a strong red afterglow (Supplementary Fig. 12). And the Py/BPO and MAPy/BPO can still maintain obvious red afterglow after being continuously irradiated for 24 h (365 nm, 40 μW/cm2) (Supplementary Fig. 12). In addition, even if the doped materials are left in the ambient environment for one month, the phosphorescence activities are basically unchanged. Therefore, the RTP properties of these materials are very stable to water, light, and air.

Table 1 Photophysical data of the guest–host materials.
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Generally, the triplet excitons are unstable and easily assimilated by the motion of molecules, leading to the quenching of phosphorescence. However, for the guest–host system, the host matrix can provide a rigid environment to restrict the motion of guest molecules, thereby ensuring the guests emit phosphorescence42,43. We first register the phosphorescence of the solution and solid guests at low temperature (77 K) to verify that the phosphorescence from the guest–host system is emitted by the guest molecules. The spectra show that the guests in the solution state have two fine peaks at 77 K, and the emission peaks are also red-shifted from 596/665 nm to 652/725 nm (Supplementary Fig. 13). The spectral data were almost completely consistent with the phosphorescence wavelengths of the corresponding doped materials. The results confirm that the phosphorescence in the guest–host system is emitted by the guest molecules. Taking advantage of the low melting point of the host, the influence of the host morphology on the phosphorescence performance of the guest–host system was analyzed. The Py/BPO molten state at room temperature (subcooling state) show only fluorescence but no phosphorescence (Fig. 3a, b). However, when the guest–host material begins to crystallize, the material produces a bright red phosphorescence. This clearly proves that the host matrix restricts the guest molecular motion and is a necessary factor in determining the RTP properties of the guest–host system.

Fig. 3: Non-radiative suppression of guest excitons by host matrix.
figure 3

a Photographs of Py/BPO in different states. b Phosphorescence spectra of Py/BPO. Excitation wavelength: 380 nm; Delayed time: 1 ms. c Model setup of Py/BPO guest–host system. d Spatial distances between the Py molecule and the surrounding BPO molecules. e Interaction distances of C-H---π or C-H---O interactions between Py molecule and surrounding BPO molecules. The distances between each phenyl ring center of Py molecule and the hydrogen atom of the BPO molecules are marked by a red line. The corresponding distances between the oxygen atom of BPO and the hydrogen atoms of Py are marked by a blue line.

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Molecular dynamics simulations

The local microenvironment of the molecules such as the molecular configuration, intermolecular distance, and intermolecular interaction plays an important role in determining the photophysical phenomena of materials. However, obtaining the co-crystal of host–guest is difficult because of the trace amounts of guest molecules (<0.1%) in the entire materials. Moreover, the traditional characterization methods such as X-ray diffractometry, scanning electron microscopy, and transmission electron microscopy are difficult to apply in investigating the molecular conformation of the guests in the host matrix in detail. Therefore, we simulated the molecular conformations of Py molecules in the BPO matrix using molecular dynamics/MD simulations40. The initial Py/BPO model was based on the BPO crystal. A BPO molecule is removed from the BPO crystal (Fig. 3c) and a Py molecule is inserted into the vacancy. This Py/BPO model has a 1:191 molar ratio of Py to BPO. Starting from the initial Py/BPO configuration, we performed production MD simulations for 10-ns to relax the whole guest–host system using the GROMACS software package (version 5.1.5, details in Supplementary Information). Compared with the conformations of BPO molecules in a single crystal, the corresponding conformations of the BPO molecules adjacent to the guest Py molecule in the Py/BPO guest–host system are slightly different because twisting increases the angles slightly after doping (Supplementary Fig. 14). This is because the spatial volume of the Py molecule is larger than that of the BPO molecule. However, because the number of guest/Py in the guest–host system is very small, the impact on the overall arrangement of the host matrix is minimal. Therefore, the stacking of BPO molecules in the simulated guest–host system is almost the same as for a single crystal (Supplementary Fig. 15, Supplementary Fig. 16). The XRD results also confirm little change in the arrangement of the BPO host before and after doping with guest molecules (Supplementary Fig. 17). Therefore, we have a microenvironment model of the guest–host system that is reasonable and reliable for our MD simulations.

With this Py/BPO model, we first analyzed the relative spatial positions of the Py molecule in the BPO matrix (Fig. 3d). The distances between the guest and host molecules in the six directions (up, down, front, back, left, and right) range from 2.3 to 3.1 Å. That is, the guest molecules are in a relatively dense matrix environment, which can effectively inhibit their motion. More importantly, although these distances are relatively similar, the host has a twisted molecular conformation. Therefore, there is no π---π interaction between host and guest, and hence it is not conducive for luminescence. In contrast, between the host and Py molecules, multiple C-H---π interactions are evident over short distances (2.3–3.2 Å, red line) (Fig. 3e), and the average distance between a Py molecule and surrounding host molecules is only 2.77 Å. In addition, the C-H---O interactions between Py and host molecules are also evident over short distances (2.5 and 2.6 Å, blue line) (Fig. 3e). The above analysis shows that the Py-doped host matrix provides a relatively close and strongly interactive environment for guest molecules that effectively restricts the non-radiative decay channels.

RTP mechanism study

The rigid environment provided by the matrix is necessary for the guest–host system to display RTP characteristics. However, is this the only role the host molecules play? We chose separately as host sulfonyldibenzene (SOB), sulfinyldibenzene (SIB), and diphenylphosphine oxide (PPO), which also have good crystallinity and a similar structure to BPO (Fig. 4a), and MAPy as guest. The three guest–host materials (MAPy/SOB, MAPy/SIB, and MAPy/PPO) were prepared with a guest–host molar ratio of 1:1000. Unfortunately, although these materials have strong cyan fluorescence under a UV lamp, no red afterglow appears once the UV source is removed (Fig. 4b). The fluorescence spectra of the three guest–host materials show wavelengths centered around 430 nm (Supplementary Fig. 18a), with quantum yields as high as 63, 71, and 76% in the order given above. Such high luminous intensities indicate that the host indeed inhibits the motion of the guest molecules. However, the delayed spectra suggest that the guest–host materials have almost no phosphorescence emission (Supplementary Fig. 18b). Note that, although the phosphorescence from MAPy/SOB and MAPy/SIB are very weak, there is an emission peak near 670 nm that once again demonstrates that the phosphorescence in the guest–host material is emitted by the guest molecules. The above comparative experiments show that the rigid restrictive environment provided by the host is a necessary but not a sufficient factor, for the guest–host materials to display RTP properties.

Fig. 4: Luminescence properties of guest molecules in other hosts.
figure 4

a Molecular structure of the reference hosts. b Luminescent images of the reference guest–host materials.

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Energy transfers between host and guest molecules have gradually been revealed to play a vital role in phosphorescence activity. Among them, Förster resonance energy transfer (FRET) is considered a viable explanation why some guest–host materials have RTP properties23,38. To verify whether there is a FRET between host and guest, the absorption and excitation spectra of host BPO and guest MAPy were investigated. The absorption and excitation wavelengths of host BPO (Fig. 5a) only reach 418 nm, whereas the absorption and excitation wavelengths of the guest MAPy reach 465 nm. Therefore, we investigated the phosphorescence emission of MAPy/BPO material at different excitation wavelengths. The results show that even if the excitation wavelength is extended to 440 nm, the MAPy/BPO powder maintains a strong phosphorescence emission (Fig. 5b) and has a red afterglow visible to the naked eye after removing the 420-nm UV source (Fig. 5c). These results clearly demonstrate that the phosphorescence of MAPy/BPO does not come from the energy absorbed by the host matrix, but from the energy absorbed by the guest molecules. Therefore, a FRET between host and guest is ruled out.

Fig. 5: Energy transfer between guest and host.
figure 5

a Excitation spectra of host BPO powder and guest MAPy powder. b Phosphorescence spectra of guest–host material MAPy/BPO at different excitation wavelengths. Excitation wavelength: 380 nm; Delayed time: 1 ms. c Luminescence photos of the MAPy/BPO powder. Excitation spectra of fluorescence (d)/phosphorescence (e) of MAPy in different solvent and molten state host (Concentration: 1 × 10−4 mol/L). f Phosphorescence decay curves of the guests in 77 K (Ex: 380 nm; Concentration: 1 × 10−4 mol/L; Solvent: 2-methyltetrahydrofuran). g Proposed transfer path between guest and host. h The energy levels of BPO and five guests.

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In our previous work, we found that the host could assist the excitons of the guests in energy transfer40,41,42. We, therefore, recorded the excitation spectra (fluorescence emission/420 nm) of guest MAPy in common solvents (toluene, THF, and N,N-dimethylformamide/DMF) and host BPO (molten state and crystal state). The results (Fig. 5d) show that the maximum excitation wavelength in MAPy emissions in these solvents is 346 nm, whereas the maximum excitation wavelengths in host emissions in the molten and crystalline states are red-shifted to 392 and 387 nm, respectively. The excitation spectra of the phosphorescence emission (660 nm) also show that the maximum excitation wavelengths in emissions from MAPy in these solvents are significantly longer than that of the crystalline host (Fig. 5e). Hence, we conclude that the host not only acts as the rigid matrix, but also changes the energy transfer process for the guest in the excited state. Furthermore, the phosphorescence lifetimes of guest molecules at 77 K are only between 12–23 ms (Fig. 5f), which are much shorter than that of the host matrix. This also shows that the host matrix prolongs the ISC process of the guest excitons.

From the above experimental results and our previous work40,41,42, we conjecture that the T1 of the host is the bridge between S1 and T1 of the guest (Fig. 5g), and hence the excited energy from the guest is transferred from S1 to T1 of the guest via the T1 path of the host. To verify this mechanism, density functional theory calculations were performed to obtain the singlet and triplet energy levels of the guests and host (Calculated the energy level of the host in the crystalline state). The energy range for the S1 and T1 states of the five guest molecules are 3.01–3.49 eV and 1.84–2.15 eV, respectively (Fig. 5h). The ΔEST of the guest molecules are in the range of 1.17–1.34 eV; such large energy gaps make excitonic ISC difficult. However, the band gaps between the S1 state of the guests and the T1 state of the host are only 0.11–0.59 eV (Fig. 5h), which is advantageous for excitonic ISC. Therefore, the synergy action for the guest–host system is also an important factor in the phosphorescence activity of guest–host materials.

Application studies in time-resolved bioimaging

Long-wavelength emissions are well-known to be beneficial in reducing tissue scattering and enhancing tissue penetration, and thus improve bioimaging quality. Encouraged by the excellent properties of these near-infrared RTP materials, an application to bioimaging was investigated. Because DMAPy/BPO among the materials studied exhibits the longest wavelength with a quite long lifetime, DMAPy/BPO and the biocompatible amphiphilic copolymer PEG-b-PPG-b-PEG (F127) were selected as nanoparticle (NP) cores and the encapsulation matrix, respectively. To ensure our DMAPy/BPO NPs were accessible in vivo with good RTP performance, a top-down method was employed to produce the NPs12,47. The phosphorescence wavelength of nanoparticles is almost the same as that in the solid-state (Supplementary Fig. 19a), but the phosphorescence lifetime is reduced to 70 ms (Supplementary Fig. 19b), and the phosphorescence quantum yield has also been reduced to 3.1%. This may be due to the small size of the nanoparticles causing the host matrix to not be able to coat the guest molecules well12,47. In addition, to study the morphology of the nanoparticles, the XRD curve of the nanoparticles obtained by suction filtration were tested, and the result showed that the nanoparticles have good crystallinity (Supplementary Fig. 20). To further verify the advantages of long-wavelength RTP materials, a short-wavelength (λPhos. = 520 nm) but strong intensity (ФPhos. = 64%) RTP material DOB/BPO reported in our previous work was selected as a control and DOB/BPO NPs were prepared by the same method48. Dynamic light scattering and transmission electron microscopy data indicated both DMAPy/BPO and DOB/BPO NPs formed a near-spherical morphology with a mean hydrodynamic diameter of ≈ 100 nm (Fig. 6a and Supplementary Fig. 21). Both kinds of NPs revealed strong resistance to photobleaching, indicative of little change in their intensities after eight cycles of stimulation or eighty minutes of 365-nm UV light irradiation (Fig. 6b and Supplementary Figs. 22,  23). We further verified the quantitative conversion of the phosphorescence intensity with NP concentrations. The phosphorescence intensities of DMAPy/BPO NPs and DOB/BPO NPs were captured at t = 10 s post-excitation, and possess good linearity with the NP concentration (Fig. 6c and Supplementary Fig. 24). DMAPy/BPO NPs and DOB/BPO NPs display the main phosphorescence signals (Fig. 6d) under Dsred (575–650 nm) and GFP (515–575 nm) filters, respectively. This result is consistent with their phosphorescence spectra.

Fig. 6: Phosphorescence properties of DMAPy/BPO and DOB/BPO nanoparticles.
figure 6

a Diameter distribution of DMAPy/BPO nanoparticles. Inset: transmission electron microscopy image, scale bar = 100 nm. b The normalized phosphorescence intensities of DMAPy/BPO NPs as a function of cycle number of UV light irradiation (n = 3). c The phosphorescence intensities as a function of the concentration of DMAPy/BPO NPs (n = 3). d Phosphorescence images of DMAPy/BPO and DOB/BPO NPs (4 mg mL−1) were captured through different filters. e Phosphorescence images of DMAPy/BPO and DOB/BPO NPs (10 mg mL−1) covered with different thicknesses of chicken tissue. f SBR ratios from coverings with different tissue thicknesses given in (e). g Cytotoxicities of DMAPy/BPO and DOB/BPO NPs against 4T1 cells. The 4T1 cells were incubated with DMAPy/BPO and DOB/BPO NPs at different concentrations for 8 h (n = 4). h Fold change plot of phosphorescence intensities of DMAPy/BPO NPs in various metal ions. Error bars: mean ± standard deviation (n = 3). Triple asterisks represent p < 0.01 compared with Na+. i Fold change plot of phosphorescence intensities for DMAPy/BPO NPs in different tissue homogenates. Error bars: mean ± standard deviation (n = 3). Triple asterisks represent p < 0.01 compared with PBS.

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As tissue penetration is a considerable challenge for in vivo bioimaging, tissue penetration depths of the NPs were compared between DMAPy/BPO NPs and DOB/BPO NPs. The phosphorescence signals of both DMAPy/BPO NPs and DOB/BPO NPs (Fig. 6e, f) decreased with the increasing thickness of chicken breast tissue. With the advantages of RTP materials, ultra-high SBR signals were observed without covering the chicken breast tissue. However, the inherent limit with short wavelengths leads to a relatively low tissue penetration (SBR = 5.4 at thickness 7.5 mm). In contrast, the NIR phosphorescence signal of the DMAPy/BPO NPs can still be detected (SBR = 15) under a 12.5-mm thick coverage of chicken breast tissue. This result revealed excellent deep tissue imaging from NIR emissions of NPs and moreover without excitation.

After we verified that both kinds of NPs had good cytocompatibility (Fig. 6g), we investigated the phosphorescent performance of DMAPy/BPO NPs in various metal ions (widespread in vivo) and tissue homogenates to confirm bioimaging feasibility in vivo. After 1 min-long irradiation using a 365-nm handheld UV lamp, the phosphorescence signals of DMAPy/BPO NPs incubated with different metal ions were recorded immediately under the same conditions using an IVIS bioimaging instrument. However, ferric ions (including Fe2+ and Fe3+) were found to quench the phosphorescence signals significantly compared with the signals in Na+ (Fig. 6h). This result might be attributed to the interaction between ferric ions with outer vacant orbitals and O/N heteroatoms with lone pair electrons in DMAPy/BPO NPs49 Furthermore, the DMAPy/BPO NPs were found to exhibit different phosphorescence quench behaviors in different tissue homogenates and blood (Fig. 6i). Compared with the phosphorescence signal in PBS, the signals of DMAPy/BPO NPs were significantly quenched in blood and blood-rich tissues (such as heart and liver) through the quenching of Fe2+ and Fe3+ ions, which would be beneficial when imaging tumors.

Applications in intravital phosphorescence imaging were investigated. The solutions of DMAPy/BPO NPs and DOB/BPO NPs were subcutaneously injected into Balb/c nude mice, followed by imaging with an IVIS instrument in bioluminescent mode after 1-min irradiation from the 365 nm handheld UV lamp. The images were captured 10 s after the removal of the light source. To ensure the biosafety of the UV irradiation procedure, the phosphorescence signals were activated by the handheld UV lamp at 10 mW cm−2 power density, which is below the maximum power exposure allowed for skin irradiation (18 mW cm−2)47. For comparison, fluorescence signals derived from DMAPy/BPO NPs and DOB/BPO NPs were also evaluated, simultaneously. The subcutaneous phosphorescence imaging result (Fig. 7a) in living mice reveals that both phosphorescent signals from DMAPy/BPO and DOB/BPO NPs can be observed at 10 s after excitation. The SBR of DMAPy/BPO NPs and DOB/BPO NPs subcutaneous phosphorescence imaging at 10 s are 160 and 75 (Fig. 7b), respectively. In contrast, the fluorescence signals of DMAPy/BPO NPs and DOB/BPO NPs were hardly distinguished from the tissue autofluorescence. We note that, although the skin thickness of mice is just ~0.5 mm, short-wavelength-emitting DOB/BPO NPs exhibit a lower SBR than DMAPy/BPO NPs in subcutaneous phosphorescence imaging because of scattering from skin tissue. These results are in accordance with Fig. 5e, f and also demonstrate that long-wavelength emissions from DMAPy/BPO can effectively decrease tissue scattering and provide high-quality phosphorescence bioimaging. The phosphorescence imaging of lymph nodes was further investigated because lymph-node labeling is clinically important in guiding tumor surgery. The phosphorescence signal (Fig. 7c, d) of the axillary lymph node is clearly evident (SBR = 55) whereas the fluorescence signal is not distinguishable. Thus, the lymph-node imaging confirms the effectiveness of DMAPy/BPO NPs for phosphorescence tissue imaging.

Fig. 7: Applications in intravital phosphorescence imaging.
figure 7

a Phosphorescence and fluorescence imaging of a mouse with the subcutaneous inclusions of DMAPy/BPO NPs and DOB/BPO NPs (4 mg mL−1). Circles indicate the locations of nanoparticle injection. b Signal to background ratio for phosphorescence and fluorescence imaging of subcutaneous injection in live mice. c Phosphorescence and fluorescence imaging of lymph nodes in mice 0.5 h after intradermal injection of DMAPy/BPO NPs (4 mg mL−1) into the forepaw of live mice. d Signal to background ratio for phosphorescence and fluorescence imaging of lymph nodes in live mice. e Phosphorescence and fluorescence imaging of live tumor-bearing mice 6 h after the injection of DMAPy/BPO NPs into the vein (4 mg mL−1). f Signal to background ratio for phosphorescence and fluorescence imaging of tumor in live mice. All error bars were based on standard deviation (n = 3).

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Precise identification of complicated diseases such as cancer cells for high-performance imaging. Encouraged by the good performance of lymph-node imaging, we evaluated the phosphorescence imaging capability in cancer diagnosis in vivo. To probe the feasibility of using long-wavelength RTP materials in such circumstances, the armpit tumor-bearing mice were prepared with 4T1 breast cancer cells. A solution of DMAPy/BPO NPs was injected through the tail vein into live mice. At 6 h post-injection, the signals of DMAPy/BPO NPs were activated by UV light for 1 min. Next, after removal of the UV lamp excitation, phosphorescence images were captured at 10 s using the IVIS instrument in the bioluminescence mode. Similarly, fluorescence imaging was recorded at the same time for comparison. The phosphorescence signal (Fig. 7e) clearly originates from the armpit tumor. Because the NIR phosphorescence emission involves no autofluorescence interference, the SBR for the phosphorescence guided armpit tumor imaging is as high as 43 (Fig. 7f).

The mice bearing armpit tumors were sacrificed, and the main tissues were excised for ex vivo phosphorescence imaging. Reticuloendothelial system organs are known to have enriched nanomaterials. Interestingly, only the liver displayed a low phosphorescence signal; in other main organs, almost no phosphorescence signal was observed (Supplementary Fig. 25). This result might be attributed to the phosphorescence signal being quenched by the liver because of its abundant blood supply, which is in accordance with an earlier result (Fig. 6i). Furthermore, tissues with phosphorescence signals were collected and stained with H&E (Supplementary Fig. 26), verifying the presence of an armpit tumor. The main organs were stained with H&E as well. Compared with the main organs of PBS pretreatment live mice, the DMAPy/BPO NPs did not cause obvious damage to these organs (Supplementary Fig. 27). This work confirmed that by avoiding autofluorescence interference and reducing the tissue scattering, RTP materials (DMAPy/BPO NPs) with both long-wavelength and long-lifetime properties can serve as potent probes for image-guided diagnosis.

Discussion

In conclusion, we provide a practical idea for the construction of organic RTP materials with NIR wavelength and ultralong lifetime: i.e., the guests should have sufficient conjugation to reduce the T1 level, and the host matrix assists the guest molecules in exciton transfer and inhibits the non-radiative transition. To the best of our knowledge, this is the first report on pure organic RTP materials with both long-wavelength (>700 nm) and ultralong lifetime (>100 ms) simultaneously. What’s more, we demonstrate for the first time that pure organic NIR phosphorescence is successfully used for in vivo bioimaging. This work also represents one of the very few examples among currently available pure organic RTP materials able to be competent for in-depth in vivo bioimaging via intravenous injection in an animal model.

Methods

Synthesis of guest compounds

The mixture of 1-bromopyrene or 1,6-dibromopyrene (10.0 mmol), boronic acid (12.0 or 24.0 mmol), Pd(PPh3)4 (5.0 mol%), and K2CO3 (5.0 mol%) were dissolved in THF (10.0 mL) and water (1.0 mL). The mixture was stirred for 12 h at 80 °C under a nitrogen atmosphere. The solvent was removed under reduced pressure and the residue were purified by column chromatography (petroleum ether: ethyl acetate = 1:100, v:v) to afford the pure MOPy/MAPy/DMOPy/DMAPy compounds.

Preparation of doped materials

Put the corresponding amount of host and guest together, and heat the mixture to 60 °C in an air atmosphere. After the guests are completely dissolved in the molten hosts, the mixed systems are cooled to room temperature, and the mixed systems are crystallized to obtain the doped materials. The doped materials with high guest–host molar ratios (1:10, 1:100, 1:100) are using a direct weighing method, while for guest–host molar ratio (1:10000) doped materials, we use the indirect dilution method.

Bioimaging measurement

The amphiphilic copolymer PEG-b-PPG-b-PEG (F127) was purchased from Aladdin Ltd. Fetal bovine serum (FBS) was provided by Thermo Fisher Scientific Inc. (Waltham, MA, USA). Transmission electron microscopy (TEM) images were acquired from a JEM-2010F transmission electron microscope with an accelerating voltage of 200 kV. Dynamic light scattering (DLS) was measured on a 90 plus particle size analyzer. In vitro and in vivo phosphorescence imaging was performed by the IVIS® Lumina II imaging system.

Preparation of nanoparticles

To 1 mL of the aqueous solution of F127 (10 mg), the DMAPy/BPO crystals (1 mg) were added. The mixture was then sonicated by a microtip-equipped probe sonicator (Branson, S-250D) for 10 min. The resultant suspension was filtered through a 0.45 μm syringe-driven filter to afford a solution of nanoparticles. And then the resultant solution was concentrated.

In vitro phosphorescent imaging of nanoparticles solutions

The phosphorescent intensities of DMAPy/BPO and DOB/BPO nanoparticles were recorded using IVIS® Lumina II imaging system at t = 10 s after each kind of nano solutions were irradiated by 365 nm handheld UV lamp (12 W) for 1 min. The IVIS system was set in bioluminescence mode with an open/GFP/Dsred filter setting (exposure time: 17 s).