To improve the sensitivity of LET-1055 to H
2S, we strategically designed a FRET platform, where LET-1055 with H
2S-quenched property acted as an energy acceptor, and the Rh930 with maximum absorbance/emission of 890/930 nm displayed as an energy donor (Fig.
3A), because of its sufficient overlap in absorbance/emission bands between these 2 emitters and excellent inertia toward H
2S (Fig. S8). Therefore, Rh930 can not only be a credible energy donor to LET-1055, but also resist the targeted signal interference, ensuring the accuracy of H
2S detection. Afterward, we constructed FRHS via amphiphilic 1,2-distearoyl-sn-glycero-3-phosphoethanolamine-
N-[methoxy (polyethylene glycol)-2000] (DSPE-PEG
2000)-assisted encapsulation of Rh930 and LET-1055 with a molar ratio of 1:2.5 (Rh930:LET-1055) [
52]. Obviously, the as-prepared FRHS displayed the characteristic absorption/emission bands of Rh930 and LET-1055 (Fig.
3A and Fig. S9). The transmission electron microscopy (TEM) image showed that FRHS was dominated by spherical morphology with an average size of about 100 nm (Fig.
3B). The size distribution of FRHS was also evaluated by dynamic light scattering (DLS) (Fig.
3C). As a result, the hydrodynamic diameter of FRHS was about 170 nm, which is larger than that of TEM measurement. The size difference may be attributed to the DSPE-PEG
2000 coating layer and the shrinking of the FRHS during the dryness process of TEM sample preparation. Subsequently, we evaluated the sensitivity and specificity of FRHS toward H
2S. As shown in Fig.
3D, with the addition of S
2−, the NIR-II FL intensity of FRHS was enhanced at 930 nm (FL
930) and decreased at 1,060 nm (FL
1060), yielding a good linear correlation between FL
930/FL
1060 intensities and S
2− concentrations from 0 to 20 μM (Fig.
3E). The LOD for S
2− was calculated to be 96 nM, which was lower than that in healthy tissues [
45], thus enabling us to monitor H
2S level in pathological tissues. Furthermore, the time-dependent reaction kinetics of FRHS with S
2− indicated that the FRHS also held fast reaction kinetics toward S
2− (Fig.
3F and Fig. S10), akin to the sole LET-1055. Encouraged by the above results, we applied NIR-II FL imaging to visualize the aforementioned FRET process. Obviously, the NIR-II FL intensity of channel 2 (Ch.2, 1,000 to 1,700 nm, filter: long-pass [LP] 1,100 nm) exhibited continuous decrease behavior for FRHS during incubation with S
2− solution, while the signals in channel 1 (Ch.1, 900 to 1,000 nm, filters: short-pass [SP] 1,000 nm and LP 900 nm) showed an opposite tendency. Thus, the ratiometric NIR-II FL imaging was delineated by the ratio of 2 channels (denoted as Ch.1/Ch.2) (Fig.
3G), showing a distinct FL signal enhancement. Combined with the excellent selectivity of FRHS for S
2− (Fig.
3H and I and Fig. S11), the S
2−-induced ratiometric NIR-II FL imaging by FRHS possessed great potential for H
2S detection.