Open Access Article
Keqian Zoua,
Rongrong Hea,
Lizhong Zenga,
Yujia Liu
b,
Zheng Xua,
Masafumi Unno
*b,
Liwen Xu
*a and
Zhanjiang Zheng
*a
aCollege of Material, Chemistry and Chemical Engineering, Key Laboratory of Organosilicon Chemistry and Material Technology, Ministry of Education, Zhejiang Key Laboratory of Organosilicon Material Technology, Hangzhou Normal University, Hangzhou, 311121, China. E-mail: liwenxu@hznu.edu.cn; zzjiang78@hznu.edu.cn
bDepartment of Chemistry and Chemical Biology, Graduate School of Science and Technology, Gunma University, Kiryu 376-8515, Japan. E-mail: unno@gunma-u.ac.jp
First published on 30th March 2026
In this study, we synthesized two novel vinyl-substituted, BINOL-hybridized tricyclic-ladder-type siloxanes (referred to as Vi-TLS-BINOLs) via a B(C6F5)3-catalyzed Piers–Rubinsztajn reaction. Fluorescence studies of the Vi-TLS-BINOLs revealed enhanced fluorescence emission attributed to the restricted intramolecular motion by the ladder-type structure. In comparison to the precursor BINOL, Vi-TLS-BINOLs L1 and L2 exhibit a 5.2-fold and 4.8-fold increase in fluorescence quantum yield in THF, respectively. Furthermore, it was observed that both Vi-TLS-BINOLs could selectively recognize Fe3+ through fluorescence quenching. ESI-HRMS analysis confirmed the formation of [L1 + 2Fe] and [L1 + 3Fe] complexes with Fe3+. The detection limits for Fe3+ were determined to be 10.6 µM and 16.3 µM, respectively.
Iron is a vital metal found on Earth that is essential for the majority of life forms and human health. It is a key component of proteins and enzymes vital for sustaining good health, playing an important role in oxygen metabolism, oxygen transportation, and electron transfer.12–14 An imbalance in Fe3+ levels can significantly impart metabolism and cell homeostasis, leading to a variety of diseases including anemia, chronic renal disease, and hemochromatosis.12–14 To address this issue, various techniques have been developed for the detection of iron ions, with fluorescence spectroscopy being particularly effective for its high sensitivity, selectivity, and cost-effectiveness.15–18 However, the preparation of these sensors is laborious and requires complex procedures.19–24 Therefore, the design and synthesis of novel and easily-accessible sensors remains a challenge.
1,1′-Binaphthalene-2,2′-diol (BINOL) and its derivatives, which are characterized by biaryl compounds exhibiting axial chirality and two active phenolic hydroxyl groups, as well as being easily modifiable, have attracted significant attention in fluorescence-based molecular recognition.25–30 In connecting with our continuing research on chemosensors utilizing the BINOL fluorophore,10,11,31–33 we report herein two novel vinyl-substituted, tricyclic-ladder-type siloxanes hybridized with BINOL (Vi-TLS-BINOLs), prepared via the Piers–Rubinsztajn reaction (Scheme 1). Their distinctive structure comprises a central siloxane ring and two side rings, each containing five oxygens. This unique structure suggests the potential for accommodating metal ions through a “host–guest” recognition process within their macrocyclic cavities. Further Fluorescence spectroscopy study showed that Vi-TLS-BINOLs possess the capability to selectively recognize iron ions through a quenching process.
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| Scheme 1 Synthesis of the new vinyl substituted BINOL-hybrided tricyclic ladder-type siloxanes L1 and L2. | ||
The hybridized ladder-type siloxanes L1 and L2 were fully characterized using 1H, 13C, 29Si NMR, and HRMS-ESI. The 1HNMR data of L1 (see Fig. S13) confirmed the complete functionalization of Si–H groups, as evidenced by the absence of resonances for Si–H groups (4.74 ppm) from the precursor [ViSi(OSiMe2H)O]4. Signals ranging from 5.09 to 6.14 ppm corresponding to the vinyl groups, and four singlet signals (−0.22, −0.18, 0.23, 0.31 ppm) of the methyl protons of Si–(CH3)2 were observed, attributed to the axial chirality of the BINOL and the constrained rotation of (Me2)Si–O bonds from the cyclic structure of L1. The 13C NMR spectrum of L1 (see Fig. S14) displayed four characteristic signals at −0.06, 0.01, 0.30, and 0.77 ppm corresponding to the carbon of Si–(CH3)2. The 29Si NMR (see Fig. 1) analysis of L1 showed two sets of signals, attributed to the T-unit silicon atoms (Si in blue, −80.83 and −81.23 ppm) and D-unit silicon atoms (Si in red, −12.28 and −12.62 ppm), respectively. HRMS-ESI mass spectroscopy was utilized to characterize compound L1 further. The results aligned with the calculated mass of ([M + Na]+ calcd for C56H60NaO12Si8: 1171.2137; found: 1171.2125). Additionally, the isotopic distribution pattern on the mass spectrum matched the calculated pattern well (refer to Fig. S9).
The UV absorption bands observed in the ladder hybridized molecule are ascribed to the transitions of the binaphthyl rings (See Fig. 2a), specifically the 1Bb transition occurring between 230 and 250 nm, the 1La transition spanning from 250 to 300 nm, and the 1Lb transition ranging from 300 to 350 nm. As shown in Fig. 2b, the fluorescence spectra (λex = 260 nm) of L1 and L2 in THF solution displayed emission bands at 355 and 359 nm respectively. Their quantum yields (ΦF, see Table 1) in THF (1.0 × 10−5 M) were found to be 11.9% and 11.1% respectively. These values are significantly higher than the quantum yield of the precursor BINOL (2.3%). Furthermore, in their powder forms, L1 and L2 exhibited drastically increased fluorescence (ΦF = 41.3% and 20.4% respectively), which remain higher than that of the solid precursor BINOL (13.7%). The enhanced fluorescence of L1 and L2 is proposed to result from the restriction of intramolecular motion induced by the ladder-type structure. This structure effectively immobilizes the BINOL chromophores within the ladder skeleton, thereby inhibiting non-radiative processes.38,39 Consequently, this phenomenon is referred to as ladderization-induced emission enhancement (LIEE), which is conceptually grounded in the well-established principle of restriction of intramolecular motion (RIM).40 In many flexible fluorophores, excited-state energy is readily dissipated through non-radiative channels such as torsional rotations and other vibrational modes.41 By covalently locking the BINOL units into a rigid ladder architecture at the single-molecule level, these non-radiative decay pathways are effectively minimized. This strategy is distinct from, yet complementary to, the widely studied phenomenon of aggregation-induced emission (AIE). In AIE systems, emission is activated by the formation of intermolecular aggregates in poor solvents or the solid state, which physically hinders intramolecular rotations. In contrast, LIEE achieves this restriction at the single-molecule level through robust covalent bonds. Consequently, L1 and L2 are already significantly more emissive than their precursor in dilute solution.
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| Fig. 2 (a) UV absorption spectra of compound L1-L2 in 10 µM THF; (b) fluorescence emission spectra (λex = 260 nm) of compound L1-L2 in 10 µM THF. | ||
| R-BINOL | Ladder L1 | Ladder L2 | |
|---|---|---|---|
| ΦF (%) (solid) | 13.7 | 41.3 | 20.4 |
| ΦF (%) (in THF) | 2.3 | 11.9 | 11.1 |
The recognition ability of compound L1 towards perchlorate salts of various metals (Fe3+, Ag+, Al3+, Ca2+, Cd2+, Cu2+, K+, Li+, Mn2+, Na+, NH4+, Pb2+, Zn2+) was investigated using fluorescence spectroscopy in THF solutions (λex = 260 nm, see Fig. 3). Addition of 50 equivalents of each metal revealed that Fe3+ significantly reduced fluorescence intensity at 355 nm, Cu2+ caused half quenching, while other metal ions had slight impact on fluorescence emission. Further experiments showed that 50 equivalents of Fe3+ led to up to 99% quenching in MeOH, compared to 93% quenching in THF. Subsequent fluorescence titration experiments in MeOH demonstrated a incremental reduction in fluorescence intensity at 355 nm with increasing Fe3+ concentrations, as shown in Fig. 4. The quenching response was analyzed using a Stern–Volmer plot (see Fig. S3), with the equation F0/F = Ksv[Q] + 1, where F0 and F represent fluorescence intensity in the absence and presence of Fe3+, respectively, and [Q] is the molar concentration of quencher Fe3+. This analysis yielded a calculated quenching constant (Ksv) of 2.2 × 104. The Ksv value for compound L2 was determined to be 2.8 × 104 similarly. The high Ksv values, along with the nonlinear behavior observed, suggest the formation of a non-fluorescent complex in the ground state, likely due to the oxygen atoms' capability to coordinate with iron ions, resulting in fluorescence quenching.42,43 Furthermore, the fluorescence response of L1 to Fe3+ was assessed in solutions buffered at pH 4, 7, and 10 to determine the impact of pH on sensing performance (see Fig. S11). Addition of 15 equivalents of Fe3+ resulted in largely consistent fluorescence intensities across the pH range tested. Complete fluorescence quenching occurred with 40 equivalents of Fe3+, regardless of the pH of the solution. Sensor L2 exhibited a similar response pattern (Fig. S12), suggesting limited influence of pH on the sensing capabilities of these two sensors.
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| Fig. 3 Fluorescence emission data (λex = 260 nm) of compound L1 with the addition of various metal ions (50 equivalents) in 10 µM THF, and iron ions (50 equivalents, Fe3+(#)) in 10 µM MeOH. | ||
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| Fig. 4 Fluorescence emission spectra (λex = 260 nm) of compound L1 (10 µM) in MeOH with the increasing concentration of Fe3+, inset displays a Stern–Volmer plot of L1 upon addition of Fe3+ in MeOH. | ||
In the investigation of the Fe3+ calibration curve for compound L1, a linear relationship was examined within the concentration range of 0–200 µM in Fig. S5. Through meticulous data processing and statistical analysis, a highly linear calibration curve was established with a correlation coefficient (R2) of 0.96, indicating a robust degree of data fitting. The detection limit was determined utilizing the standard 3σ/K method, involving the calculation of the standard deviation σ from 10 blank tests and the utilization of the calibration curve's gradient K, resulting in a Fe3+ detection limit of 10.6 µM. For compound L2, the same approach was employed, yielding a Fe3+ detection limit of 16.3 µM as inferred from the data analysis presented in Fig. S6. Both compounds demonstrated comparable detection performance (Table S1), affirming the reliability and precision of the developed methodology.
Competitive metal binding experiments in MeOH were conducted to assess the selectivity of compound L1 for Fe3+ ions amidst a complex mixture of potentially interfering species, including Ag+, Al3+, Ca2+, Cd2+, Cu2+, K+, Li+, Mn2+, Na+, NH4+, Pb2+, Zn2+ (30 equiv.) (Fig. 5). Analysis of the fluorescence intensity depicted in Fig. 5 revealed no significant changes when comparing the profiles with and without the presence of other metal ions. Notably, only K+ exhibited a minor impact on the quenching process, indicating the high selectivity of compound L1 for Fe3+ ions. Furthermore, parallel competitive binding experiments conducted with L2 across diverse interfering metals demonstrated a similarly reliable sensing capability (Fig. S7), thereby confirming the robustness of this sensor design.
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| Fig. 5 Fluorescent emission responses of L1 (2.5 µM) with different perchlorate salts of metal ions (30 equiv.) in the presence or absence of Fe3+ (30 equiv.) in MeOH. | ||
The structure of the BINOL-hybridized compound L1 was optimized to investigate its properties. The HOMO/LUMO molecular orbitals were calculated using the Gaussian 03 program at the B3LYP/6-31G(d,p) level (refer to Fig. 6). The electron densities of the HOMO in compound L1 were observed to be distributed along the binaphthyl rings and oxygen atoms, creating an electron cloud cavity capable of encapsulating iron ions during the recognition process. To further elucidate the interaction between L1 and iron ions, ESI-MS analysis was performed on a mixture of Fe3+ and ladder-type siloxane L1 in methanol (refer to Fig. S8). The ion peaks detected at m/z 1261.0900 and 1317.0468 correspond to [L1 + 2Fe] and [L1 + 3Fe] complexes, indicating the formation of complexes between Fe3+ and ladder-type siloxane L1 at molar ratios of 2
:
1 and 3
:
1, respectively. These results suggest that ladder-type siloxane L1 chelates with iron ions through the oxygens of BINOL and T4-siloxane, leading to the formation of cavity-captured complexes with stoichiometries of 2
:
1 or 3
:
1. This nonfluorescent complex is believed to be responsible for the observed decrease in fluorescence intensity, where the electrons in the excited state will transfer to the half-filled 3d orbitals of the paramagnetic Fe3+, leading to the fluorescence quenching of ladder-Fe3+ complex with the nonradiative electronehole annihilation.44
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| Fig. 6 The shape and energy of the HOMO and LUMO orbitals of compound L1 calculated at the DFT level using a B3LYP/6-31G(d,p) basis set. | ||
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