Fluorescent turn-on probes based on a rhodamine spirolactam (RSL) structure have recently become a popular means of detecting pH, metal ions, and other analytes of interest. RSLs are colorless and non-fluorescent until the target analyte induces opening of the spirocyclic ring system, revealing the fully conjugated and highly fluorescent rhodamine dye. Among RSLs opened by acid, we have observed wide variation in the kinetics of the fluorescence turn-on process such that some probes would not be usable in situations where a rapid reading is desired or the pH fluctuates temporally. Herein we present a systematic investigation of the fluorescence turn-on kinetics of RSLs to probe the hypothesis that the reaction rates are influenced by the electronic properties of the spirolactam ring system. A series of 8 aniline-derived RSLs with para substituents ranging from electron-donating to electron-withdrawing was prepared from rhodamine B. The fluorescence turn-on rates are observed to increase by a factor of four as the substituent is tuned from methoxy to nitro. This effect is explained in terms of the destabilization of the reaction intermediate by the substituent. As the reaction rates increase across the series, a concomitant increase in fluorescence intensity is also observed. This result is attributed to an increase in the concentration of the fluorescent form of the dye and is consistent with the expected equilibrium properties of this system. These findings are applied to the design of a faster-reacting and more intensely fluorescent RSL pH probe.
Rhodamine spirolactams (RSLs) have recently emerged as popular fluorescent pH probes due to their fluorescence turn-on capability and ease of functionalization at the spirolactam nitrogen. Design of RSLs is often driven by biological targeting or compatibility concerns, rather than the pH sensitivity of the probe, and the relationship between RSL structure and pK is not well understood. To elucidate the relationship between pK values and the properties of substituents attached to the spirolactam nitrogen, a series of 19 aniline-derived RSLs is presented. RSLs derived from di-ortho-substituted anilines exhibit pK tunability across the moderately acidic region (ca. pH 4-6). Evaluation of pK data using the Fujita-Nishioka model for ortho substituent effects reveals that both steric and electronic substituent properties influence RSL pH responsiveness, with pK values increasing as substituent size and electron withdrawing character increase. These trends are attributed to changes in the RSL structure induced by large substituents, and to electronic influences on the protonated spirocyclic reaction intermediate. To demonstrate the practical applicability of these probes in completely aqueous environments, RSL-doped conjugated polymer nanoparticles that exhibit a ratiometric fluorescence response to changing pH levels are presented.
Resonantly enhanced second harmonic generation (SHG) spectra of Coumarin 152 (C152) adsorbed at the water-silica interface show that C152 experiences a local dielectric environment slightly more polar than that of bulk water. This result stands in contrast to recently reported time-resolved fluorescence experiments and simulations that suggest an alkane-like permittivity for interfacial water at strongly associating, hydrophilic solid surfaces. Taken together, these results imply that while the static electric field across the aqueous-silica interface may be large, restricted water dynamics lead to apparent nonpolar solvation behavior similar to that experienced by solutes in confinement. Resonance-enhanced SHG spectra and time-resolved fluorescence of C152 adsorbed to aqueous-hydrophobic silica surfaces show that when water’s ability to hydrogen bond with the silica surface is eliminated, a solute’s interfacial solvation and corresponding ability to photoisomerize converge to an intermediate limit similar to that experienced in bulk acetone or methanol. While water structure and dynamics at solid-liquid interfaces have received considerable attention, results presented below show how strong solvent-substrate interactions can create conflicting pictures of solute reactivity across buried interfaces.
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