Effect of Proton Substitution by Alkali Ions on the Fluorescence Emission of Rhodamine B Cations in the Gas Phase

Freezing Conformers for Gas-Phase Förster Resonance Energy Transfer

Various techniques are available to illuminate geometric structures of molecular ions in gas phase, such as Förster Resonance Energy Transfer (FRET) informing on distances between two dyes covalently attached to a molecule. Typically, cationic rhodamines, which absorb and emit visible light, are used for labeling. Extensive work has revealed that the transition energy of a rhodamine is intricately linked to its nearby microenvironment, with nearby charges causing Stark-shifted emission. This occurs because the inter-dye Coulomb interaction is weaker in the excited state (S1) than in the ground state (S0) due to the increase in polarizability upon excitation. Therefore, absorption and emission spectra, along with FRET efficiencies, provide insights into structural motifs. At room temperature, multiple conformers often co-exist, leading to overlapping absorption bands among different conformers and broad spectra. To study specific conformers, it is necessary to isolate them, for example, using ion-mobility spectrometry. Another approach is to reduce temperature, which results in spectral narrowing and distinct absorption bands, allowing for the selection of specific conformers through selective excitation. Here, we describe the instrumentation used for cryogenically cold FRET experiments and discuss recent results for small model systems, as well as future directions for a technique still in its infancy.

Vibrationally Resolved Absorption, Fluorescence, and Preresonance Raman Spectroscopy of Isolated Pyronin Y Cation at 5 K

Exploring how charge-changing affects the photoluminescence of small organic dyes presents challenges. Here, helium tagging photodissociation (PD) action spectroscopy in the gas phase and dispersed laser-induced fluorescence (DF) spectroscopy in the solid Ne matrix are used to compare the intrinsic photophysical properties of pyronin Y cation [PY]+ and its one electron-reduced neutral radical [PY]• at 5 K. Whereas the cation shows efficient visible photoluminescence, no emission from the neutral, in line with theoretical predictions, was detected. B3LYP/aug-cc-pVDZ calculations based on the TD-DFT/FCHT method allow for unambiguous assignment of recorded vibrationally resolved absorption and emission spectra. Surprisingly, our experimental sensitivity was high enough to also observe electronic preresonance Raman (ePR-Raman) spectra of [PY]+, with a significant efficiency factor (EF). These characteristics of the [PY]•/[PY]+ pair suggest that appropriately functionalized derivatives may open new perspectives in the area of in vivo bioimagining microscopy and find applications in various sophisticated stimulated-Raman spectroscopies.

A new setup for low-temperature gas-phase ion fluorescence spectroscopy

Here, we present a new instrument named LUNA2 (LUminescence iNstrument in Aarhus 2), which is purpose-built to measure dispersed fluorescence spectra of gaseous ions produced by electrospray ionization and cooled to low temperatures (<100 K). LUNA2 is, as an earlier room-temperature setup (LUNA), optimized for a high collection efficiency of photons and includes improvements based on our operational experience with LUNA. The fluorescence cell is a cylindrical Paul trap made of copper with a hole in the ring electrode to permit laser light to interact with the trapped ions, and one end-cap electrode is a mesh grid combined with an aspheric condenser lens. The entrance and exit electrodes are both in physical contact with the liquid-nitrogen cooling unit to reduce cooling times. Mass selection is done in a two-step scheme where, first, high-mass ions are ejected followed by low-mass ions according to the Mathieu stability region. This scheme may provide a higher mass resolution than when only one DC voltage is used. Ions are irradiated by visible light delivered from a nanosecond 20-Hz pulsed laser, and dispersed fluorescence is measured with a spectrometer combined with an iCCD camera that allows intensification of the signal for a short time interval. LUNA2 contains an additional Paul trap that can be used for mass selection before ions enter the fluorescence cell, which potentially is relevant to diminishing RF heating in the cold trap. Successful operation of the setup is demonstrated from experiments with rhodamine dyes and oxazine-4, and spectral changes with temperature are identified.

Gas-phase action and fluorescence spectroscopy of mass-selected fluorescein monoanions and two derivatives

Gaseous fluorescein monoanions are weakly fluorescent; they display a broad fluorescence spectrum and a large Stokes shift. This contrasts with the situation in aqueous solution. One explanation of the intriguing behavior in vacuo is based on internal proton transfer from the pendant carboxyphenyl group to one of the xanthene oxygens in the excited state; another that rotation of the carboxyphenyl group relative to the xanthene leads to a partial charge transfer from one chromophore (xanthene) to the other (carboxyphenyl) when the π orbitals start to overlap. To shed light on the mechanism at play, we synthesized two fluorescein derivatives where the carboxylic acid group is replaced with either an ester or a tertiary amide functionality and explored their gas-phase ion fluorescence using the home-built LUminescence iNstrument in Aarhus (LUNA) setup. Results on the fluorescein methyl ester that has no acidic proton clearly disprove the former explanation: The spectrum remains broad, and the band center (at 605 nm) is shifted even more to the red than that of fluorescein (590 nm). Experiments on the other variant that contains a piperidino amide are also in favor of the second explanation as here the piperidino already causes the dihedral angle between the planes defining the xanthene and the benzene ring to be less than 90° in the ground state (i.e., 63°), according to density functional theory calculations. As a result of the closer similarity between the ground-state and excited-state structures, the fluorescence spectrum is narrower than those of the other two ions, and the band maximum is further to the blue (575 nm). In accordance with a more delocalized ground state of the amide derivative, action spectra associated with photoinduced dissociation recorded at another setup show that the absorption-band maximum for the amide derivative is redshifted compared to that of fluorescein (538 nm vs. 525 nm).

Luminescence spectroscopy of oxazine dye cations isolated in vacuo

Gas-phase luminescence spectroscopy reveals transition energies of oxazine dye cations with no disturbance from counter ions or solvent molecules.

Absorption and luminescence spectroscopy of mass-selected flavin adenine dinucleotide mono-anions

We report the absorption profile of isolated Flavin Adenine Dinucleotide (FAD) mono-anions recorded using photo-induced dissociation action spectroscopy. In this charge state, one of the phosphoric acid groups is deprotonated and the chromophore itself is in its neutral oxidized state. These measurements cover the first four optical transitions of FAD with excitation energies from 2.3 to 6.0 eV (210-550 nm). The S₀ → S₂ transition is strongly blue shifted relative to aqueous solution, supporting the view that this transition has a significant charge-transfer character. The remaining bands are close to their solution-phase positions. This confirms that the large discrepancy between quantum chemical calculations of vertical transition energies and solution-phase band maxima cannot be explained by solvent effects. We also report the luminescence spectrum of FAD mono-anions in vacuo. The gas-phase Stokes shift for S₁ is 3000 cm^-1, which is considerably larger than any previously reported for other molecular ions and consistent with a significant displacement of the ground and excited state potential energy surfaces. Consideration of the vibronic structure is thus essential for simulating the absorption and luminescence spectra of flavins.

Luminescence spectroscopy of chalcogen substituted rhodamine cations in vacuo

A library of fluorescent rhodamine cations has been characterized with view to their potential use in gas-phase structural biology experiments.

Sibling rivalry: intrinsic luminescence from two xanthene dye monoanions, resorufin and fluorescein, provides evidence for excited-state proton transfer in the latter

Excited-state proton transfer in gas-phase fluorescein monoanions results in a broad, featureless emission band and a large Stokes shift compared to resorufin, which shares the same xanthene core structure.