Electronic and vibrational spectroscopy of cold protonated amino acids in the gas phase

In this thesis report, we describe a novel home-built instrument designed to study the spectroscopy of biomolecular ions in the gas phase and at low temperature, and we present the first experimental results obtained on protonated aromatic amino acids. The apparatus consists in a tandem mass spectrometer equipped with a nanospray ion source and a cryocooled 22-pole ion trap. The charged species produced by the source traverse a first quadrupole mass filter and mass-selected ions are then accumulated and thermalized in the ion trap, where their vibrational temperature can be lowered to ~ 10 K. Two setups allow us to generate ultraviolet and infrared laser light to spectroscopically probe the trapped ions by photodissociation. The resulting fragment ions are finally released from the trap and mass analyzed by a second quadrupole spectrometer. Photodissociation electronic spectra have been measured for the protonated amino acids tryptophan (TrpH+) and tyrosine (TyrH+), as well as for hydrated complexes of the former. The spectrum of TyrH+ exhibits sharp, fully resolved vibronic transitions, which attests to the low temperature of the ions. In contrast, that of tryptophan shows a broad absorption band that covers several hundreds of wavenumbers. This has been attributed to lifetime broadening related to an ultrafast (< ~ 100 fs) deactivation mechanism of the TrpH+ S1(ππ*) excited state. This phenomenon is caused by a strong coupling between this ππ* state and a nearby dissociative state of πσ* character mainly localized on the charged ammonium group. Solvation of TrpH+ by only two water molecules is sufficient to significantly destabilize the σ* orbitals and reduce that coupling, which results in a longer excited-state lifetime and a fully resolved electronic spectrum. These interpretations are supported by ab initio and density functional theory (DFT) calculations. Infrared-ultraviolet double resonance spectroscopic techniques have been successfully implemented to identify the different conformers of TyrH+ and doubly hydrated protonated tryptophan (TrpH+·W2) by measuring conformer-specific vibrational and electronic spectra for each of them. By comparison with the results of DFT geometry and harmonic frequency calculations, we could confidently determine the structures of the TyrH+ conformers and suggest possible assignments for those of TrpH+·W2. Two important stabilizing interactions could be inferred from these results: (i) the attraction between the charged ammonium group and the π-electron cloud of the aromatic ring; (ii) the hydrogen-bonding interaction of a donor water molecule to the acceptor indole ring of TrpH+·W2.

A new tandem mass spectrometer for photofragment spectroscopy of cold, gas-phase molecular ions

Ulrich Lorenz, Thomas Rizzo, Annette Svendsen

We present here the design of a new tandem mass spectrometer that combines an electrospray ion source with a cryogenically cooled ion trap for spectroscopic studies of cold, gas-phase ions. The ability to generate large ions in the gas phase without fragmentation, cool them to ~10 K in an ion trap and perform photofragment spectroscopy opens up new possibilities for spectroscopic characterization of large biomolecular ions. The incorporation of an ion funnel, together with a number of small enhancements, significantly improves the sensitivity, signal stability and ease of use compared with the previous instrument built in our laboratory.

American Institute of Physics2010

Influence of the protein environment on spectroscopy and ultrafast dynamics of retinal in bacteriorhodopsin

Selma Schenkl

The environment is important for the exact course of a chemical reaction. As an example of the strong influence of the environment on the reaction, this work studies the isomerization reaction of the chromophore retinal in the binding pocket of the protein bacteriorhodopsin. Three selected distance scales with reference to the chromophore are addressed: The distant protein surface at a length scale of 3-5 nm, the fuzzy environment of the binding pocket (1-2 nm) and the immediate neighborhood represented by the amino acid tryptophan Trp86 (5 Å). First, static absorption and fluorescence spectroscopies are applied to three dimensionally crystallized bacteriorhodopsin. An especially adapted set-up was developed for each task. The analysis of data is carried out in comparison with the measured spectra of the native protein membrane in solution. While the absorption spectrum shows a broadening on the high-energy side, the fluorescence spectrum deviates in the general shape of that measured in solution. The synoptic analysis of all spectra reveals the existence of three spectroscopically distinct species in the crystal: BR490 (absorption maximum at 490 nm) with a relative contribution of 28%, BR570 (native spectrum of solution, 68%), and BR610 ("blue membrane", 4%). BR490 appears particularly in the additional fluorescence band at 550 nm and is assigned to the dehydrated species of bacteriorhodopsin. The presence of that particular species indicates the suppression of rehydration in a partially dehydrated crystal and shows that the three dimensional arrangement hinders water diffusion. A simple model, close domains are assumed to form, eventually suppressing free water diffusion in a crystal. The lack of water on the protein surface modifies the protonation states of the amino acids in the binding pocket and therefore the optical properties of the retinal. The chromophore actually reacts on the alteration of its distant environment upon incorporation in the protein crystal. The second distance scale - the fuzzy environment - is addressed by a time-integrated fluorescence spectroscopy on native bacteriorhodopsin as function of the excitation wavelength (430 nm to 650 nm). The optimized experimental set-up guaranteed that the fluorescence of only the excited state I460 contributed. The measured spectra show maxima at 740 nm, and exhibit a Stokes shift of 5000 cm-1, independent of the excitation wavelength. The similarity of the fluorescence excitation spectrum with the spectrum of absorbed photons excludes energy-dependent loss channels. However, the spectra show a growing asymmetric broadening on the high-energy side with decreasing excitation wavelength. The additional fluorescence originates from vibrational hot states, also supported by the decomposition by Gaussian functions. A comparison with the fluorescence spectrum of blue membranes shows that the low-energy part also arises from vibrational hot states. Consequently, the first fast intramolecular vibrational energy relaxation does not entirely distribute the access-energy to other modes. The remaining energy is found in a quasi-static occupation of vibrational modes. The subsequent second vibrational relaxation — probably not only involving the retinal but also the protein — takes place on a time scale similar to that of the isomerization. The fast isomerization reaction prevents dissipation of energy relaxation of the excited state of the retinal into the protein environment. On a third distance scale, femtosecond spectroscopy in the UV offers a direct view into the electrostatic interaction of the chromophore with its immediate neighborhood. For the first time, the retinal isomerization was studied within the spectral window of the tryptophan absorption from 265 nm to 310 nm. For this, a set-up adapted to UV wavelengths was realized, basing on non-linear optics. The developed single-shot detection system yields a sensitivity of 10-5 in optical density. In the transient absorption measurements, a time resolution of 90 fs was achieved. At short probe wavelengths (265 nm - 294 nm), the measured transients show first a fast reduction of the absorption which subsequently recovers on three time scales (380 fs, 3 ps, > 16 ps). With increasing probe wavelength an induced transient absorption becomes dominant (282 nm - 294 nm). It has a rise time of 280 fs, and decays with a time constant of 4.3 ps. With further increasing probe wavelength the absorption signal decays faster. In response to the complex signature of the transients, an iterative and model-independent transient-decomposition is introduced. A set of three basis elements were identified: one bleach, and two absorption transients. The two induced absorption transients are assigned to retinal. The dynamics of the excited state (I460) in the first retinal-transient is described by two time constants (280 fs and 1 ps). The fast time constant leads to the photoproduct, while the slower one leads back to the ground state, presumably by internal conversion. The 250 fs delayed onset of the second transient (photo-intermediate J) is connected to a wave packet motion in the excited state. This delayed onset of the transient was observed for the first time. It demands a rise time of the J photo-intermediate of only 280 fs. This contrasts common estimates of 500 fs given in literature. For the first time, the temporal behavior of the permanent dipole moment of retinal is observed experimentally. Its evolution is imprinted in the dominant bleach feature (265 nm - 294 nm), originating from tryptophan Trp86. In the excited state, the permanent dipole moment increases strongly within the first 250 fs, and decays exponentially afterwards, following the formation of the photoproduct. However, the related time constant of 380 fs is slightly greater than that of 280 fs of the photoproduct J. This discrepancy may indicate a remaining long-lived polarization of the binding pocket. In brief, by using the intrinsic tryptophan as a probe, the local evolution of the electric field during the isomerization reaction was investigated. Indeed the isomerization reaction is reflected in the immediate environment. The variety of optical spectroscopy provides methods especially adapted for studying the influences of the environment on a chemical reaction. The results achieved here highlight the importance of these influences.

EPFL2004

Infrared photofragment spectroscopy of charged amino acid water clusters in the gas phase

Anthi Kamariotou

We present in this work a new technique, which combines laser photofragmentation spectroscopy with tandem mass spectrometry, for structural investigations of biomolecular ions in the gas phase. A novel apparatus was designed and built for the implementation of these studies. In this instrument closed shell ions are produced in the gas phase by electrospray ionization and stored in a hexapole ion trap prior to mass selection of a parent beam in a first quadrupole and then irradiation in an octupole ion guide using laser light. Mass analysis of the photofragmentaion products in a final stage quadrupole as a function of the wavelength generates an action spectrum. We applied this new technique to follow the microsolvation of charged amino acids in the gas phase. In these studies, the nanoelectrospray ionization source generates a distribution of water clusters of charged amino acids at various hydration levels. A particular size of cluster is selected and irradiated by infrared laser pulses resulting in the dissociation of one water molecule. Detection of the photofragmentation of this weak non-covalent bond allows us to generate the vibrational action spectrum of this particular cluster. We use a two-stage difference frequency mixing setup to produce laser light in the 2900–3800 cm-1, allowing us to probe the light-atom stretching region. IR photofragmentation spectra have been obtained for the hydrates of protonated and lithiated valine and those of protonated tryptophan. By probing the region of free and hydrogen-bonded N-H and O-H stretch vibrations and with the help of density functional theory calculations at the B3LYP/6-31++G** level, we relate spectral changes to the structure of clusters. In the study of lithiated valine water clusters, we addressed the question of zwitterion formation upon the combined effect of water and an external ion. Our data indicate the presence of the non-zwitterionic form of valine upon addition of up to four water molecules. In all of the species studied here, the hydration process is driven by solvation of the charge, and upon completion of a first shell around it, water preferentially forms a second solvation shell with no strong competition from other hydration sites on the amino acid backbone. Strikingly, similar water network structures have been observed at the highest hydration level of completely different species, probably indicating the existence of stable ordered water structures. We obtained evidence for a structrual change of the valine backbone in lithiated valine upon addition of the third water molecule, while no conformational change has been identified in the clusters of the protonated species. We have thus been able to answer questions related to the conformational preferences of the amino acid and the structuring of the water network.