Effects of Alkaline Earth Metal Ion Complexation on Amino Acid Zwitterion Stability: Results from Infrared Action Spectroscopy

Infrared consequence spectroscopy of gaseous protonated and metal ion cationized complexes

In this article, the new and exciting techniques of infrared consequence spectroscopy (sometimes called action spectroscopy) of gaseous ions are reviewed. These techniques include vibrational predissociation spectroscopy and infrared multiple photon dissociation spectroscopy and they typically complement one another in the systems studied and the information gained. In recent years infrared consequence spectroscopy has provided long-awaited direct evidence into the structures of gaseous ions from organometallic species to strong ionic hydrogen bonded structures to large biomolecules. Much is being learned with respect to the structures of ions without their stabilizing solvent which can be used to better understand the effect of solvent on their structures. This review mainly covers the topics with which the author has been directly involved in research: structures of proton-bound dimers, protonated amino acids and DNA bases, amino acid and DNA bases bound to metal ions and, more recently, solvated ionic complexes. It is hoped that this review reveals the impact that infrared consequence spectroscopy has had on the field of gaseous ion chemistry.

Vibrational spectroscopy of bare and solvated ionic complexes of biological relevance

The low density of ions in mass spectrometers generally precludes direct infrared (IR) absorption measurements. The IR spectrum of an ion can nonetheless be obtained by inducing photodissociation of the ion using a high-intensity tunable laser. The emergence of free electron lasers (FELs) and recent breakthroughs in bench-top lasers based on nonlinear optics have now made it possible to routinely record IR spectra of gas-phase ions. As the energy of one IR photon is insufficient to cause dissociation of molecules and strongly bound complexes, two main experimental strategies have been developed to effect photodissociation. In infrared multiple-photon dissociation (IR-MPD) many photons are absorbed resonantly and their energy is stored in the bath of vibrational modes, leading to dissociation. In the "messenger" technique a weakly bound van der Waals atom is detached upon absorption of a single photon. Fundamental, historical, and practical aspects of these methods will be presented. Both of these approaches make use of very different methods of ion preparation and manipulation. While in IR-MPD ions are irradiated in trapping mass spectrometers, the "messenger" technique is generally carried out in molecular beam instruments. The main focus of this review is the application of IR spectroscopy to biologically relevant molecular systems (amino acids, peptides, proteins). Particular issues that will be addressed here include gas-phase zwitterions, the (chemical) structures of peptides and their collision-induced dissociation (CID) products, IR spectra of gas-phase proteins, and the chelation of metal-ligand complexes. Another growing area of research is IR spectroscopy on solvated clusters, which offer a bridge between the gas-phase and solution environments. The development of state-of-the-art computational approaches has gone hand-in-hand with advances in experimental techniques. The main advantage of gas-phase cluster research, as opposed to condensed-phase experiments, is that the systems of interest can be understood in detail and structural effects can be studied in isolation. It will be shown that IR spectroscopy of mass-selected (bio)molecular systems is now well-placed to address specific questions on the individual effect of charge carriers (protons and metal ions), as well as solvent molecules on the overall structure.

Effect of cation complexation on the structure of a conformationally flexible multiply charged anion: stabilization of excess charge in the Na+ x adenosine 5'-triphosphate dianion ion-pair complex

We report a computational study of the conformationally and tautomerically flexible cation-dianion complex of Na(+) with doubly deprotonated adenosine 5'-triphosphate (ATP) using a hierarchical selection method. The method uses molecular dynamics to generate initial conformeric structures, followed by a classification process that groups conformers into five "families" to ensure that a representative sample of structures is retained for further analysis, while very similar conformational structures are eliminated. Hierarchical ab initio calculations (DFT and MP2) of typical conformers of the families are then performed to identify the lowest-energy conformeric structures. The procedure described should provide a useful methodology for conducting higher-level ab initio calculations of medium-sized gas-phase biological molecules for interpreting contemporary laser spectroscopy measurements. For Na(+) x [ATP-2H](2) (considering tautomers where the phosphate chain of ATP is doubly deprotonated), the calculations reveal that the sodium cation interacts directly with the negatively charged phosphates (maximum distance = 2.54 A) in all of the low-energy conformers, while a number of the structures also display close cation-adenine interactions producing compact ball-like structures. These compact structures generally correspond to the lowest-energy conformers. The structural variation between the bare [ATP-2H](2-) molecular ion (Burke et al. J. Phys. Chem. A 2005 , 109 , 9775-9785) and the Na(+) x [ATP-2H](2-) cluster is discussed in detail, including the effect of sodiation on the intramolecular hydrogen-bonding network within ATP in a gas-phase environment.

Proton affinity and zwitterion stability: new results from infrared spectroscopy and theory of cationized lysine and analogues in the gas phase

The gas-phase structures of alkali metal cationized lysine (Lys), alpha-N-methyllysine (NMeLys), and epsilon-N,N-dimethyllysine (Lys(Me)(2)) are investigated using infrared multiple photon dissociation (IRMPD) spectroscopy utilizing light generated by a free electron laser and ab initio calculations. The proton affinities of the compounds span a range of approximately 20 kJ/mol. For NMeLys x M(+), experiment and theory indicate that NMeLys is nonzwitterionic for M = Li and zwitterionic for M = Na and K. For Lys(Me)(2) x M(+), experiment and theory indicate that Lys(Me)(2) is zwitterionic for M = Li, Na, and K. This is the first spectroscopic observation of the zwitterionic form of an amino acid complexed with Li(+). The results are compared with IRMPD spectra reported previously for Lys and -N-methyllysine (Lys(Me)) complexed with Li, Na, and K, and new calculations performed at higher levels of theory for those ions. The combined experimental and theoretical results indicate that protonation in the zwitterionic forms of the these amino acids is favored at the more basic methylated amine site, but that any relationship between the proton affinity of the amino acid and the relative zwitterion stability of the alkali metal cationized amino acid is only indirect. These results provide additional evidence that proton affinities are not a reliable indicator of zwitterion stability for cationized amino acids because side chains can have very different effects on the stability of different conformers in the neutral, protonated, and metal cationized forms.

Alanine polypeptide structural fingerprints at room temperature: what can be gained from non-harmonic Car-Parrinello molecular dynamics simulations

Structural infrared fingerprints of neutral gas phase alanine peptides of increasing size and complexity (dipeptide, octapeptide, and beta-strand peptide) are characterized through DFT-based Car-Parrinello molecular dynamics simulations. Harmonic and nonharmonic vibrational signatures are calculated from the time correlation of the dipole moment of the gas phase peptide in a direct way (without any approximation) respectively from low temperature (20 K) and room temperature (300 K) molecular dynamics. Our main purpose is to answer the two following questions: (i) Is the direct inclusion of temperature for the calculation of infrared spectra mandatory for the comprehension of the vibrational signatures experimentally recorded at room temperature? (ii) To what extent is the amide I, II, and III domain sensitive enough to the local structure of the peptides, to provide vibrational signatures that can be definitely used to assess the peptide conformation at 300 K?