Conformer-specific IR Research Articles

Conformer-Specific Spectroscopy and IR-Induced Isomerization of a Model γ-Peptide: Ac-γ4-Phe-NHMe.

Single-conformation IR and UV spectroscopy of the prototypical capped γ-peptide Ac-γ4-Phe-NHMe (γ4F) was carried out under jet-cooled conditions in the gas phase in order to understand its innate conformational preferences in the absence of a solvent. We obtained conformer-specific IR and UV spectra and compared the results with calculations to make assignments and explore the differences between the γ2- and γ4-substituted molecules. We found four conformers of γ4F in our experiment. Three conformers form nine-membered hydrogen-bonded rings (C9) enclosed by an NH···O═C H-bond but differing in their phenyl ring positions (a, g+, and g-). The fourth conformer forms a strained seven-membered hydrogen-bonded ring in which the amide groups lie in a nominally anti-parallel arrangement stacked on top of one another (labeled S7). This conformer is a close analogue of the amide-stacked conformer (S) found previously in γ2F, in which the Phe side chain is substituted at the γ2 position, Ac-γ2-Phe-NHMe (J. Am. Chem. Soc. 2009, 131, 14243-14245). IR population transfer spectroscopy was used to determine the fractional abundances of the γ4F conformers in the expansion. A combination of force field and density functional theory calculations is used to map out the conformational potential energy surfaces for γ4F and compare it with its γ2F counterpart. Based on this analysis, the phenyl ring prefers to take up structures that facilitate NH···π interactions in γ4F or avoid phenyl interactions with the C═O group in γ2F. The disconnectivity graph for γ4F reveals separate basins associated with the C9 and amide-stacked conformational families, which are separated by a barrier of about 42 kJ/mol. The overall shape of the potential energy surface bears a resemblance to peptides and proteins that have a misfolding pathway that competes with the formation of the native structure.

A conformation-specific IR spectroscopic signature for weak C[double bond, length as m-dash]OC[double bond, length as m-dash]O n→π* interaction in capped 4R-hydroxyproline.

Collagen, the most abundant protein in animals, has a unique triple helical structure comprising three parallel left-handed polyproline II (PPII) strands while each of the strands consists of a repeating sequence of X-Y-Gly, where X = proline (Pro) and Y = 4-hydroxyproline (Hyp). Collagen forms a stable triple helix of very long polypeptide strands despite the absence of intra-strand hydrogen bonding in the individual polypeptide chains. It has been reported that non-covalent n→π* interaction plays a significant role in stabilizing the individual polypeptide strands in collagen. However, there is no direct spectroscopic evidence for the presence of this interaction in collagen or its building block. Herein, we have observed for the first time a conformation-specific IR spectroscopic signature for C[double bond, length as m-dash]OC[double bond, length as m-dash]O n→π*-amide interaction in a capped Hyp residue, the most important monomer building block of collagen, using isolated gas phase IR spectroscopy and quantum chemistry calculations. The proof of the existence of this interaction in a model monomer has implications for better understanding of its role not only in structures of collagen but also most of the other proteins and larger peptides.

Site-specific binding of a water molecule to the sulfa drugs sulfamethoxazole and sulfisoxazole: a laser-desorption isomer-specific UV and IR study.

To determine the preferred water molecule binding sites of the polybasic sulfa drugs sulfamethoxazole (SMX) and sulfisoxazole (SIX), we have studied their monomers and monohydrated complexes through laser-desorption conformer-specific UV and IR spectroscopy. Both the SMX and SIX monomer adopt a single conformer in the molecular beam. On the basis of their conformer-specific IR spectra in the NH stretch region, these conformers were assigned to the SMX and SIX global minimum structures, both exhibiting a staggered sulfonamide group and an intramolecular C-HO[double bond, length as m-dash]S hydrogen bond. The SMX-H2O and SIX-H2O complexes each adopt a single isomer in the molecular beam. Their isomeric structures were determined based on their isomer-specific IR spectra in the NH/OH stretch region. Quantum Theory of Atoms in Molecules analysis of the calculated electron densities revealed that in the SMX-H2O complex the water molecule donates an O-HN hydrogen bond to the heterocycle nitrogen atom and accepts an N-HO hydrogen bond from the sulfonamide NH group. In the SIX-H2O complex, however, the water molecule does not bind to the heterocycle but instead donates an O-HO[double bond, length as m-dash]S hydrogen bond to the sulfonamide group and accepts an N-HO hydrogen bond from the sulfonamide NH group. Both water complexes are additionally stabilized by a Cph-HOH2 hydrogen bond. Interacting Quantum Atoms analysis suggests that all intermolecular hydrogen bonds are dominated by the short-range exchange-correlation contribution.

Conformation-Specific Infrared and Ultraviolet Spectroscopy of Cold [YAPAA+H]+ and [YGPAA+H]+ Ions: A Stereochemical "Twist" on the β-Hairpin Turn.

Incorporation of the unnatural d-proline (DP) stereoisomer into a polypeptide sequence is a typical strategy to encourage formation of β-hairpin loops because natural sequences are often unstructured in solution. Using conformation-specific IR and UV spectroscopy of cold (≈10 K) gas-phase ions, we probe the inherent conformational preferences of the DP and LP diastereomers in the protonated peptide [YAPAA+H]+, where only intramolecular interactions are possible. Consistent with the solution-phase studies, one of the conformers of [YADPAA+H]+ is folded into a charge-stabilized β-hairpin turn. However, a second predominant conformer family containing two sequential γ-turns is also identified, with similar energetic stability. A single conformational isomer of the LP diastereomer, [YALPAA+H]+, is found and assigned to a structure that is not the anticipated "mirror image" β-turn. Instead, the LP stereocenter promotes a cis-alanine-proline amide bond. The assigned structures contain clues that the preference of the DP diastereomer to support a trans-amide bond and the proclivity of LP for a cis-amide bond is sterically driven and can be reversed by substituting glycine for alanine in position 2, forming [YGLPAA+H]+. These results provide a basis for understanding the residue-specific and stereospecific alterations in the potential energy surface that underlie these changing preferences, providing insights to the origin of β-hairpin formation.

Solvent Effects on the Encapsulation of Divalent Ions by Benzo-18-Crown-6 and Benzo-15-Crown-5.

We measure UV photodissociation (UVPD) spectra of cold benzo-15-crown-5 (B15C5) and benzo-18-crown-6 (B18C6) complexes with divalent ions (M(2+) = Ca(2+), Sr(2+), Ba(2+), and Mn(2+)), solvated with an H2O or a CH3OH molecule: M(2+)·B15C5·H2O, M(2+)·B15C5·CH3OH, M(2+)·B18C6·H2O, and M(2+)·B18C6·CH3OH. All the species show a number of sharp vibronic bands in the 36,600-37,600 cm(-1) region, which can be attributed to electronic transitions of the B18C6 or B15C5 component. Conformer-specific IR spectra of these complexes are also obtained by IR-UV double-resonance spectroscopy in the OH stretching region. All the IR-UV spectra of the H2O complexes show IR bands at ∼3610 and ∼3690 cm(-1); these bands can be assigned to the symmetric and asymmetric OH stretching vibrations of the H2O component. The CH3OH complexes also show the stretching vibration of the OH group at ∼3630 cm(-1). The H2O and the CH3OH components are directly bonded to the M(2+) ion through the M(2+)···O bond in all the complexes, but a small difference in the conformation results in a noticeable difference in the OH stretching frequency, which enables us to determine the number of conformers. For Ca(2+), Sr(2+), and Mn(2+), the number of conformers for the B18C6 complexes is in the range of 2-5, which is clearly larger than complexes with B15C5 (1 or 2). However, for Ba(2+) the number of conformers with B18C6 (1 or 2) is almost the same as that with B15C5. This is probably because the Ba(2+) ion is too large to be located in the cavity center of either B15C5 and B18C6, which provides an open site at the Ba(2+) ion suitable for solvation with H2O or CH3OH. The more conformations a complex can take, the more entropically favored it is at nonzero temperatures. Hence, the larger number of conformations suggests higher stability of the complexes under solvated conditions, leading to a higher degree of ion encapsulation in solution.

Mimicking the First Turn of an α-Helix with an Unnatural Backbone: Conformation-Specific IR and UV Spectroscopy of Cyclically Constrained β/γ-Peptides

The folding preferences of two capped, constrained β/γ-dipeptide isomers, Ac-βACPC-γACHC-NHBn and Ac-γACHC-βACPC-NHBn, (designated βγ and γβ, respectively), have been investigated using single- and double-resonance ultraviolet and infrared spectroscopy in the gas phase. These capped β/γ-dipeptides have the same number of backbone atoms between their N- and C-termini as a capped α-tripeptide and thus serve as a minimal structural unit on which to test their ability to mimic the formation of the first turn of an α-helix. Resonant two-photon ionization and UV-UV hole-burning spectroscopy were performed in the S0-S1 region, revealing the presence of three unique conformations of βγ and a single conformation of γβ. Resonant ion-dip infrared spectra were obtained in the NH stretch region from 3300 to 3500 cm(-1) and in both the amide I and amide II regions from 1400 to 1800 cm(-1). These infrared spectra were compared to computational predictions from density functional theory calculations at the M05-2X/6-31+G(d) level, leading to assignments for the observed conformations. Two unique bifurcated C8/C13 H-bonded ring structures for βγ and a single bifurcated C9/C13 H-bonded ring structure for γβ were observed. In all cases, the H-bonding patterns faithfully mimic the first full turn of an α-helix, most notably by containing a 13-membered H-bonded cycle but also by orienting the interior amide group so that it is poised to engage in a second C13 H-bond as the β/γ-peptide lengthens in size. The structural characteristics of the β/γ-peptide version of the 13-helix turn are compared with the α-helix counterpart and with a reported crystal structure for a longer β/γ-peptide oligomer.

Single-conformation UV and IR spectroscopy of model G-type lignin dilignols: the β–O–4 and β–β linkages

Single-conformation ultraviolet and infrared spectroscopy was performed on dilignols containing two of the three biologically prevalent β-lignol linkages, erythro β–O–4 (β-aryl ether) and (±) β–β (pinoresinol). Both dilignols contain guaiacol(G)-type sub-units, representative of these linkages in G-type lignin. Resonant two-photon ionization (R2PI), IR-UV, and UV-UV holeburning (UVHB) spectroscopy in the cold, isolated environment of a supersonic expansion was carried out to determine the spectroscopic signatures associated with each linkage conformation, revealing striking differences in the vibronic intensity patterns between the two molecules in the UV. Two conformational isomers were found for the β–O–4 dilignol, both being classified into the fully hydrogen-bonded family with α-OH⋯OCH3 (C8) and γ-OH⋯Oβ (C5) H-bonds that are characteristic of the β–O–4 linkage. Conversely, a single dominant conformation was found for the conformationally-constrained pinoresinol. Resonant ion-dip infrared (RIDIR) spectroscopy provided conformation-specific IR spectra in the OH stretch and alkyl CH stretch regions, yielding complementary data that reported on both the intramolecular H-bonding and more subtle linkage features, respectively. DFT M05-2X calculations predict that the rigid β–β linkage had far fewer low-energy conformations in the first 20 kJ mol−1 (3) than the more flexible β–O–4 linkage (45). In the β–O–4 lignin dimer, the distinct UV chromophores lead to a splitting between S1 and S2 states that is determined mainly by the differences in the chemical structures of the two chromophores. In pinoresinol however, the assigned structure has C2 symmetry, with a calculated vertical excitonic splitting between the S1 and S2 states of 74 cm−1 (TDDFT). After taking into account the reduction in splitting associated with the geometry change in the aromatic rings upon electronic excitation, a vibronically quenched excitonic splitting of no more than a few wavenumbers is predicted for the C2 symmetric pinoresinol, but a definite experimental confirmation was not possible. These results predict that, under most circumstances, adjacent chromophores along a lignin polymer chain are not significantly electronically coupled to one another, and can be treated largely as isolated chromophores.

Cyclic Constraints on Conformational Flexibility in γ-Peptides: Conformation Specific IR and UV Spectroscopy

Single-conformation spectroscopy has been used to study two cyclically constrained and capped γ-peptides: Ac-γACHC-NHBn (hereafter γACHC, Figure 1a), and Ac-γACHC-γACHC-NHBn (γγACHC, Figure 1b), under jet-cooled conditions in the gas phase. The γ-peptide backbone in both molecules contains a cyclohexane ring incorporated across each Cβ-Cγ bond and an ethyl group at each Cα. This substitution pattern was designed to stabilize a (g+, g+) torsion angle sequence across the Cα-Cβ-Cγ segment of each γ-amino acid residue. Resonant two-photon ionization (R2PI), infrared-ultraviolet hole-burning (IR-UV HB), and resonant ion-dip infrared (RIDIR) spectroscopy have been used to probe the single-conformation spectroscopy of these molecules. In both γACHC and γγACHC, all population is funneled into a single conformation. With RIDIR spectra in the NH stretch (3200-3500 cm(-1)) and amide I/II regions (1400-1800 cm(-1)), in conjunction with theoretical predictions, assignments have been made for the conformations observed in the molecular beam. γACHC forms a single nearest-neighbor C9 hydrogen-bonded ring whereas γγACHC takes up a next-nearest-neighbor C14 hydrogen-bonded structure. The gas-phase C14 conformation represents the beginning of a 2.614-helix, suggesting that the constraints imposed on the γ-peptide backbone by the ACHC and ethyl groups already impose this preference in the gas-phase di-γ-peptide, in which only a single C14 H-bond is possible, constituting one full turn of the helix. A similar conformational preference was previously documented in crystal structures and NMR analysis of longer γ-peptide oligomers containing the γACHC subunit [Guo, L., et al. Angew. Chem. Int. Ed. 2011, 50, 5843-5846]. In the gas phase, the γACHC-H2O complex was also observed and spectroscopically interrogated in the molecular beam. Here, the monosolvated γACHC retains the C9 hydrogen bond observed in the bare molecule, with the water acting as a bridge between the C-terminal carbonyl and the π-cloud of the UV chromophore. This is in contrast to the unconstrained γ-peptide-H2O complex, which incorporates H2O into both C9 and amide-stacked conformations.

Gas-Phase Spectroscopy of Laser-Desorbed Acedan and Proline-Acedan

Acedan (2-acetyl-6-dialkylaminonaphthalene) and prolineacedan (A and B in Scheme 1, respectively) are precursors for two-photon fluorescent probes such as ANO1, which turns on its fluorescence when bound to nitric oxide (NO). In spite of their similar molecular structures, A and B have different photophysical properties including absorption coefficient and fluorescence quantum yield. In order to prove the hypothesis that their different fluorescence properties stem from their different conformational structures, we tried to measure their conformation-specific UV and IR spectra in gas phase. The experimental setup has been described in previous publications. In-house synthesized powder sample of A or B was mixed with carbon black powder and the mixture was deposited on the lateral face of a graphite disk. The sample was desorbed by 1064 nm radiation of a pulsed Nd:YAG laser in vacuum, and the desorbed molecules were subsequently cooled down by pulsed supersonic expansion of Ar gas at 40 bar. UV spectra were measured by two-color resonance-enhanced multiphoton ionization (REMPI) with frequency-doubled output of Nd:YAG pumped dye lasers and a time-of-flight mass spectrometer. IR laser was provided by difference frequency generation of a dye laser and an Nd:YAG laser. IR-UV spectroscopy was used to record conformer-specific IR spectrum while the IR was scanned, and conformer-specific UV spectrum while the UV was scanned. Figure 1 shows 1+1' REMPI spectra of B (m/z = 283) and its fragments (m/z = 182, 241) with the second UV at 266 nm. Even though laser-desorption was employed to vaporize the sample, significant fragmentation was observed in the photoionization mass spectrum. The fragment of B at m/z = 241 (241) shows much stronger ion signal than the molecular ion (B, m/z = 283). As B and 241 showed similar vibronic bands in this region, it was assumed that 241 is issued from dissociative ionization of B, and the strong REMPI spectrum of 241 was presumed to reflect that of B. Figure 2 shows the 1+1' REMPI spectrum of 241 at lower

Gas-phase salt bridge interactions between glutamic acid and arginine

The gas-phase side chain-side chain (SC-SC) interaction and possible proton transfer between glutamic acid (Glu) and arginine (Arg) residues are studied under low-temperature conditions in an overall neutral peptide. Conformation-specific IR spectra, obtained with the free electron laser FELIX, in combination with density functional theory (DFT) calculations, provide insight into the occurrence of intramolecular proton transfer and detailed information on the conformational preferences of the peptides Z-Glu-Alan-Arg-NHMe (n = 0,1,3). Low-energy structures are obtained using molecular dynamics simulations via the simulated annealing approach, resulting in three types of SC-SC interactions, in particular two types of pair-wise interactions and one bifurcated interaction. These low-energy structures are optimized and frequency calculations are performed using the B3LYP functional, for structural analysis, and the M05-2x functional, for relative energies, employing the 6-311+G(d,p) basis set. Comparison of experimental and computed spectra suggests that only a single conformation was present for each of the three peptides. Despite the increasing spacing between the Glu and Arg residues, the peptides have several types of interactions in common, in particular specific SC-SC and dispersion interactions between the Arg side chain and the phenyl ring of the Z-cap. Comparison with previous experiments on Ac-Glu-Ala-Phe-Ala-Arg-NHMe as well as molecular dynamics simulations further suggest that the pairwise interaction observed here is indeed energetically most favorable for short peptide sequences.

Conformational Study of Z-Glu-OH and Z-Arg-OH: Dispersion Interactions versus Conventional Hydrogen Bonding

The gas-phase conformational preferences of the model dipeptides Z-Glu-OH and Z-Arg-OH have been studied in the low-temperature environment of a supersonic jet. IR-UV ion-dip spectra obtained using the free electron laser FELIX provide conformation-specific IR spectra, which in combination with density functional theory (DFT) allow us to determine the conformational structures of the peptides. Molecular dynamics modeling using simulated annealing generates a variety of low-energy structures, for which geometry optimization and frequency calculations are then performed using the B3LYP functional with the 6-311+G(d,p) basis set. By comparing experimental and theoretical IR spectra, three conformations for Z-Glu-OH and two for Z-Arg-OH have been identified. For three of the five structures, the dispersion interaction provides an important contribution to the stabilization, emphasizing the importance of these forces in small peptides. Therefore, dispersion-corrected DFT functionals (M05-2X and B97D) have also been employed in our theoretical analysis. Second-order Møller-Plesset perturbation theory (MP2) has been used as benchmark for the relative energies of the different conformational structures. Finally, we address the ongoing debate on the gas-phase structure of arginine by elucidating whether isolated arginine is canonical, tautomeric, or zwitterionic.

A sting in the tail of flexible molecules: spectroscopic and energetic challenges in the case of p-aminophenethylamine

The neurotransmitter analogue p-aminophenethylamine (APEA) illustrates many of the pitfalls and challenges associated with spectroscopic and conformational analysis of flexible molecules. The combined experimental-theoretical study presented here resolves a long-standing controversy over its conformational energetic preferences. Jet-cooled resonance enhanced two-photon ionisation (R2PI) and IR-UV ion depletion techniques enabled conformer-specific IR spectra in the NH-CH stretch region to be measured for four distinct conformers of APEA. Comparison of spectra with theoretical calculations (including MP2, M06-2X and B3LYP with aug-cc-pVTZ basis sets) allows the two most populated conformers to be unambiguously identified as those having a gauche arrangement of the side chain, which facilitates an NH···π type hydrogen bond. The other two observed conformers are assigned to structures with an anti-side chain. A fifth gauche conformer, predicted to be least stable, is not observed. Comparison with published conformer specific IR spectra of tyramine (Makara et al., J. Phys. Chem. A, 2008, 112, 13463-13469) and Raman spectra of phenylethylamine (Golan et al., J. Chem. Phys., 2009, 131, 024305) reveals an entirely consistent pattern of spectral signatures associated with the four specific conformations of the ethylamine side chain evident in APEA, and aids assignment of the associated CH and NH stretch fundamentals, some of which have very weak IR intensities. Extensive calculations of the relative energetic trends of the five conformers have been carried out. In comparison to the highest level of theory considered, CCSD(T)-F12b/cc-pVDZ-F12, MP2 overestimate the energy difference, whereas DFT significantly underestimates the energetic preference for NH···π stabilised gauche conformers, although inclusion of dispersion (M06-2X, B3LYP-D3) improves the DFT results.

Highly Resolved Spectra of Gas-Phase Gramicidin S: A Benchmark for Peptide Structure Calculations

We have measured a vibrationally resolved UV spectrum of doubly protonated gramicidin S (GS) in the gas phase and, subsequently, a highly resolved, conformer-specific IR spectrum in the 6 mum fingerprint region, using a cold ion trap in combination with table-top lasers. The study has revealed at least three conformational states of GS populated under our experimental conditions, with the major one showing evidence of a symmetric three-dimensional structure similar to that in the condensed phase. The derived qualitative constraints, along with the measured vibrational frequencies, serve as a benchmark for computations of peptide structure.

Probing the competition between secondary structures and local preferences in gas phase isolated peptide backbones

Combining laser desorption with a supersonic expansion together with the selectivity of IR/UV double resonance spectroscopy makes it possible to isolate and characterise the gas phase of remarkable backbone conformations of short peptide chains mimicking protein segments. A systematic bottom-up approach involving a conformer-specific IR study of peptide sequences of increasing sizes has enabled us to map the spectral signatures of the intramolecular interactions, which shape the peptide backbone, in particular H-bonds. The precise data collected are directly comparable to the most sophisticated quantum chemistry calculations of these species and therefore constitute a stringent test for the theoretical methods used. One-residue chains reveal the local conformational preference of the backbone and its dependence upon the nature of the residue. The investigation of longer chains provides evidence for a competition between simple successions of local conformational preferences along the chain and more folded structures, in which a new H-bonding network, involving distant H-bonding sites along the backbone, takes place. From three residues, the issue of helical folding can also be addressed. The present review of the gas phase literature data emphasizes the observation of remarkable secondary structures of biology, including short segments of beta-strands, gamma- and beta-turns, combinations of turns, including a 3(10) helix. It also provides evidence for the flexibility of the peptide chains, i.e., a critical influence of rather minor interactions (like side-chain/backbone interactions) on the conformational stability. Finally, the paper will discuss future promising directions of the present approach.