Effect of a cis-4-aminopiperidine-3-carboxylic acid (cis-APiC) residue on mixed-helical folding of unnatural peptides.

The α/ß-peptide 11/9-helix and the ß-peptide 12/10-helix belong to "mixed" helices, in which two types of hydrogen bonds with opposite directionality alternate along the helical axis. cis-2-Aminocyclohexanecarboxylic acid (cis-ACHC) is known to promote these mixed helices and stabilize the helical propensity more than other acyclic ß-residues. Application of a mixed-helical backbone still requires sufficient solubility in aqueous solution. In this regard, we chose cis-4-aminopiperidine-3-carboxylic acid (cis-APiC) as a foldamer building block that can provide both sufficient aqueous solubility and mixed-helical propensity. Conformational analyses of α/ß- and ß-peptides containing a cis-APiC residue by circular dichroism spectroscopy and single-crystal X-ray crystallography suggest that the incorporation of cis-APiC instead of cis-ACHC can enhance the aqueous solubility of the mixed-helical peptides without any adverse effect on helical folding. In addition, the ratio between right- and left-handed 12/10-helices of ß-peptides can be rationalized by relative energies between the local conformations of the cis-APiC residue.

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.

Coexistence of Left- and Right-Handed 12/10-Mixed Helices in Cyclically Constrained ß-Peptides and Directed Formation of Single-Handed Helices upon Site-Specific Methylation.

The inherent conformational preferences of the neutral ß-peptide foldamer series, Ac-(ACHC)n-NHBn, n = 2-4, are studied in the gas phase using conformation-specific IR-UV double resonance methods. The cyclically constrained chiral ß-amino acid cis-2-aminocyclohexane carboxylic acid (ACHC) is designed to bring both right- and left-handed helices into close energetic proximity. Comparison of the infrared spectra in the NH stretch and amide I/II regions with the predictions of DFT calculations lead to the unambiguous assignment of four out of the six observed conformations of the molecules in this series, while corroborating computational and spectral evidence, affords tentative assignments of the remaining two conformers for which IR data were not recorded. The observed structures fall into one of two conformational families: a right-handed 12/10-mixed helix or its "cap-disrupted" left-handed helical analogue, which coexist with significant populations. Site-specific and stereospecific methylation on the cyclohexane backbone at the dipeptide (n = 2) level is also tested as a means to sterically lock in a predetermined cyclohexane chair conformation. These substitutions are proven to be a means of selectively driving formation of one helical screw sense or the other. Calculated relative energies and free energies of all possible structures for the molecules provide strong supporting evidence that the rigid nature of the ACHC residue confers unusual stability to the 12/10-mixed helix conformation, regardless of local environment, temperature, or C-terminal capping unit. The simultaneous presence of both handed helices offers unique opportunities for future studies of their interconversion.

Side chain-specific 11/9-helix propensity of α/ß-peptides with alternating residue types.

The 11/9-helix is among the most stable and non-traditional helical structures for α/ß-peptides with alternating residue types. The effect of side chain groups of α-residues and ß3-residues on the 11/9-helix propensity was examined under various solvent conditions. An α-amino acid residue with one of the four representative side chain groups was incorporated into the central position of an α/ß-pentapeptide backbone. A ß-branched valine residue did not show any destabilizing effect. α,α-Dimethylsubstituted Aib residue was tolerated under nonpolar conditions, but did not promote 11/9-helical folding. The oligomer with a glycine residue did not show 11/9-helical folding under polar solvent conditions. The single unmatched stereochemistry of d-alanine was deleterious to 11/9-helical folding. Replacement of a cyclic ß-residue with an acyclic ß3-residue in the 11/9-helical structure had a slight destabilizing effect, which could be compensated by a longer peptide sequence with more cyclic ß-residues. These results provide a guidance for incorporating functional groups into an 11/9-helical α/ß-peptide backbone to design functional oligomers.

Conformation-Specific Spectroscopy of Asparagine-Containing Peptides: Influence of Single and Adjacent Asn Residues on Inherent Conformational Preferences.

The infrared and ultraviolet spectra of a series of capped asparagine-containing peptides, Ac-Asn-NHBn, Ac-Ala-Asn-NHBn, and Ac-Asn-Asn-NHBn, have been recorded under jet-cooled conditions in the gas phase in order to probe the influence of the Asn residue, with its -CH2-C(═O)-NH2 side chain, on the local conformational preferences of a peptide backbone. The double-resonance methods of resonant ion-dip infrared (RIDIR) spectroscopy and infrared-ultraviolet hole-burning (IR-UV HB) spectroscopy were used to record single-conformation spectra in the infrared and ultraviolet, respectively, free from interference from other conformations present in the molecular beam. Ac-Asn-NHBn spreads its population over two conformations, both of which are stabilized by a pair of H-bonds that form a bridge between the Asn carboxamide group and the NH and C═O groups on the peptide backbone. In one the peptide backbone engages in a 7-membered H-bonded ring (labeled C7eq), thereby forming an inverse γ-turn, stabilized by a C6/C7 Asn bridge. In the other the Asn carboxamide group forms a C8/C7 H-bonded bridge with the carboxamide group facing in the opposite direction across an extended peptide backbone involving a C5 interaction. Both Ac-Ala-Asn-NHBn and Ac-Asn-Asn-NHBn are found exclusively in a single conformation in which the peptide backbone engages in a type I ß-turn with its C10 H-bond. The Asn residue(s) stabilize this ß-turn via C6 H-bond(s) between the carboxamide C═O group and the same residue's amide NH. These structures are closely analogous to the corresponding structures in Gln-containing peptides studied previously [Walsh, P. S. et al. PCCP 2016, 18, 11306-11322; Walsh, P. S. et al. Angew. Chem. Int. Ed. 2016, 55, 14618-14622], indicating that the Asn and Gln side chains can each configure so as to stabilize the same backbone conformations. Spectroscopic and computational evidence suggest that glutamine is more predisposed than asparagine to ß-turn formation via unusually strong side-chain-backbone hydrogen-bond formation. Further spectral and structural similarities and differences due to the side-chain length difference of these similar amino acids are presented and discussed.

Conformer-Specific and Diastereomer-Specific Spectroscopy of αßα Synthetic Foldamers: Ac-Ala-ßACHC-Ala-NHBn.

The folding propensities of a capped, cyclically constrained, mixed α/ß diastereomer pair, ( SRSS) Ac-Ala-ßACHC-Ala-NHBn (hereafter RS) and ( SSRS) Ac-Ala-ßACHC-Ala-NHBn ( SR), have been studied in a molecular beam using single-conformation spectroscopic techniques. These α/ß-tripeptides contain a cyclohexane ring across each Cα -Cß bond, at which positions their stereochemistries differ. This cyclic constraint requires any stable species to adopt one of two ACHC configurations: equatorial C═O/axial NH or equatorial NH/axial C═O. Resonant two-photon ionization (R2PI) and infrared-ultraviolet hole-burning (IR-UV HB) spectroscopy were used in the S0-S1 region of the UV chromophore, revealing the presence of three unique conformational isomers of RS and two of SR. Resonant ion-dip infrared spectra were recorded in both the NH stretch (3200-3500 cm-1) and the amide I (1600-1800 cm-1) regions. These experimental vibrational frequencies were compared with the scaled calculated normal-mode frequencies from density functional theory at the M05-2X/6-31+G(d) level of theory, leading to structural assignments of the observed conformations. The RS diastereomer is known in crystalline form to preferentially form a C11/C9 mixed helix, in which alternating hydrogen bonds are arranged in near antiparallel orientation. This structure is preserved in one of the main conformers observed in the gas phase but is in competition with both a tightly folded C7eq/C12/C8/C7eq structure, in which all four amide NH groups and four C═O groups are engaged in hydrogen bonding, as well as a cap influenced C7eq/NH···π/C11 structure. The SR diastereomer is destabilized by inducing backbone dihedral angles that lie outside the typical Ramachandran angles. This diastereomer also forms a C11/C9 mixed helix as well as a cap influenced bifurcated C7ax-C11/NH···π/C7eq structure as the global energy minimum. Assigned structures are compared with the reported crystal structure of analogous α/ß-tripeptides, and disconnectivity graphs are presented to give an overview of the complicated potential energy surface of this tripeptide diastereomer pair.

12/10-Helical ß-Peptide with Dynamic Folding Propensity: Coexistence of Right- and Left-Handed Helices in an Enantiomeric Foldamer.

We present the first examples of atomic-resolution crystal data for the ß-peptide 12/10-helix from oligomers of cis-2-aminocyclohexane carboxylic acid (cis-ACHC) with alternating chirality. The local conformations of two enantiomeric cis-ACHC dimer units suggested that a chiral ß-peptide may adopt both right-handed and left-handed helical conformations in solution. To probe the conformational behavior of 12/10-helical ß-peptides, the two reference helices with a single handedness were synthesized with a more rigidified cis-ACHC derivative. Comparison with these reference helices at low temperature revealed that a chiral cis-ACHC oligomer with alternating chirality indeed displays 12/10-helical conformations with both handedness that equilibrate rapidly in solution. This is a very rare example of chiral oligomers with helix inversion ability. The 12/10-helical backbone should be a valuable addition to potential scaffolds for applications involving helices with dynamic folding propensity.

Helical α/ß-depsipeptides with alternating residue types: conformational change from the 11-helix to the 14/15-helix.

Short α/ß-peptides that consist of alternating l-α-amino acids and trans-2-aminocyclopentanecarboxylic acid are known to adopt both 11- and 14/15-helical conformations in solution. We report short α/ß-depsipeptides containing (S)-lactic acid as the third residue from the N-terminus. The α/ß-depsipeptide pentamers and heptamers adopt 14/15-helical conformations analogous to the α-helix in the crystal state and display 14/15-helical conformations predominantly in solution.

Helical folding of α/ß-peptides containing ß-amino acids with an eight-membered ring constraint.

αßα-Tripeptide that contains a cyclic ß-amino acid with an eight-membered ring, a cis-2-aminocyclooct-5-enecarboxylic acid (cis-ACOE) or a cis-2-aminocyclooctanecarboxylic acid (cis-ACOC) displayed an 11/9-helical turn in the crystal state. The related α/ß-peptide oligomers were shown to adopt 11/9-helical conformations in solution.

Exploring a ß-Amino Acid with a Seven-Membered Ring Constraint as a Foldamer Building Block for Nontraditional Helices.

We explored trans- and cis-2-aminocycloheptanecarboxylic acid (ACHpC) as potential building blocks for helical foldamers. trans-ACHpC does not show sufficient folding propensity in unnatural peptides. cis-ACHpC promotes nontraditional helices of two unnatural peptide backbones: the 11/9-helix for 1:1 α/ß-peptides and the 12/10-helix for ß-peptides with interconvertible handedness. The two opposite-handed 12/10-helices rapidly interconvert in solution by pseudorotation of the two twist chair forms of the cycloheptane moiety in each cis-ACHpC residue.

3-(N-arylsulfamoyl)benzamides, inhibitors of human sirtuin type 2 (SIRT2).

Inhibition of sirtuin 2 (SIRT2) is known to be protective against the toxicity of disease proteins in Parkinson's and Huntington's models of neurodegeneration. Previously, we developed SIRT2 inhibitors based on the 3-(N-arylsulfamoyl)benzamide scaffold, including3-(N-(4-bromophenyl)sulfamoyl)-N-(4-bromophenyl)benzamide(C2-8, 1a), which demonstrated neuroprotective effects in a Huntington's mouse model, but had low potency of SIRT2 inhibition. Here we report that N-methylation of 1a greatly increases its potency and results in excellent selectivity for SIRT2 over SIRT1 and SIRT3 isoforms. Structure-activity relationships observed for 1a analogs and docking simulation data suggest that the para-substituted amido moiety of these compounds could occupy two potential hydrophobic binding pockets in SIRT2. These results provide a direction for the design of potent drug-like SIRT2 inhibitors.

Single-conformation infrared spectra of model peptides in the amide I and amide II regions: experiment-based determination of local mode frequencies and inter-mode coupling.

Single-conformation infrared spectra in the amide I and amide II regions have been recorded for a total of 34 conformations of three α-peptides, three ß-peptides, four α/ß-peptides, and one γ-peptide using resonant ion-dip infrared spectroscopy of the jet-cooled, isolated molecules. Assignments based on the amide NH stretch region were in hand, with the amide I/II data providing additional evidence in favor of the assignments. A set of 21 conformations that represent the full range of H-bonded structures were chosen to characterize the conformational dependence of the vibrational frequencies and infrared intensities of the local amide I and amide II modes and their amide I/I and amide II/II coupling constants. Scaled, harmonic calculations at the DFT M05-2X/6-31+G(d) level of theory accurately reproduce the experimental frequencies and infrared intensities in both the amide I and amide II regions. In the amide I region, Hessian reconstruction was used to extract local mode frequencies and amide I/I coupling constants for each conformation. These local amide I frequencies are in excellent agreement with those predicted by DFT calculations on the corresponding (13)C = (18)O isotopologues. In the amide II region, potential energy distribution analysis was combined with the Hessian reconstruction scheme to extract local amide II frequencies and amide II/II coupling constants. The agreement between these local amide II frequencies and those obtained from DFT calculations on the N-D isotopologues is slightly worse than for the corresponding comparison in the amide I region. The local mode frequencies in both regions are dictated by a combination of the direct H-bonding environment and indirect, "backside" H-bonds to the same amide group. More importantly, the sign and magnitude of the inter-amide coupling constants in both the amide I and amide II regions is shown to be characteristic of the size of the H-bonded ring linking the two amide groups. These amide I/I and amide II/II coupling constants remain similar in size for α-, ß-, and γ-peptides despite the increasing number of C-C bonds separating the amide groups. These findings provide a simple, unifying picture for future attempts to base the calculation of both nearest-neighbor and next-nearest-neighbor coupling constants on a joint footing.

Helical Structures of Nylon-Like Oligomers Consisting of 1,2-Diamine and 1,2-Dicarboxylic Acid Building Blocks Containing a Five-Membered Ring Constraint.

A series of nylon-like oligomers was synthesized, which consisted of alternating cyclic 1,2-diamine and 1,2-dicarboxylic acid building blocks with a five-membered ring constraint. The nylon 2 4 oligomers are symmetric and display helical structures similar to the ß-peptide 12-helix with intramolecular 12-membered ring hydrogen bonds. The cyclopentane moiety allows each building block to promote 12-helical folding. In addition, a tartaric acid derivative with the acetonide moiety increases the solubility of oligomers in common organic solvents and promotes helical folding.

Crystallographic characterization of 12-helical secondary structure in ß-peptides containing side chain groups.

Helices are the most extensively studied secondary structures formed by ß-peptide foldamers. Among the five known ß-peptide helices, the 12-helix is particularly interesting because the internal hydrogen bond orientation and macrodipole are analogous to those of α-peptide helices (α-helix and 3(10)-helix). The ß-peptide 12-helix is defined by i, i+3 C═O···H-N backbone hydrogen bonds and promoted by ß-residues with a five-membered ring constraint. The 12-helical scaffold has been used to generate ß-peptides with specific biological functions, for which diverse side chains must be properly placed along the backbone and, upon folding, properly arranged in space. Only two crystal structures of 12-helical ß-peptides have previously been reported, both for homooligomers of trans-2-aminocyclopentanecarboxylic acid (ACPC). Here we report five additional crystal structures of 12-helical ß-peptides, all containing residues that bear side chains. Four of the crystallized ß-peptides include trans-4,4-dimethyl-2-aminocyclopentanecarboxylic acid (dm-ACPC) residues, and the fifth contains a ß(3)-hPhe residue. These five ß-peptides adopt fully folded 12-helical conformations in the solid state. The new crystal structures, along with previously reported data, allow a detailed characterization of the 12-helical conformation; average backbone torsion angles of ß-residues and helical parameters are derived. These structural parameters are found to be similar to those for i, i+3 C═O···H-N hydrogen-bonded helices formed by other peptide backbones generated from α- and/or ß-amino acids. The similarity between the conformational behavior of dm-ACPC and ACPC is consistent with previous NMR-based conclusions that 4,4-disubstituted ACPC derivatives are compatible with 12-helical folding. In addition, our data show how a ß(3)-residue is accommodated in the 12-helix, thus enhancing understanding of the diverse conformational behavior of this flexible class of ß-amino acids.

Helix formation in preorganized beta/gamma-peptide foldamers: hydrogen-bond analogy to the alpha-helix without alpha-amino acid residues.

We report the first high-resolution structural data for the beta/gamma-peptide 13-helix (i,i+3 C=O...H-N H-bonds), a secondary structure that is formed by oligomers with a 1:1 alternation of beta- and gamma-amino acid residues. Our characterization includes both crystallographic and 2D NMR data. Previous studies suggested that beta/gamma-peptides constructed from conformationally flexible residues adopt a different helical secondary structure in solution. Our design features preorganized beta- and gamma-residues, which strongly promote 13-helical folding by the 1:1 beta/gamma backbone.

Laser spectroscopy of conformationally constrained alpha/beta-peptides: Ac-ACPC-Phe-NHMe and Ac-Phe-ACPC-NHMe.

Single-conformation ultraviolet and infrared spectra have been recorded under the isolated molecule conditions of a supersonic expansion for three conformationally constrained alpha/beta-peptides, Ac-L-Phe-ACPC-NHMe (alpha(L)beta(ACPC)), Ac-ACPC-L-Phe-NHMe (beta(ACPC)alpha(L)), and Ac-ACPC-D-Phe-NHMe (beta(ACPC)alpha(D)). These three molecules are close analogues of the hAla-containing alpha/beta-peptide counterparts Ac-L-Phe-beta(3)-hAla-NHMe, Ac-beta(3)-hAla-L-Phe-NHMe, and Ac-beta(3)-hAla-D-Phe-NHMe, which have been studied recently by James et al. (J. Am. Chem. Soc. 2009, 131, 6574). Incorporation of the beta-amino acid trans-2-aminocyclopentanecarboxylic acid (ACPC) constrains the beta-peptide backbone via the cyclopentane ring, producing clear changes in the conformational preferences relative to the unconstrained analogues. The conformational control is manifested most obviously in the complete absence of C6 H-bonded rings, which were dominant in the unconstrained alpha/beta-peptides. The most stable C6 ring structure (C6a) in the absence of the ACPC ring cannot be formed in its presence, while a secondary C6 ring (C6b) has its energy destabilized by approximately 20 kJ/mol. In alpha(L)beta(ACPC), the preference for C5 structures in the N-terminal position, combined with the strong preference for C8 structures in the beta-peptide subunit, leads to the observation of two C5/C8 bifurcated double ring conformers. Both C8/C7 sequential double rings and C11 single rings are observed in beta(ACPC)alpha(L) and beta(ACPC)alpha(D). Here, the ACPC ring selectively stabilizes the C8a ring over other possible C8 structures. Finally, the combined evidence from IR and UV spectra lead to tentative assignments for diastereomeric pairs, exhibiting small but understandable shifts in the IR and UV spectra induced by the change in chirality at the alpha-peptide chiral center.

Crystallographic characterization of helical secondary structures in 2:1 and 1:2 alpha/beta-peptides.

Oligomers containing both alpha- and beta-amino acid residues ("alpha/beta-peptides") are intriguing as potential foldamers. A large set of alpha/beta-peptide backbones can be generated by combining alpha- and beta-amino acid residues in different patterns; however, most research to date has focused on the simplest pattern, 1:1 alpha:beta. We have begun to explore the range of variation that can be achieved with alpha-residue/beta-residue combinations by examining the folding behavior of oligomers that contain 2:1 and 1:2 alpha:beta patterns. The beta-residues in our systems have a five-membered-ring constraint (trans-2-aminocyclopentanecarboxylic acid (ACPC) residues), because these preorganized subunits strongly promote helical folding for 1:1 alpha:beta backbones and pure beta backbones. Previously we concluded that two helical conformations are available to 2:1 and 1:2 alpha/beta-peptides containing ACPC or analogously constrained beta-residues, one helix defined by i,i+3 CO...H-N backbone hydrogen bonds and the other defined by i,i+4 CO...H-N hydrogen bonds. These deductions were based on 2D NMR analysis of a 2:1 heptamer and a 1:2 hexamer in methanol. Crystallographic analysis of a pair of analogous nonpolar alpha/beta-peptides showed only the i,i+3 hydrogen-bonded helical conformations. We now report four new crystal structures of 2:1 alpha/beta-peptides, ranging in length from 5 to 11 residues, and six new crystal structures of 1:2 alpha/beta-peptides, ranging in length from 6 to 10 residues. All 10 of these new structures are fully helical, and all helices display the i,i+3 CO...H-N hydrogen bonding pattern. These crystallographic data sets, collectively, provide high structural definition for the i,i+3 hydrogen-bonded helical secondary structures available to these foldamer backbones.

Single-conformation and diastereomer specific ultraviolet and infrared spectroscopy of model synthetic foldamers: alpha/beta-peptides.

Resonant two-photon ionization (R2PI), UV hole-burning (UVHB), and resonant ion-dip infrared (RIDIR) spectroscopies have been used to record single-conformation infrared and ultraviolet spectra of three model synthetic foldamers with heterogeneous backbones, alpha/beta-peptides Ac-beta(3)-hAla-L-Phe-NHMe (betaalphaL), Ac-beta(3)-hAla-D-Phe-NHMe (betaalphaD), and Ac-L-Phe-beta(3)-hAla-NHMe (alphabetaL), isolated and cooled in a supersonic expansion. BetaalphaL and betaalphaD are diastereomers, differing only in the configuration of the alpha-amino acid residue; betaalphaL and alphabetaL contain the same residues, but differ in residue order. In all three alpha/beta-peptides the beta(3)-residue has S absolute configuration. UVHB spectroscopy is used to determine that there are six conformers of each molecule and to locate and characterize their S(0)-S(1) transitions in the origin region. RIDIR spectra in the amide NH stretch region reflect the number and strength of intramolecular H-bonds present. Comparison of the RIDIR spectra with scaled, harmonic vibrational frequencies and infrared intensities leads to definite assignments for the conformational families involved. C8/C7(eq) double-ring structures are responsible for three conformers of betaalphaL and four of betaalphaD, including those with the most intense transitions in the R2PI spectra. This preference for C8/C7(eq) double rings appears to be dictated by the C7(eq) ring of the alpha-peptide subunit. Three of the conformers of betaalphaL and betaalphaD form diastereomeric pairs (A/A', C/C', and G/G') that have nearly identical S(0)-S(1) origin positions in the UV and belong to the same conformational family, indicating no significant change associated with the change in chirality of the alpha-peptide subunit. However, betaalphaL favors formation of a C6/C5 conformer over C11, while the reverse preference holds in betaalphaD. Calculations indicate that the selective stabilization of the lowest-energy C11(g(+)) structure in betaalphaD occurs because this structure minimizes steric effects between the beta(2) methylene group and C=O(1). In the alpha/beta-peptide alphabetaL, two conformers dominate the spectrum, one assigned to a C5/C8 bifurcated double-ring, and the other to a C5/C6 double-ring structure. This preference for C5 rings in the alpha/beta-peptide occurs because the C5 ring is further stabilized by an amide NH...pi interaction involving an NH group on the adjacent amide, as it is in the alpha-peptides. Comparison of the NH stretch spectra of C8/C7(eq) structures in betaalphaL with their C7(eq)/C8 counterparts in alphabetaL shows that the central amide NH stretch is shifted to lower frequency by some 50-70 cm(-1) due to cooperative effects associated with the central amide accepting and donating a H-bond to neighboring amide groups. This swaps the ordering of the C8 and C7 NH stretch fundamentals in the two molecules.

Crystallographic characterization of helical secondary structures in alpha/beta-peptides with 1:1 residue alternation.

Oligomers that contain both alpha- and beta-amino acid residues in a 1:1 alternating pattern have recently been shown by several groups to adopt helical secondary structures in solution. The beta-residue substitution pattern has a profound effect on the type of helix formed and the stability of the helical conformation. On the basis of two-dimensional NMR data, we have previously proposed that beta-residues with a five-membered ring constraint promote two different types of alpha/beta-peptide helix. The "11-helix" contains i, i+3 CO...H-N hydrogen bonds between backbone amide groups; these hydrogen bonds occur in 11-atom rings. The alpha/beta-peptide "14/15-helix" contains i, i+4 CO...H-N hydrogen bonds, which occur in alternating 14- and 15-atom rings. Here we provide crystallographic data for 14 alpha/beta-peptides that form the 11-helix and/or the 14/15-helix. These results were obtained for a series of oligomers containing beta-residues derived from ( S,S)- trans-2-aminocyclopentanecarboxylic acid (ACPC) and alpha-residues derived from alpha-aminoisobutyric acid (Aib) or l-alanine (Ala). The crystallized alpha/beta-peptides range in length from 4 to 10 residues. Nine of the alpha/beta-peptides display the 11-helix in the solid state, three display the 14/15-helix, and two display conformations that contain both i, i+3 and i, i+4 CO...H-N hydrogen bonds, but not bifurcated hydrogen bonds. Only 3 of the 14 crystal structures presented here have been previously described. These results suggest that longer alpha/beta-peptides prefer the 14/15-helix over the 11-helix, a conclusion that is consistent with previously reported NMR data obtained in solution.

Single-conformation ultraviolet and infrared spectroscopy of model synthetic foldamers: beta-peptides Ac-beta3-hPhe-NHMe and Ac-beta3-hTyr-NHMe.

The conformational preferences and infrared and ultraviolet spectral signatures of two model beta-peptides, Ac-beta3-hPhe-NHMe (1) and Ac-beta3-hTyr-NHMe (2), have been explored under jet-cooled, isolated molecule conditions. The mass-resolved, resonant two-photon ionization spectra of the two molecules were recorded in the region of the S0-S1 origin of the phenyl or phenol ring substituents, respectively. UV-UV hole-burning spectroscopy was used to determine that two conformations of 1 are present, with the transitions due to conformer A, with S0-S1 origin at 34431 cm(-1), being almost 20 times larger than those due to conformer B, with S0-S1 origin at 34404 cm(-1). Only one conformation of 2 was observed. Resonant ion-dip infrared spectroscopy provided single-conformation infrared spectra in the 3300-3700 cm(-1) region. The spectra of conformer A of both molecules have H-bonded and free amide NH stretch infrared transitions at 3400 and 3488 cm(-1), respectively, while conformer B of 1 possesses bands at 3417 and 3454 cm(-1). For comparison with experiment, full optimizations of all low-lying minima of 1 were carried out at the DFT B3LYP/6-31+G* and RIMP2/aug-cc-pVDZ levels of theory, and single point MP2/6-31+G* calculations at the DFT geometries. On the basis of the comparison with previous studies in solution and the calculated results, conformer A of 1 and 2 were assigned to a C6 conformer, while conformer B of 1 was assigned to a unique C8 structure with a weak intramolecular H-bond. The reasons for the preference for C6 over C8 structures and the presence of only two conformations in the jet-cooled spectrum are discussed in light of the predictions from calculations.