Floor Ter Braak1, Hidde Elferink1, Kas J Houthuijs2, Jos Oomens2, Jonathan Martens2, Thomas J Boltje1. 1. Radboud University, Institute for Molecules and Materials, Synthetic Organic Chemistry, Heyendaalseweg 135, 6525 AJ Nijmegen, The Netherlands. 2. Radboud University, FELIX Laboratory, Institute of Molecules and Materials, Toernooiveld 7, 6525 ED Nijmegen, The Netherlands.
Abstract
A detailed understanding of the reaction mechanism(s) leading to stereoselective product formation is crucial to understanding and predicting product formation and driving the development of new synthetic methodology. One way to improve our understanding of reaction mechanisms is to characterize the reaction intermediates involved in product formation. Because these intermediates are reactive, they are often unstable and therefore difficult to characterize using experimental techniques. For example, glycosylation reactions are critical steps in the chemical synthesis of oligosaccharides and need to be stereoselective to provide the desired α- or β-diastereomer. It remains challenging to predict and control the stereochemical outcome of glycosylation reactions, and their reaction mechanisms remain a hotly debated topic. In most cases, glycosylation reactions take place via reaction mechanisms in the continuum between SN1- and SN2-like pathways. SN2-like pathways proceeding via the displacement of a contact ion pair are relatively well understood because the reaction intermediates involved can be characterized by low-temperature NMR spectroscopy. In contrast, the SN1-like pathways proceeding via the solvent-separated ion pair, also known as the glycosyl cation, are poorly understood. SN1-like pathways are more challenging to investigate because the glycosyl cation intermediates involved are highly reactive. The highly reactive nature of glycosyl cations complicates their characterization because they have a short lifetime and rapidly equilibrate with the corresponding contact ion pair. To overcome this hurdle and enable the study of glycosyl cation stability and structure, they can be generated in a mass spectrometer in the absence of a solvent and counterion in the gas phase. The ease of formation, stability, and fragmentation of glycosyl cations have been studied using mass spectrometry (MS). However, MS alone provides little information about the structure of glycosyl cations. By combining mass spectrometry (MS) with infrared ion spectroscopy (IRIS), the determination of the gas-phase structures of glycosyl cations has been achieved. IRIS enables the recording of gas-phase infrared spectra of glycosyl cations, which can be assigned by matching to reference spectra predicted from quantum chemically calculated vibrational spectra. Here, we review the experimental setups that enable IRIS of glycosyl cations and discuss the various glycosyl cations that have been characterized to date. The structure of glycosyl cations depends on the relative configuration and structure of the monosaccharide substituents, which can influence the structure through both steric and electronic effects. The scope and relevance of gas-phase glycosyl cation structures in relation to their corresponding condensed-phase structures are also discussed. We expect that the workflow reviewed here to study glycosyl cation structure and reactivity can be extended to many other reaction types involving difficult-to-characterize ionic intermediates.
A detailed understanding of the reaction mechanism(s) leading to stereoselective product formation is crucial to understanding and predicting product formation and driving the development of new synthetic methodology. One way to improve our understanding of reaction mechanisms is to characterize the reaction intermediates involved in product formation. Because these intermediates are reactive, they are often unstable and therefore difficult to characterize using experimental techniques. For example, glycosylation reactions are critical steps in the chemical synthesis of oligosaccharides and need to be stereoselective to provide the desired α- or β-diastereomer. It remains challenging to predict and control the stereochemical outcome of glycosylation reactions, and their reaction mechanisms remain a hotly debated topic. In most cases, glycosylation reactions take place via reaction mechanisms in the continuum between SN1- and SN2-like pathways. SN2-like pathways proceeding via the displacement of a contact ion pair are relatively well understood because the reaction intermediates involved can be characterized by low-temperature NMR spectroscopy. In contrast, the SN1-like pathways proceeding via the solvent-separated ion pair, also known as the glycosyl cation, are poorly understood. SN1-like pathways are more challenging to investigate because the glycosyl cation intermediates involved are highly reactive. The highly reactive nature of glycosyl cations complicates their characterization because they have a short lifetime and rapidly equilibrate with the corresponding contact ion pair. To overcome this hurdle and enable the study of glycosyl cation stability and structure, they can be generated in a mass spectrometer in the absence of a solvent and counterion in the gas phase. The ease of formation, stability, and fragmentation of glycosyl cations have been studied using mass spectrometry (MS). However, MS alone provides little information about the structure of glycosyl cations. By combining mass spectrometry (MS) with infrared ion spectroscopy (IRIS), the determination of the gas-phase structures of glycosyl cations has been achieved. IRIS enables the recording of gas-phase infrared spectra of glycosyl cations, which can be assigned by matching to reference spectra predicted from quantum chemically calculated vibrational spectra. Here, we review the experimental setups that enable IRIS of glycosyl cations and discuss the various glycosyl cations that have been characterized to date. The structure of glycosyl cations depends on the relative configuration and structure of the monosaccharide substituents, which can influence the structure through both steric and electronic effects. The scope and relevance of gas-phase glycosyl cation structures in relation to their corresponding condensed-phase structures are also discussed. We expect that the workflow reviewed here to study glycosyl cation structure and reactivity can be extended to many other reaction types involving difficult-to-characterize ionic intermediates.
.[1] The first report on the
characterization of glycosyl cations using infrared ion spectroscopy..[2] A mechanistic study of the reaction mechanism(s)
of glycosyl cations derived from conformationally locked uronic acids..[3] A systematic study of the ability of acyl groups to participate
in the stabilization of glycosyl cations.
Introduction
Glycosylation, the expression of carbohydrate structures (glycans)
on proteins and lipids, is found in all domains of life.[4] The collection of all glycans found on a cell
is called the “glycome”, which is rich in information
and a key player in a plethora of physiological and pathological processes.[5] The information contained within the glycome
can be written, read, and erased by glycosyltransferases, lectins,
and glycosidases, respectively. Glycans are structurally very diverse
because they are composed of different monosaccharides which, when
connected, give rise to different regio- and stereoisomers producing
long, short, branched, and linear glycans that can attach to a protein
and/or lipid carrier.[6] Similar to genomics
for DNA and proteomics for proteins, “glycomics” is
the study that seeks to identify and understand the structure and
function of specific glycans in biological processes. Genomics and
proteomics have benefited from the availability of advanced molecular
biology methods and the availability of well-defined synthetic standards
prepared using automated solid-phase synthesis methodology. Because
their biosynthesis is not under direct genetic control, glycans are
expressed in microheterogeneous forms, challenging their isolation
and characterization from a biological sample. Hence, in many cases
well-defined oligosaccharides can be obtained only by chemical or
enzymatic synthesis.[7] The chemical synthesis
of glycans is challenging because of the structural diversity and
complexity of this class of molecules. The monosaccharide constituents
of glycans are connected to each other at the anomeric center via
an acetal linkage termed the glycosidic bond. Glycosidic bonds can
exist as two anomers (equatorial and axial), and the anomeric stereochemistry
is usually defined relative to the C-2 substituent, 1,2-cis or 1,2-trans, or relative to the last chiral substituent
on the carbohydrate chain (α or β).[8]Glycosidic bonds are synthesized in so-called glycosylation
reactions,
which can be described as a nucleophilic substitution reaction between
a glycosyl donor carrying an anomeric leaving group and a glycosyl
acceptor containing a nucleophilic alcohol. Controlling the diastereoselectivity
of glycosylation reactions is the major challenge in oligosaccharide
synthesis and is achieved by the application of two main strategies.[9] First, an acyl group at the C-2 position of the
glycosyl donor can be used to trap the glycosyl cation formed after
the departure of the leaving group, affording a dioxolanium ion (Scheme A). The displacement
of this dioxolanium ion by the glycosyl acceptor affords 1,2-trans glycosides with high stereoselectivity.[10] In general, the use of a 2-O-acyl functionality to synthesize 1,2-trans glycosides
is very reliable and highly stereoselective and can be applied to
solid-phase oligosaccharide synthesis.[11] In the case of d-gluco-type donors, β-linked products
are obtained, whereas d-manno-type donors give α-linked
products. Furthermore, this strategy is also applicable to the synthesis
of 2-deoxy-2-amino-glycosides using amine-protecting groups that can
engage in neighboring group participation (NGP). The participation
of acyl functionalities further away from the anomeric center, i.e.,
placed on the C-3, C-4, or C-6 hydroxyl groups, has also been suggested
to direct the stereoselectivity of glycosylation reactions (Scheme B). This potentially
allows for the utilization of the relative stereochemistry of C-3,
C-4, or C-6 groups to control the facial selectivity in glycosylation
reactions, thereby enabling the stereoselective synthesis of C-2-deoxy
and 1,2-cis-glycosides. However, contradictory results
have been reported, and there is an ongoing debate as to the role
and strength of this stereoelectronic effect.[12]
Scheme 1
Stereoselective Glycosylation via (A) the Neighboring Group Participation
of a C-2 Acyl Group and (B) the Neighboring Group Participation of
a C-3 Acyl Group and (C) the Glycosylation Mechanisms of Glycosyl
Triflate Intermediates
The second main strategy is utilizing glycosyl donors that do not
contain protecting groups capable of participation (Scheme C).[13,14] In this case, the glycosyl cation is trapped by the triflate counterion,
resulting from most promoter systems, leading to an α- or β-glycosyl
triflate. The mechanism of glycosylation reactions proceeding via
these intermediates continues to be a topic of much research and takes
place in the continuum between SN1-like and SN2-like reaction pathways.[15] Reactions
with the glycosyl acceptor can take place via a dissociative (SN1) or associative (SN2) substitution reaction.
Glycosyl triflates can be characterized by low-temperature NMR and
have been shown to be reactive intermediates via SN2-like
pathways, leading to stereospecific reactions affording the opposite
diastereomer as the main product. In some cases, the observed glycosyl
triflate affords a product with retention of the anomeric configuration,
which cannot be explained by an SN2-like pathway. In these
cases, reactions are expected to take place via other reaction intermediates
that are in rapid equilibrium with the observed α-glycosyl triflate
following the Curtin–Hammett principle. Likely candidates in
this respect are the glycosyl oxocarbenium ion and β-glycosyl
triflate (Scheme C).Hence, to better understand the mechanistic pathways of glycosylation
reactions, identification of the structures of all reactive intermediates
is crucial. However, the intrinsic high reactivity, short lifetime,
and equilibrium with the corresponding contact ion pair complicates
the characterization of low-abundance reactive intermediates. This
challenge has recently been addressed by trapping the oxocarbenium
ion in a superacidic medium, which enabled the recording of NMR spectra
of glycosyl cations derived from 3,4,6-tri-O-acetyl-2-deoxy-glucosides.[16] Under superacidic conditions, all acetyl groups
were protonated, thereby disabling the assessment of their ability
to stabilize the cationic center. Glycosyl cations have also been
generated using mass spectrometry in the absence of solvent and counterions,
offering unique conditions for studying the stability and reactivity
of these intermediates.[17−20] Although the information that can be extracted from
a single mass measurement is limited, various forms of tandem mass
spectrometry provide a means of determining the structural details. Infrared ion spectroscopy (IRIS) has emerged as a powerful
method for characterizing molecular ions in the gas phase, and we
and others have applied this technique to elucidate the structure
of glycosyl cations.[1,21]Herein, we review the recent
developments in the use of mass spectrometry
to generate glycosyl cations and the use of IRIS to characterize them
spectroscopically. The main types of instrumentation will be discussed,
including their capabilities, differences, and limitations. An overview
of glycosyl cations characterized thus far using IRIS is provided.
The structural insights from IRIS applied to glycosyl ion structure
is discussed along with its relevance to glycosyl cations as reactive
intermediates in the condensed phase. We note that in parallel there
have been strong efforts to apply IRIS in the chemical analysis of
glycans, but this is beyond the scope of the present review.[22−27]
Investigating
Glycosyl Cations Using Mass Spectrometry
The introduction
of soft-ionization sources for mass spectrometry,
in particular, electrospray ionization (ESI) and matrix-assisted laser
desorption ionization (MALDI), enabled gas-phase studies of intact
labile molecular ions using mass spectrometry.[28,29] The ESI process is often referred to as a means to directly transfer
ions from solution to the gas phase and is now used extensively to
study systems ranging from small molecules to entire protein complexes
(Figure A).[30,31] Such gas-phase studies offer a unique environment for examining
factors influencing the structure, stability, and reactivity of glycosyl
cations under controlled, isolated conditions. Although the amount
of structural information that can be extracted from a mass-to-charge
ratio (m/z) measurement is limited,
various forms of tandem mass spectrometry (MS/MS) have been used to
complement m/z information with
indirect structural and reactivity information. Tandem mass spectrometry
involves the activation of a mass-selected ion population in order
to induce fragmentation reactions, which are often unique for different
molecular species that are inseparable on the basis of m/z.[32,33] Here we will focus on “in-source”
fragmentation, where all ions are accelerated and collisionally activated
in a region of the mass spectrometer where high-vacuum conditions
are not yet reached (Figure B), and mass-isolated collision-induced dissociation (CID),
where ions of a specific mass are selected and fragmented separately
from ions of other masses (Figure C). CID has the advantage that mass isolation prior
to fragmentation allows for the direct correlation of fragment ions
to an individual precursor ion.
Figure 1
(A) Principle of electrospray ionization.
(B) Direct in-source
formation of a glycosyl cation. (C) Formation of a glycosyl cation
through CID.
(A) Principle of electrospray ionization.
(B) Direct in-source
formation of a glycosyl cation. (C) Formation of a glycosyl cation
through CID.In 2005, Denekamp and co-workers
performed pioneering mass spectrometry
experiments investigating the generation and stability of glycosyl
cations. Peracetylated α- and β-hexoses were ionized and
fragmented using CID.[17] Peracetylated β-anomers
with a 1,2-trans relative stereochemistry most readily
underwent fragmentation toward a glycosyl cation, presumably resulting
from the departure of the anomeric leaving group. This high reactivity
was attributed to the ability of the C-2 ester to directly perform
neighboring group participation in this specific configuration (Scheme A). Additionally,
the relative stereochemistry at C-4 was investigated, with galactose
fragmenting more readily to the glycosyl ion than glucose and mannose.
In subsequent work, the same authors evaluated the effect of the nature
of the protecting and leaving groups on glycosyl cation formation
and the stabilization of a series of glycopyranosyl thioglycosides
(Scheme B).[18] Glycosyl cations were observed after CID of
the parent ammonium adducts bearing protecting groups capable of NGP
(Bz or Ac). Despite their electron-withdrawing character, these acyl
groups were shown to stabilize the oxocarbenium ion effectively through
π-overlap. Conversely, the presence of ether protecting groups
lacking this favorable overlap was shown to hamper glycosyl cation
formation. The ease of glycosyl cation formation correlated with the
protecting group pattern used at the C-2 and/or C-4 position and was
found to be Bz > Ac > (CH3)3Si > alkyl.
When
a series of thioaryl leaving groups were compared, only a modest effect
on glycosyl cation formation was found.
Scheme 2
(A) Formation of
glycosyl cations from acetylated glycoside precursors
using CID (RA = Relative Abundance of the Glycosyl Cation Fragment),
(B) Influence of the Protecting Group Nature on Glycosyl Cation Formation,
(C) Influence of Protecting Groups and Their Dipole Moment on the
Energetics of Sialyl Oxocarbenium Ions, and (D) Evaluation of the
Effects of Linkage Stereochemistry, Leaving Group Geometry, and Protecting
Group Pattern on the Stability of the Glycosyl Linkage Using Survival
Yield Analysis
Crich et al. used
the in-source fragmentation of sialoside donors
to produce the corresponding glycosyl cations to measure sialyl donor
reactivity (Scheme C).[19] To this end, threshold fragmentation
energies of a series of sialoside donors carrying 4,5-N-acetyl oxazolidinone, 4,5-oxazolidinone, or carbonate protecting
groups were investigated. The use of cyclic protecting groups necessitated
higher excitation energies (in-source cone voltage) to induce fragmentation
toward the glycosyl cation. This effect was attributed to the electron-withdrawing
abilities of the oxazolidinone and cyclic carbonates by the alignment
of a single large dipole antiparallel to the mean plane of the pyranose
ring. Hence, it was concluded that cyclic protecting groups retarded
the formation of the glycosyl cation and instead promoted associative
reaction mechanisms.More recently, Rodgers et al. studied the
influence of the anomeric
configuration and protecting group pattern on the stability of the
glycosidic bond.[20] To this end, the sodium
adducts of eight glycosyl phosphates were examined via survival yield
analysis based on their CID fragmentation toward glycosyl cations
(Scheme D). They found
that the relative C1–C2 stereochemistry is a major factor affecting
the stability of the glycosidic bond. Greater stability was found
for 1,2-cis anomers than for their respective 1,2-trans anomers. The
glycosidic bond cleavage of 1,2-cis-glycosyl phosphates
was therefore hypothesized to proceed via an oxocarbenium ion intermediate,
whereas the cleavage of 1,2-trans isomers takes place
via a syn elimination mechanism akin to a McLafferty type rearrangement.
Furthermore, it was found that cyclic protecting groups stabilize
the glycosidic bond of 1,2-cis anomers while activating the bond of
the 1,2-trans anomers. The same effect was found when a C-3 BnO substituent
is present, whereas no significant effect on bond stability was found
for the C-2 BnO substituent.Although such gas-phase MS studies
provide interesting fundamental
observations that may suggest aspects of reactivity that can be extended
to the condensed phase, a major limitation is that no direct structural
information is obtained for the glycosyl cations produced. Generating
a fundamental understanding of the underlying chemical reactivity
requires a clearer picture of the glycosyl cation structure. The use
of MS in combination with IRIS has therefore emerged as a powerful
method for assigning molecular structures to ions observed in MS experiments.[26,27,34−38] In this Account, we focus on the extra dimension
that is obtained by combining MS with IR spectroscopy in search of
a better understanding of the chemical glycosylation mechanism.
Infrared Ion Spectroscopy (IRIS)
The challenge to obtaining
IR spectra of gaseous, mass-selected molecular ions lies in the extremely
low densities of ions in any type of tandem mass spectrometer (≪106 cm–3), which precludes the application
of direct absorption spectroscopy using conventional (FT)IR spectrometers.
Various action spectroscopy methods have been developed to overcome
these challenges.IR multiple-photon dissociation (IRMPD) spectroscopy
was originally developed in the early 1990s by employing Fourier transform
ion cyclotron resonance (FTICR) mass spectrometers and CO2 lasers that were line-tunable at wavelengths between 9 and 11 μm
(Figure A).[39−41] Irradiating the mass-selected ion cloud inside the ICR cell while
the laser frequency is being tuned induces precursor ion dissociation
whenever the laser frequency is resonant with a vibrational band of
the investigated ion. Simultaneously, a series of mass spectra are
recorded to enable the detection of ion fragmentation. By plotting
the fractional ion dissociation as a function of laser frequency,
an IR spectrum can be reconstructed (Figure A). Because the dissociation threshold is
much higher than the photon energy, sizable laser powers are required
to drive multiple-photon absorption. Because of the limited analytical
usefulness of the CO2 laser wavelength range, the technique
would likely have fallen into oblivion if it were not for the advent
of widely tunable IR lasers in the early 2000s, in particular, IR
free-electron lasers (FELs) and OPO/OPA systems. Currently, IR FEL
facilities at Radboud University (FELIX), Université Paris-Sud
(CLIO), and the Fritz-Haber Institute (FHI-FEL) are routinely used
for ion spectroscopy in the fingerprint IR range (∼500 to 2000
cm–1), and many groups employ table-top OPO sources
to cover the X–H stretching range between 2500 and 4000 cm–1. The IRMPD process relies on rapid intramolecular
vibrational redistribution (IVR) during the IR-induced activation
of the ion. The gradual heating of the system during the sequential
absorption of multiple photons typically causes a small red shift
(a few cm–1) and broadening of the vibrational band
as compared to a linear absorption spectrum.[42,43]
Figure 2
(A)
Principle of IRMPD spectroscopy at ambient temperature. (B)
Principle of helium nanodroplet spectroscopy at 0.37 K.
(A)
Principle of IRMPD spectroscopy at ambient temperature. (B)
Principle of helium nanodroplet spectroscopy at 0.37 K.To mitigate the band broadening associated with IRMPD spectroscopy,
linear (one-photon) action spectroscopy can be achieved by attaching
a weakly bound tag to the species under investigation that serves
as a “messenger” reporting on the absorption of an IR
photon.[44] The binding energy of the tag
should be lower than the IR photon energy, and the tag should minimally
alter the IR fingerprint of the analyte, making rare gas (Rg) atoms
favorable tags. To stabilize the [M + Rg]+ ion, cryogenic
temperatures are required. Resonant excitation of the [M + Rg]+ ion by a single IR photon induces tag detachment, which is
monitored in the MS as an m/z shift.
Even lower temperature spectroscopy can be achieved using He nanodroplets,
which are clusters of thousands of He atoms that have been employed
for spectroscopic experiments since the early 1990s (Figure B).[45−47] The He nanodroplets
are at 0.37 K, and their superfluidity provides the ultimate noninteracting
matrix environment. The droplets are produced in a supersonic expansion
through a cold nozzle and can contain between 102 and 106 He atoms depending on the backing pressure and nozzle temperature.
The droplets pick up gaseous molecules that they encounter, and these
analytes quickly thermalize to 0.37 K by the evaporation of He atoms,
thus becoming embedded within the He droplet. Various methods have
been devised to study the spectroscopy of ionized molecules embedded
in He droplets.[48,49] In the implementation of von
Helden and co-workers, a pulsed nozzle at 15–25 K produces
He droplets in the size range of 104–106 atoms.[25] They travel through a linear
hexapole RF ion trap at 80 K containing the thermalized and mass-selected
ions of interest. In the trap, droplets pick up an ion and continue
their journey toward the extraction zone of a time-of-flight mass
spectrometer (TOF-MS). Here, an FEL pulse irradiates the droplets,
and resonant absorption by the embedded ion causes its ejection from
the droplet and its detection in the TOF-MS. The measured spectra
sample the ion at very low temperature, greatly reducing the number
of quantum states and conformations populated, and typically provide
better spectral resolution than IRMPD spectra (Figure B).To extract information on molecular
structure from experimental
IR spectra, they can be matched to reference spectra either measured
from chemical standards or predicted from quantum chemically calculated
vibrational spectra. Workflows to generate predicted IR spectra typically
involve a large set of candidate geometries for a specific glycosyl
cation isomer that reflects all possible conformations and modes of
intramolecular stabilization.[50,51] After a low-level geometry
optimization, often using molecular mechanics, a number of low-energy
structures are selected. The selected geometries are then optimized
at the density functional theory (DFT) level, and their predicted
IR spectra and Gibbs free energies are computed. Electronic energies
are usually also computed at higher levels of theory to give more
accurate relative energies. Predicted IR spectra of the lowest-energy
conformations are then compared to the experimental spectrum, facilitating
the structural assignment of the glycosyl cation. Especially for comparison
with IRMPD spectra, assignments are mainly based on peak positions
(cm–1) because IRMPD band intensities may deviate
somewhat from computed linear IR intensities.
Characterization of Glycosyl
Cations Using IRIS
Our
first IRIS-based characterization of glycosyl cations potentially
involved in glycosylation reactions focused on glycosyl cations that
were generated by CID MS/MS from mannosides modified with methyl (Figure A) or acetyl (Figure B) protecting groups.[1] In the case of the permethylated mannoside, the
IR spectrum showed a vibrational characteristic for the anomeric carbonylonium
C=O+–C stretch (∼1609 cm–1, Figure A). The
experimental spectrum (Figure A, black line) could be matched to the DFT-calculated spectrum
(Figure A, color fill)
of the mannosyl oxocarbenium ion in the 3E conformation.
Figure 3
Comparison
of computed IR spectra (filled gray) and measured IRMPD
spectra (black line). IRMPD spectra of (A) a mannosyl oxocarbenium
ion and (B) a mannosyl dioxolanium ion.
Comparison
of computed IR spectra (filled gray) and measured IRMPD
spectra (black line). IRMPD spectra of (A) a mannosyl oxocarbenium
ion and (B) a mannosyl dioxolanium ion.In contrast, a mannoside donor modified with acetyl protecting
groups formed a glycosyl dioxolanium ion by the participation of the
C-2 acetyl group (Figure B). This was observed from the IR spectrum as the interaction
of a participating group with the anomeric center leading to the disappearance
of the anomeric carbonylonium C=O+ stretch. Instead,
O–C+–O and C+–CH3 stretching modes (∼1540 and ∼1495 cm–1) characteristic of the formation of a bicyclic glycosyl dioxolanium
ion were observed. C=O stretching vibrations of the nonparticipating
acetyl esters appeared at higher wavenumbers (1700–1800 cm–1). At lower wavenumbers (700–1500 cm–1), a large number of bands were observed, including many that are
diagnostic in deciding on the best match of the experimental (Figure B, black line) versus
DFT calculated spectrum (Figure B, color fill).The first example of helium nanodroplet
spectroscopy to characterize
glycosyl cations was reported by Pagel et al. and presents the IRIS
spectra of glycosyl cations originating from gluco-, galacto-, and
mannosides containing a C-2 acetyl group.[21] NGP of the C-2 ester was confirmed for all three glycosyl cations
as well as finer structural details observable as a result of the
exquisite spectral resolution of the helium nanodroplet method.[21] However, the structural assignment of the galactosyl
cation was impeded by a more congested fingerprint region presumable
due to coexisting dioxolanium ion conformers. Coexisting ring conformations
in the unprotected galactosyl cations were further explored by Dvores
et al. by combining IRMPD spectroscopy with more advanced computational
approaches.[52] Their simulations were unable
to definitively assign the oxocarbenium ion but did indicate that
a rapid conversion between ring conformations should occur at room
temperature.Subsequent studies focused on probing the contribution
of protecting
groups at more remote positions in shaping glycosyl cation structures.
We explored the use of IRIS to investigate glycosylation reactions
of 6,3-uronic acid lactones. We previously observed that conformationally
locked 6,3-mannuronic acid lactones reacted with very high β-selectivity.[2,53] However, glycosyl donors carrying a C-4 benzyl substituent (1) provided β-glycosides in very low yields because
a 1,4-anhydrosugar (5) was formed as the major product
(Scheme A).[53] The lactone bridge presumably leads to β-selective
oxocarbenium ion conformer 3 but also allows for the
participation of the C-4 benzyl ether (4), which upon
loss of benzyl triflate affords 1,4-anhydrosugar 5 (Scheme A). To prevent anhydrosugar
formation, we prepared donors 6–9 carrying a C-4 O-acetyl or O-methyl
group (Scheme B).[2] The structures of the corresponding glycosyl
cations were determined using IRIS. The thioglycoside leaving group
was oxidized to the sulfoxide in the case of 6 and 8 to avoid overlap in fragmentation channels. Cations resulting
from methylated uronic acid lactones 7 and 9 were characterized as oxocarbenium ions, even though the calculated
minimum-energy conformation involved the participation of the C-4 O-methyl group (Scheme B). In the case of the C-4 O-acetyl-modified
donors (7 and 9), stabilization of the cationic
center by the C-4 acetyl group was observed (Scheme B).[2] The absence
of solvent and a counterion in the gas phase is expected to drive
intramolecular stabilization, which may not necessarily occur in solution.
Hence, care needs to be taken in interpreting the relevance of glycosyl
cation structures obtained using MS and characterized by IRIS. Indeed,
VT-NMR experiments of mannosyl donor 10 showed the sole
formation of β-glycosyl triflate 11 upon activation
(Scheme C). The participation
of the C-4 O-acetyl or O-methyl
groups could not be detected by NMR. However, because the β-glycoside
product is obtained upon addition of a nucleophile, the β-glycosyl
triflate is not a reactive intermediate via an SN2-like
pathway. Hence, β-glycoside formation is expected to occur via
oxocarbenium ion 12 or an α-triflate intermediate
(Scheme C).
Scheme 3
(A) Proposed
Intermediates in the Reaction of 4-Benzyl-6,3-uronic
Acid Mannolactones, (B) Overview of Characterized Glycosyl Cations
Derived from 6,3-Uronic Acid Lactone Donors (6 and 8, LG = SOPh; 7 and 9, LG = SPh),
and (C) Proposed Intermediates in the Reaction of 4-Acetyl-6,3-uronic
Acid Mannolactones
The participation
of C-4 acyl groups on the 15–18 series
of galactoside donors was investigated using the
FHI-FEL technique and was reported by Pagel et al.[51] Galactosides 17 and 18, each
carrying a C-4 acetyl group, formed a bridged glycosyl cation involving
the stabilization of the cationic center by C-4 NGP (Scheme ). Glycosyl cations 17a and 18a adopted a 1S5 ring conformation
wherein the C-4-acetyl group participates. In contrast, glycosyl cations
formed from C-6 acetylated donor 15 and perbenzylated
donor 16 showed unexpected evidence for the presence
of one or both oxonium (1,4B) and oxocarbenium intermediates
with a heavily distorted ring pucker (5S1).
Solution-phase experiments were also performed to investigate the
impact of different protecting group combinations on the stereochemical
outcome of the glycosylation reaction. Galactosyl imidates carrying
a C-4 acetyl group (17 and 18) showed a
consistently higher α-selectivity than building blocks lacking
an acetyl group at this position (15 and 16). This observation suggests that the reaction intermediates involved
are different. Whether C-4 acyl participation occurs in the condensed
phase remains to be investigated.[12] In
a recent low-temperature NMR study reported by Crich et al., only
the glycosyl triflate intermediate was found upon activation of a
4-O-benzoyl galactopyranosyl donor. Methylation at
the 4-position resulted in a more conformationally labile tertiary
ester, effectively lowering the barrier to participation, and only
in this case was participation of the C-4 ester observed.[54]
Scheme 4
Overview of Characterized Glycosyl Cations
Derived from Galactosides
Using He Nanodroplet Spectroscopy
15–18, LG = TCAI.
Overview of Characterized Glycosyl Cations
Derived from Galactosides
Using He Nanodroplet Spectroscopy
15–18, LG = TCAI.To systematically investigate
the role of acyl groups on the glycosyl
donor in the stabilization of glycosyl cations, gluco-, galacto-,
and mannosyl donors 22–24 carrying
a single ester at the C-2, C-3, C-4, or C-6 position were investigated.
Pagel et al. reported the structures of C-2 acyl-stabilized glycosyl
cations (22a, 23a, and 24a/b), and the exact conformation of the pyranose ring was determined
(Scheme ).[21] The participation of the C-2 ester in glucose
induces a 3S1 ring conformation (22a), and the mannosyl cation adopts a B0,3 conformation
(23a). The structural assignment of the galactosyl cation
was impeded by a more congested fingerprint region, but coexisting
dioxolanium ions bearing distinct ring conformations 4E
(24a) and 1S3 (24b) were proposed. Subsequently, we characterized the full set of glucose,
mannose, and galactose cations substituted with a single acetyl ester
at the C-3, C-4, or C-6 position.[3] IRIS
afforded highly diagnostic spectra because acetyl participation led
to the disappearance of its C=O stretch in the IR spectrum.
The participation of the C-3 position was observed for all donors,
leading to the formation of glycosyl dioxanium ions (25a–27a, Scheme ). In contrast, the IRIS spectra of glycosyl cations
derived from donors carrying a C-6 ester all featured a C=O
stretch. However, a dioxolanium ion signature was also observed, which
is inconsistent with the formation of an unstabilized oxocarbenium
ion. Careful analysis using DFT calculations indicated that ring opening
had likely occurred by the participation of the C-6 ester at C-5.
This affords a dioxolanium ion signature and a C=O stretch
corresponding to the C-1 aldehyde (Scheme ). Participation of the C-4 acetyl ester
was observed for glucoside 30 and galactoside 28, but ring opening was observed for mannoside 29 (Scheme ).
Scheme 5
Overview of Glycosyl
Cations Characterized from Monoacetyl Glycoside
Precursors
22–24, LG = SEt; 25 and 30, LG = SPh; 26–29, LG = SOPh.
Overview of Glycosyl
Cations Characterized from Monoacetyl Glycoside
Precursors
22–24, LG = SEt; 25 and 30, LG = SPh; 26–29, LG = SOPh.The relevance of the observed gas-phase glycosyl cations may be
debated because gas-phase conditions drive the internal stabilization
via LRP, which may not necessarily occur under typical glycosylation
conditions. Moreover, ions characterized by IRIS likely represent
the most stable ions but give little information about the access
to other low-energy structures that are more accessible in the condensed
phase. To bridge the gap between the gas phase and solution, a full
conformational energy landscape (CEL) of all glycosyl cations in their
unstabilized (oxocarbenium ion) and stabilized (ester participation)
forms was calculated for both gas-phase and solution-phase conditions.[3,55] The CEL maps revealed that for the mannosyl cation carrying a C-3 O-acetyl ester, the energy difference between the oxocarbenium
and dioxanium ion forms was greatest, whereas they were close in conformational
space. Hence, because of these factors, the strength of internal stabilization
was expected to be high for mannose but smaller for the glucose and
galactose derivatives. Consistent with this hypothesis, glycosylations
with C-3 O-benzoyl mannosides were found to be highly
α-selective irrespective of the nucleophile strength (Scheme A).[56] Even though C-3 participation was observed in the gas phase
for glucoside 25 and galactoside 27, the
extent of stabilization by DFT calculations was moderate and is also
reflected in more aselective glycosylation reactions (Scheme A).
Scheme 6
(A) Experimentally
Determined Stereoselectivities for Model Glycosylations
of C-3 Acyl Glycosides and (B) Detection
of the Dioxanium Ion via CEST-NMR
(A) Experimentally
Determined Stereoselectivities for Model Glycosylations
of C-3 Acyl Glycosides and (B) Detection
of the Dioxanium Ion via CEST-NMR
HFIP = 1,1,1,3,3,3-hexafluoro-2-propanol,
TFE = 2,2,2-trifluoroethanol, DFE = 2,2-difluoroethanol, and MFE =
2-fluoroethanol.Hence, only for mannose do
we expected dioxanium ion 26a to play a role in the glycosylation
reaction. Recently, we were
able to demonstrate the presence of the mannosyl dioxanium ion (34) in solution via chemical exchange saturation transfer
NMR and establish its exchange kinetics with respect to the α-glycosyl
triflate (Scheme B).[55] The kinetics are consistent with a reaction
operating under the Curtin–Hammett principle because the interconversion
between the dioxanium ion and α-glycosyl triflate occurs much
faster than the reaction of α-triflate with the nucleophile.
This not only confirms the relevance of the glycosyl cation in glycosylation
reactions but also shows how selectivity can be achieved through the
formation of the dioxanium ion, as was suggested earlier on the basis
of IRIS and CEL maps.The case of the C-3 O-acyl mannosides illustrates
that the powerful combination of ion spectroscopy, DFT calculations,
and solution-phase experiments goes beyond probing the structure of
reactive intermediates. Through careful interpretation, this combination
can also provide boundary conditions as to what intermediates can
be expected in solution. It is therefore anticipated that the application
of ion spectroscopy will be extended to other relevant reactive species.[34,57−59] Also, the emergence of more sophisticated spectroscopy
schemes and hyphenation separates these isomers on the basis of their
collisional cross-sections.[60,61] Alternatively, more
sophisticated spectroscopic schemes can be employed to quantify and
disentangle coexisting isomers by isomer-selective laser dissociation
using vibrational bands that are isomer-specific.[62] The combined efforts of these different approaches will
provide a comprehensive understanding of reaction mechanisms and can
provide guidelines for the development of new synthetic strategies.
Authors: Yoshiki Narimatsu; Hiren J Joshi; Rebecca Nason; Julie Van Coillie; Richard Karlsson; Lingbo Sun; Zilu Ye; Yen-Hsi Chen; Katrine T Schjoldager; Catharina Steentoft; Sanae Furukawa; Barbara A Bensing; Paul M Sullam; Andrew J Thompson; James C Paulson; Christian Büll; Gosse J Adema; Ulla Mandel; Lars Hansen; Eric Paul Bennett; Ajit Varki; Sergey Y Vakhrushev; Zhang Yang; Henrik Clausen Journal: Mol Cell Date: 2019-06-18 Impact factor: 17.970
Authors: Fred A M G van Geenen; Ruben F Kranenburg; Arian C van Asten; Jonathan Martens; Jos Oomens; Giel Berden Journal: Anal Chem Date: 2021-01-20 Impact factor: 6.986
Authors: Eike Mucha; Mateusz Marianski; Fei-Fei Xu; Daniel A Thomas; Gerard Meijer; Gert von Helden; Peter H Seeberger; Kevin Pagel Journal: Nat Commun Date: 2018-10-09 Impact factor: 14.919
Authors: Wouter A Remmerswaal; Kas J Houthuijs; Roel van de Ven; Hidde Elferink; Thomas Hansen; Giel Berden; Herman S Overkleeft; Gijsbert A van der Marel; Floris P J T Rutjes; Dmitri V Filippov; Thomas J Boltje; Jonathan Martens; Jos Oomens; Jeroen D C Codée Journal: J Org Chem Date: 2022-06-24 Impact factor: 4.198