Glycan analysis has evolved considerably during the last decade. The advent of high-resolution ion-mobility spectrometry has enabled the separation of isomers with only the slightest of structural differences. However, the ability to separate such species raises the problem of identifying all the mobility-resolved peaks that are observed, especially when analytical standards are not available. In this work, we report an approach based on the combination of IMSn with cryogenic vibrational spectroscopy to identify N-glycan reducing-end anomers. By identifying the reducing-end α and β anomers of diacetyl-chitobiose, which is a disaccharide that forms part of the common core of all N-glycans, we are able to assign mobility peaks to reducing anomers of a selection of N-glycans of different sizes, starting from trisaccharides such as Man-1 up to glycans containing nine monosaccharide units, such as G2. By building an infrared fingerprint database of the identified N-glycans, our approach allows unambiguous identification of mobility peaks corresponding to reducing-end anomers and distinguishes them from positional isomers that might be present in a complex mixture.
Glycan analysis has evolved considerably during the last decade. The advent of high-resolution ion-mobility spectrometry has enabled the separation of isomers with only the slightest of structural differences. However, the ability to separate such species raises the problem of identifying all the mobility-resolved peaks that are observed, especially when analytical standards are not available. In this work, we report an approach based on the combination of IMSn with cryogenic vibrational spectroscopy to identify N-glycan reducing-end anomers. By identifying the reducing-end α and β anomers of diacetyl-chitobiose, which is a disaccharide that forms part of the common core of all N-glycans, we are able to assign mobility peaks to reducing anomers of a selection of N-glycans of different sizes, starting from trisaccharides such as Man-1 up to glycans containing nine monosaccharide units, such as G2. By building an infrared fingerprint database of the identified N-glycans, our approach allows unambiguous identification of mobility peaks corresponding to reducing-end anomers and distinguishes them from positional isomers that might be present in a complex mixture.
Glycosylation is one of the most common
post-translational modifications
of proteins and plays a central role in their functioning. For example,
the glycosylation pattern of biological drugs, such as monoclonal
antibodies, directly affects their efficacy, toxicity, and shelf life
and is considered a critical quality attribute by regulatory agencies.[1,2] Changes in the glycosylation pattern of cell–surface proteins
have been used as biomarkers for breast, colon, and ovarian cancer;
liver disease; and neurodegenerative diseases such as Alzheimer’s
and Parkinson’s.[3−9]Despite their biological importance, glycans represent one
of the
most difficult classes of molecules to analyze, arising from the isomeric
complexity of their monosaccharide building blocks as well as the
stereochemistry of the glycosidic linkages. While nuclear magnetic
resonance (NMR) can provide information on glycan primary structure
and stereochemistry, its application requires sufficient quantities
of pure samples, which is often challenging to obtain.[10] Liquid chromatography coupled with mass spectrometry
(LC–MS) has been considered the workhorse technique for the
analysis of complex glycan samples owing to its high sensitivity.[11,12] Nevertheless, LC–MS workflows are not sufficient to separate
and identify all glycan isomers unambiguously.[13] In addition, long LC measurement times, together with the
required sample derivatization steps, limit its throughput.High-resolution ion-mobility spectrometry (HR-IMS), on the other
hand, is capable of separating glycan isomers with the slightest structural
differences on the timescale of milliseconds.[14−17] Combined with fragmentation techniques
such as collision-induced dissociation (CID), IMSn approaches
have shown great promise for glycan isomer identification.[15,17−19] However, the unambiguous identification of glycans
based solely on the drift time or collisional cross section (CCS)
remains challenging. The measured drift times depend upon the experimental
conditions (pressure, temperature, voltages, etc.), which can be difficult
to control with high precision, especially in the case of the highest
resolution IMS techniques that use extended separation paths. The
high resolving power of such techniques introduces a new caveat to
data interpretation, especially when working with non-derivatized
glycans because it allows the separation of not only structural isomers
but also the α and β reducing-end anomers of each isomer
as well as different conformers.[15−17,20] In this case, a given isomer may present several peaks in its arrival-time
distribution (ATD). The situation becomes even more problematic when
analyzing unknown samples, where the presence of several isomeric
species is possible, and the corresponding analytical standards are
not necessarily available. Although an experimentally determined CCS
value can indicate the presence of a given isomer, there is no guarantee
that this value is unique. A CCS-based identification scheme for either
parent glycans or their fragments would thus require a database including
standards of all possible isomeric configurations of the molecule
in question, which is clearly not practical.Over the last few
years, several groups have reported the use of
infrared (IR) spectroscopy, either at room temperature[21−23] or at cryogenic temperatures,[16,18−20,24−29] for the analysis of glycan isomers. In contrast to identification
based on drift times or CCS values, an IR spectrum is an inherent
property of the analyte molecule, resulting in a vibrational fingerprint
unique to a given isomer. If the IR fingerprint of a compound has
been previously recorded and added to a database, this species can
be identified without the need for spectra of all possible isomeric
structures to exclude their presence. However, while an IR fingerprinting
approach requires isomerically pure analytical standards only once,
this still presents a problem because they are often expensive or
simply not available. Without a prior isomer separation step or an
isomer-specific detection scheme, in many cases it may be impossible
to measure isomerically pure IR fingerprint spectra.We have
recently combined cryogenic messenger-tagging IR spectroscopy
with HR-IMS isomer separation to produce highly resolved IR fingerprints
of isomeric glycan structures[16,24,25,27,30] and in some cases, we can acquire them in as little as 10 s. While
one can use this approach to identify glycans for which IR fingerprints
have been previously recorded, it cannot identify molecules for which
database entries do not exist. To address this issue, we have developed
a workflow that combines (IMS)n with cryogenic IR fingerprinting
and allows us to reconstruct the structure of unknown N-glycan positional isomers based on the mobility and IR fingerprints
of their CID fragments.[31] In addition to
providing a means to identify unknown glycan structures, it allows
us to extend our glycan IR fingerprint database with a minimal need
for analytical standards.In the present report, we build on
this work and present a procedure
for assigning all major drift peaks in the ATD of a selection of N-glycans obtained by ultrahigh-resolution IMS. Our method
is based on the identification of diagnostic fragments that allows
one to determine the precise isomeric form of the precursor molecule.
One molecule that is central to this approach is the disaccharide
GlcNAc-β(1–4)-GlcNAc, also called diacetyl-chitobiose,
which is present at the reducing end of all N-linked
glycans. Identification of the α and β anomers of diacetyl-chitobiose
allows us to assign certain peaks in the ATD of virtually all N-glycans to their respective reducing-end anomers. This,
in turn, allows us to distinguish anomers of a certain isomer from
other isomeric forms.
Experimental Section
Ion-Mobility-Selective
Cryogenic IR Spectroscopy
The
experiments described in this work were performed using a home-built
instrument described in detail elsewhere.[20] It combines high-resolution cyclic travelling-wave (TW) IMS using
structures for lossless ion manipulations (SLIM)[32−37] with cryogenic messenger-tagging IR spectroscopy. We have incorporated
a CID section within the IMS module to allow “on-board”
(IMS)n experiments.[18] Ions are
produced by a nano-electrospray source, transferred into vacuum via
a stainless-steel capillary, and guided toward the IMS module by a
dual funnel assembly (MassTech). Ions are collected in a 2 m accumulation
section of the SLIM IMS device prior to being introduced as packets
(i.e., pulses ∼100 μs–2 ms) into a 10 m serpentine
separation path. The TW potentials applied to the SLIM device propel
the ions through 2.2 mbar of N2 drift gas. We determine
the resolving power (R) as a function of the drift
length using the reverse-sequence peptides GRGDS and SDGRG (Figure b).[20] A single-cycle separation path (10 m) provides a resolution
of R ∼ 200, and this increases to ∼1000
after 20 cycles.[20] After separation, the
ions are guided through several differential pumping stages toward
a cryogenic ion trap maintained at a temperature of 45 K. A few milliseconds
prior to the arrival of an ion packet, a gas pulse (80:20 He/N2) is introduced into the trap to help confine and cool the
ions. During this process, weakly bound clusters are formed between
the analyte ions and N2, with the latter serving as a messenger
tag for spectroscopic interrogation.[38,39] A continuous,
mid-IR, fiber-pumped laser (CLT series, IPG, USA) operated at 1 W
power is used to irradiate the N2-tagged analyte ions for
the entirety of their trapping time (50 ms). At the end of each cycle,
trapped ions are released and transferred into a TOF mass spectrometer
(TofWerk). The absorption of a resonant photon by the weakly bound
clusters leads to the loss of the N2 tag, resulting in
a decrease in the tagged-ion signal and an increase in that of the
untagged ions. The IR spectrum of the analyte molecule is measured
by monitoring the tagging yield as a function of the laser wavenumber.
Figure 1
Symbols
for the monosaccharides comprising the glycans discussed
in this work.
Symbols
for the monosaccharides comprising the glycans discussed
in this work.
(IMS)n Experiments
Our SLIM IMS module includes
a trapping/CID section, which allows (IMS)n-type experiments.[18] Compared to our first design,[18] we have added a dual wire-grid assembly at the entrance
of the SLIM trap, increasing the fragmentation efficiency. After being
separated by their mobility along the 10 m serpentine path, parent
ions are introduced into the trapping region, which is held at a bias
voltage lower than that of the rest of the IMS device. As these ions
pass through the grid system at the trap entrance, they experience
a homogenous electric field of up to 3300 V/cm, which induces them
to undergo energetic collisions with N2, causing them to
dissociate. The resulting fragments are then released from the trap
and sent for additional separation cycles on the IMS device before
being directed to the cryogenic ion trap, hence allowing for the acquisition
of IR spectra of mobility separated fragments. We recently demonstrated
the use of this method to identify N-glycan positional
isomers.[31]
Identification of Drift
Peaks Corresponding to N-Glycan Isomers
Our approach for isomer identification and
database construction has been described in detail recently.[31] In brief, different glycan isomers are initially
separated according to their respective mobilities. Each separated
isomer is then subjected to CID, producing a range of fragments. Those
that are diagnostic for the structure of their precursor molecules
are subsequently mobility-separated and their IR fingerprints recorded.
Once the isomeric fragments are identified either by their relative
drift-peak position or by comparison to an IR fingerprint database,
it is possible to assign the structure of the parent molecules. Using
an initial database including IR fingerprints of diacetyl-chitobiose
isomers, we demonstrate the ability to distinguish drift peaks corresponding
to N-glycan α and β reducing-end anomers
from those of positional isomers or different gas-phase conformers.
Once the reducing-end anomers of a given N-glycan
are identified, their drift times and IR fingerprint spectra can in
turn be used to identify larger structures. Starting from a disaccharide,
we demonstrate how we can identify the reducing-end anomers of the N-glycan G2. Following this approach, we also show that
once the reducing-end anomers of a structure are identified, we can
determine the anomericity of all its Y fragments.
Materials
Man1, Man2, Man3, and Man5 glycans were purchased
from Dextra. G0-N, G0, G1, and G2 glycans were purchased from TheraProtein.
The diacetyl-chitobiose and tetraacetyl-chitotetraose samples were
purchased from Carbosynth. For nano-electrospray ionization (nESI),
5–20 μM solutions of the analytes were prepared in 50/50
MeOH/H2O. In-house prepared borosilicate glass nanospray
emitters were used to inject samples into the instrument. All molecules
were analyzed in their singly sodiated form. All gases were of 99.9999%
purity. Symbols for the monosaccharide components comprising these
glycans are given in Figure .
Results and Discussion
Identification of the α
and β Reducing-End Anomers
of Diacetyl-Chitobiose
Because the disaccharide diacetyl-chitobiose
is part of the common core found at the reducing end of all N-linked glycans, we use it as the starting point for the
identification of α and β anomers. To identify the reducing-end
anomers of this disaccharide, we used tetraacetyl-chitotetraose, a
tetrasaccharide composed of four β(1–4) linked GlcNAc
building blocks. A particularity of this molecule is that because
all monosaccharides composing it are β-linked, both Y2 and C2 fragments[40] can provide
information about the reducing-end configuration of the disaccharide
diacetyl-chitobiose. As shown schematically in Figure a, after mobility separation of the α
and β anomers of the parent tetrasaccharide, the Y2 and C2 fragments generated from the β anomer should
correspond to pure β-diacetyl-chitobiose, while the same fragments
of the α anomer will represent a mixture of both reducing-end
anomers of the disaccharide. This hypothesis is based on the previously
demonstrated anomeric retention of the glycosidic bond upon CID fragmentation.[19,23] An ATD of the precursor molecule tetraacetyl-chitotetraose is displayed
in Figure b and shows
two distinct mobility peaks, suggesting the presence of two reducing-end
anomers. Figure c
shows the ATDs (in red) of a mixture of Y2 and C2 fragments corresponding to diacetyl-chitobiose (m/z 447) produced upon CID of the first (bottom panel)
and second (top panel) drift peaks of the tetrasaccharide.
Figure 2
(a) Fragmentation
scheme for identifying diacetyl-chitobiose anomers.
(b) ATD of tetraacetyl-chitotetraose after one separation cycle in
the IMS device. (c) ATDs of the 447 m/z fragments (red traces) and the 449 m/z18O substituted fragments (dashed blue traces) after
four separation cycles obtained from peak one (bottom panel) and peak
two (top panel) of the tetrasaccharide.
(a) Fragmentation
scheme for identifying diacetyl-chitobiose anomers.
(b) ATD of tetraacetyl-chitotetraose after one separation cycle in
the IMS device. (c) ATDs of the 447 m/z fragments (red traces) and the 449 m/z18O substituted fragments (dashed blue traces) after
four separation cycles obtained from peak one (bottom panel) and peak
two (top panel) of the tetrasaccharide.We clearly observe an additional mobility peak at 482 ms in the
ATD of the fragments generated from the second mobility peak of the
tetrasaccharide that is not present in the ATD of the fragments generated
from the first parent mobility peak, where the main mobility feature
is centered around 488 ms. As described above, C2 and Y2 fragments should be equivalent in structure and hence yield
a single mobility feature if only the β anomer of the parent
tetrasaccharide was initially selected, while the C2 and
Y2 fragments will be of the opposite anomericity and may
result in two drift peaks when generated from the α anomer of
the parent. The mobility feature at 488 ms in Figure c can therefore be attributed to fragments
corresponding to diacetyl-chitobiose in the β configuration
and the feature at 482 ms to the α anomeric configuration. The
feature at 465 ms present in the fragment ATDs from both tetrasaccharide
species possibly corresponds to open-ring structures at the reducing
end, as proposed previously.[14]To
differentiate between the C2 and Y2 fragments,
we use 18O isotopically labeled tetrasaccharide. Because
the substitution exclusively occurs at the reducing end, it will appear
only in the Y fragments. The ATDs of isolated Y fragments should therefore
represent the arrival times of pure α or β reducing-end
anomers, depending on which anomer was selected for CID. These ATDs
are shown as blue dotted lines in Figure c, and indeed each displays a single peak
in the region of 480 to 500 ms, supporting our assignment of the two
drift peaks to the two reducing-end anomers of fragments corresponding
to diacetyl-chitobiose, with the α anomer being slightly more
mobile than the β anomer. This distinction in mobility will
later be used to assign anomers of larger species.Once identified,
the IR fingerprints of the α and β
anomers of diacetyl-chitobiose were recorded and stored in our database
(gray spectra in Figure b).
Figure 4
(a) ATD of G0-N(3) after
one IMS separation cycle. (b) IR spectral
comparison of CID fragments corresponding to diacetyl-chitobiose produced
from peak one (blue) and peak two (red) of G0-N(3), to previously
recorded database IR spectra of α (top panel, gray) and β
(bottom panel, gray) reducing-end anomers of diacetyl-chitobiose.
Identification of High-Mannose Glycan Drift Peaks Based on Fragment
Mobilities
We can use the information obtained on diacetyl-chitobiose
anomers to identify the drift peaks corresponding to the α and
β reducing-end anomers of high-mannose glycans. To do so, we
follow the same protocol as described earlier: we separate the molecules
of interest according to their mobility using IMS and then fragment
the separated isomers into diacetyl-chitobiose, for which the mobility
of the reducing-end anomers has been previously determined.Figure shows the
results obtained for different high-mannose N-glycans.
In each case, the left panels depict the ATDs of the parent molecules
after one IMS separation cycle, while the right panels show the ATDs
of the 447 m/z fragments generated
from the first (blue) and second (red) parent mobility feature after
three additional IMS separation cycles. In the present case, it is
possible to unambiguously assign α and β reducing-end
anomers based on the relative position of the fragment drift peaks
because diacetyl-chitobiose is the only one with m/z 447. The ATDs of the m/z 447 fragments shown in Figure resemble those of the diacetyl-chitobiose
species in Figure , where we assigned the earlier drift feature to the α anomer
and the later peak to the β anomer. We can thus assign the first
peak in the ATD of Man1 to the α reducing-end anomer and the
second peak to the β anomer. The reverse order was found for
both Man3 and Man5 where the first and second drift peaks correspond
to the β and α anomers, respectively.
Figure 3
(a) (left panel) ATD
of Man1 after one IMS separation cycle; (right
panel) ATDs of the diacetyl-chitobiose fragments produced by CID from
peak 1 (blue) and peak 2 (red) of Man1, after three IMS separation
cycles. (b) (left panel) ATD of Man3 after one IMS separation cycle
and (right panel) ATDs of the diacetyl-chitobiose fragments produced
from peak 1 (blue) and peak 2 (red) of Man3, after three IMS separation
cycles. (c) (left panel) ATD of Man5 after one IMS separation cycle
and (right panel) ATDs of the diacetyl-chitobiose fragments produced
from peak 1 (blue) and peak 2 (red) of Man5, after three IMS separation
cycles. The differences in the absolute drift time of diacetyl-chitobiose
obtained when fragmenting different molecules is due to different
conditions needed for the optimal separation of the parent ions.
(a) (left panel) ATD
of Man1 after one IMS separation cycle; (right
panel) ATDs of the diacetyl-chitobiose fragments produced by CID from
peak 1 (blue) and peak 2 (red) of Man1, after three IMS separation
cycles. (b) (left panel) ATD of Man3 after one IMS separation cycle
and (right panel) ATDs of the diacetyl-chitobiose fragments produced
from peak 1 (blue) and peak 2 (red) of Man3, after three IMS separation
cycles. (c) (left panel) ATD of Man5 after one IMS separation cycle
and (right panel) ATDs of the diacetyl-chitobiose fragments produced
from peak 1 (blue) and peak 2 (red) of Man5, after three IMS separation
cycles. The differences in the absolute drift time of diacetyl-chitobiose
obtained when fragmenting different molecules is due to different
conditions needed for the optimal separation of the parent ions.
Identification of G0-N(3) Drift Peaks Based
on Fragment IR Fingerprinting
In addition to using ATDs of
CID fragments to identify peaks in
the ATD of parent glycans, we can also use fragment IR fingerprints.
Using G0-N(3) (which has the non-reducing GlcNAc on the α-3
branch as in Figure a) as an example, we first separate isomers
of the parent molecules by their mobility.(a) ATD of G0-N(3) after
one IMS separation cycle. (b) IR spectral
comparison of CID fragments corresponding to diacetyl-chitobiose produced
from peak one (blue) and peak two (red) of G0-N(3), to previously
recorded database IR spectra of α (top panel, gray) and β
(bottom panel, gray) reducing-end anomers of diacetyl-chitobiose.The ATD of G0-N(3) after one separation cycle is
displayed in Figure a and exhibits two
drift peaks. Using CID, we produced m/z 447 fragments (corresponding to diacetyl-chitobiose) separately
for each mobility peak of G0-N(3) and recorded their corresponding
IR spectra. Figure b shows the comparison of these spectra with the previously recorded
IR fingerprints for the α and β diacetyl-chitobiose reducing-end
anomers (displayed in gray), which confirms that the fragments produced
from peak 1 of G0-N(3) correspond to β diacetyl-chitobiose,
while the one produced from peak 2 corresponds to α diacetyl-chitobiose.
It is worth noting that the main differences between the IR fingerprints
of the α and β diacetyl-chitobiose reducing-end isomers
lie within the structure of the absorptions at 3646 cm–1, as well as in the intensity of the absorption at 3463 cm–1. We can thus assign the first and second drift peaks of G0-N(3)
to its β and α reducing-end anomers, respectively.
Identification
of Hybrid N-Glycan Drift Peaks
by Fragment IR Fingerprinting
Using the information obtained
in the experiments described above, we can assign the drift peaks
of larger hybrid N-glycans. Here, we use glycan fragments
corresponding to G0-N(3) and Man3 to assign the drift peaks of the N-glycans G0 and G2, respectively. The ATD displayed in Figure a (left) shows two
major drift peaks after a single-cycle IMS separation, corresponding
to two isomers of G0. One of the main fragments observed for these
ions has an m/z of 1136. As displayed
in the middle panel of Figure a, several structures can give rise to this particular m/z, including G0-N(3), G0-N(6), and G0-core
N resulting from the loss of one GlcNAc at the reducing end. In this
case, we use IR spectroscopy to identify, which of these fragments
are produced. The spectra are shown in the right-hand panel of Figure a for fragments generated
from the first drift peak of G0 (blue) and for the second drift peak
(red). A comparison to previously recorded database IR fingerprints
of G0-N(3) reducing-end anomers (shown in gray) identifies fragments
from the first drift peak of G0 as the β anomer of G0-N(3) and
fragments from the second drift peak as the α anomer of the
same molecule. Because the reducing-end anomericity does not change
upon CID, we can thus assign the first drift peak of G0 to β
anomers and the second drift peak to its α anomer.
Figure 5
(a) (left panel)
ATD of G0 after one IMS separation cycle; (middle
panel) ATDs of G0-N(3) fragments produced from peak 1 (blue) and peak
2 (red) of G0 after one IMS separation cycle; and (right panel) IR
spectral comparison of G0-N(3) fragments produced from peak 1 (blue)
and peak 2 (red) of G0 to previously recorded database IR spectra
of α (gray, top) and β (gray, bottom) reducing-end anomers
of G0-N(3) and (b) (left panel) ATD of G2 after one IMS separation
cycle; (middle panel) ATDs of Man3 fragments produced from peak 1
(blue) and peak 2 (red) of G2 after 2 IMS separation cycles; (right
panel) IR spectral comparison of Man3 fragments produced from peak
1 (blue) and peak 2 (red) of G2, to previously recorded database IR
spectra of α (gray, top) and β (gray, bottom) reducing-end
anomers of Man3.
(a) (left panel)
ATD of G0 after one IMS separation cycle; (middle
panel) ATDs of G0-N(3) fragments produced from peak 1 (blue) and peak
2 (red) of G0 after one IMS separation cycle; and (right panel) IR
spectral comparison of G0-N(3) fragments produced from peak 1 (blue)
and peak 2 (red) of G0 to previously recorded database IR spectra
of α (gray, top) and β (gray, bottom) reducing-end anomers
of G0-N(3) and (b) (left panel) ATD of G2 after one IMS separation
cycle; (middle panel) ATDs of Man3 fragments produced from peak 1
(blue) and peak 2 (red) of G2 after 2 IMS separation cycles; (right
panel) IR spectral comparison of Man3 fragments produced from peak
1 (blue) and peak 2 (red) of G2, to previously recorded database IR
spectra of α (gray, top) and β (gray, bottom) reducing-end
anomers of Man3.Following the same protocol
and looking at Man3 fragments, we can
assign the first and second peaks of G2 to its β and α
reducing-end anomers, respectively. This example illustrates the utility
of IR fingerprinting, because to identify the fragments exclusively
on the basis of their drift times would require a database with ion-mobility
entries for all six possible fragments corresponding to m/z 933. In contrast, as shown in the right-hand
panel of Figure b,
the IR fingerprints of these fragments provide a positive match for
the Man3 reducing-end anomers, which allows the assignment of the
observed fragments to their corresponding structures without the need
for reference IR fingerprints of all possible alternatives.
Identification
of N-Glycan Fragment Isomers
The N-glycan drift peak identification method
presented above has been based on the assignment of drift peaks to
isomers of structurally diagnostic fragments. In a reverse application
of the presented workflow, it is also possible to obtain information
about the isomeric nature of other fragments once the drift peaks
observed for a given precursor molecule have been assigned to specific
isomers. To illustrate this approach, we chose the N-glycan G2 for which we have identified the reducing-end anomeric
configuration of the main drift peaks in the ATD of Figure b using Man3 as structurally
diagnostic fragments.Starting from the same ATD of G2, we can
generate fragments of m/z 1501 (corresponding
to the glycan G1) from each of the two identified drift peaks and
subject them to two additional separation cycles. The result, which
is displayed in Figure a, shows two distinct drift peaks for fragments corresponding to
G1 generated from either α (top panel) or β (bottom panel)
anomeric precursor ions. Following a similar fragment-based identification
protocol, we have recently demonstrated that the first two drift peaks
in the ATD of G1 (i.e., in the region of 375–390 ms) correspond
to the G1(6) positional isomer, in which the terminal galactose is
located on the upper branch, while the last two drift peaks (410–425
ms) correspond to the G1(3) positional isomers with the terminal galactose
on the lower branch.[31] Using this information,
we can assign every major drift peak in the ATD of G1 to the corresponding
isomer as well as their reducing-end anomeric configuration, as shown
in Figure b.
Figure 6
(a) (left panel)
ATD of G2 after one IMS separation cycle and (right
panel) ATDs of the G1 fragments produced from peak 1 (blue) and peak
2 (red) of G2 after two IMS separation cycles. (b) ATD of G1 after
two separation cycles with the assignment of α-3 and α-6
positional isomers and their respective reducing-end anomers.
(a) (left panel)
ATD of G2 after one IMS separation cycle and (right
panel) ATDs of the G1 fragments produced from peak 1 (blue) and peak
2 (red) of G2 after two IMS separation cycles. (b) ATD of G1 after
two separation cycles with the assignment of α-3 and α-6
positional isomers and their respective reducing-end anomers.If we go one step further and add IR fingerprint
spectroscopy to
the (IMS)n schemes described above, we can access and identify
isomers of fragments that are challenging to separate by their mobility.
To illustrate this, we used Man2(6) as an example. After up to 10
separation cycles in our IMS device (∼100 m drift path), it
was not possible to separate the Man2(6) reducing-end anomers. However,
using G0-N(3) as precursor ions for which reducing-end anomers can
be separated and identified, it is possible to obtain the α
and β reducing-end anomers of Man2(6) as fragments.After
mobility separation of G0-N(3) and identification of its
reducing-end anomers, as shown in Figure a, we selectively perform CID on the separated
drift peaks to obtain fragments corresponding to Man2(6) (m/z 771). These Man2(6) ions now have a
defined reducing-end anomericity, and we can obtain an IR fingerprint
for the α and β reducing end-anomers (Figure b). These, in turn, can serve
as structurally diagnostic fragments to identify positional isomers
and anomers of larger unknown structures. It is interesting to note
the similarity of the IR spectra of the α and β anomers
of Man2(6), with only slight differences occurring in the region 3630–3660
cm–1. This is consistent with the fact that these
anomers are difficult to separate by ion mobility.
Figure 7
(a) ATD of G0-N(3) after
one IMS separation cycle. (b) IR fingerprints
of Man2 fragments from G0-N(3) α reducing-end anomer (top spectrum,
red) and G0-N(3) β reducing-end anomer (bottom spectrum, blue).
(a) ATD of G0-N(3) after
one IMS separation cycle. (b) IR fingerprints
of Man2 fragments from G0-N(3) α reducing-end anomer (top spectrum,
red) and G0-N(3) β reducing-end anomer (bottom spectrum, blue).
Conclusions
The glycan sequencing
approach presented in this work highlights
the complementarity between HR-IMS and cryogenic IR spectroscopy.
Notably, IMSn offers richer information about the isomeric
nature of glycans and their fragments compared to MSn alone
and can be sufficient for identifying glycan structures in the cases
where the number of possible fragment isomers is limited, the IMS
resolving power is high enough to separate isomers, and a drift-time
calibration is accurate enough to discern a specific species. Nevertheless,
when working with complex structures, it is often the case that a
fragment mass-to-charge ratio corresponds to more than one isomer,
as shown in the examples in Figure . In this case, IMSn alone fails to provide
an unambiguous assignment of the glycan structure without: (a) a database
containing mobility information about all possible isomers of the
observed fragment; (b) the ability to separate them by mobility; and
(c) an accurate and reproducible determination of CCS values. The
latter is extremely challenging to obtain under ultrahigh-resolution
IMS conditions[41,42] and obtaining the required pure
analytical standards for all possible fragment isomers in question
is impractical. In contrast, using cryogenic IR spectroscopy, it is
possible to unambiguously assign a structure based on its unique IR
fingerprint alone without the need for drift-time calibration.The combination of IMSn with cryogenic IR spectroscopy
can thus be used to determine the identity of drift peaks separated
using HR-IMS, as well as to produce isomerically pure IR fingerprints
of glycans for which pure analytical standards are not available.
This approach, demonstrated here on N-glycans, can
be generalized to other classes of glycans that have common-core structures,
such as complex human milk oligosaccharides or O-linked glycans, as
well as other classes of biomolecules such as metabolites and lipids.
The work performed here suggests that the combination of IMSn with IR fingerprinting has the potential to have a major impact
in fields where the identification of the slightest structural differences
is crucial, such as drug development, disease biomarker research,
or forensics.
Authors: Michael Z Kamrath; Etienne Garand; Peter A Jordan; Christopher M Leavitt; Arron B Wolk; Michael J Van Stipdonk; Scott J Miller; Mark A Johnson Journal: J Am Chem Soc Date: 2011-03-30 Impact factor: 15.419
Authors: Ian K Webb; Sandilya V B Garimella; Randolph V Norheim; Erin S Baker; Yehia M Ibrahim; Richard D Smith Journal: J Am Soc Mass Spectrom Date: 2016-04-20 Impact factor: 3.109
Authors: Stephan Warnke; Ahmed Ben Faleh; Robert P Pellegrinelli; Natalia Yalovenko; Thomas R Rizzo Journal: Faraday Discuss Date: 2019-07-18 Impact factor: 4.008