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. Author manuscript; available in PMC: 2023 Jan 1.
Published in final edited form as: Methods Mol Biol. 2022;2437:3–19. doi: 10.1007/978-1-0716-2030-4_1

Gas-phase ion/ion reactions for lipid identification in biological tissue sections

Boone M Prentice 1,*
PMCID: PMC9148664  NIHMSID: NIHMS1807951  PMID: 34902137

Abstract

The unambiguous identification of isobaric (i.e., same nominal mass) and isomeric (i.e., same exact mass) lipids remains a challenging yet vital aspect of imaging mass spectrometry (IMS) workflows. This chapter presents a methodology for the preparation of biological tissue samples and the use of a hybrid mass spectrometer to perform gas-phase charge inversion ion/ion reactions for improved lipid identification. This gas-phase ion/ion reaction method provides lipid structural information beyond what can be obtained via conventional tandem mass spectrometry (MS/MS) experiments. While this procedure is described here for the identification of phosphatidylcholine (PC) analyte cations using 1,4-phenylenedipropionic acid reagent dianions, it can readily be generalized to perform a diverse array of ion/ion reaction chemistries.

Keywords: Lipid identification, gas-phase, ion/ion reactions, imaging mass spectrometry

1. Introduction

Imaging mass spectrometry (IMS) has emerged as a powerful technology for visualizing biochemical processes directly in tissue specimens by combining the molecular specificity of mass spectrometry with the spatial fidelity of a microscopic imaging approach. Despite the high molecular specificity of the mass spectrometer, the complex chemical milieu present in biological tissues sections results in the presence of many compounds of similar mass, at both nominal (i.e., isobaric) and exact (i.e., isomeric) m/z ratios.[1] The high level of structural homology of lipids and metabolites especially complicates the analysis of these compounds by mass spectrometry.[2,3] The failure to differentiate these compounds from one another in a mass spectrum results in the spatial distribution of a single peak no longer representing the spatial distribution of a single compound in an imaging mass spectrometry experiment, but instead representing the confluence of several compounds that have overlapping m/z values. Each unresolved ion could have a unique spatial distribution, so these types of spectral interferences result in inaccurate depictions of molecular distributions.

Chromatographic separations such as liquid chromatography (LC) and gas chromatography (GC) coupled to tandem mass spectrometry (MS/MS or MSn) are commonly employed to separate and identify components in a complex mixture. However, these technologies are often incompatible with the rapid spectral acquisition rates and direct surface sampling methods employed in imaging mass spectrometry.[46] Additionally, conventional tandem mass spectrometry ion dissociation techniques, such as collision induced dissociation (CID), are often insufficient to unambiguously identify biomolecules.[7] In the interest of broadening the range of ion dissociation chemistries accessible during tandem mass spectrometry experiments, we have developed gas-phase ion/ion reaction instrumentation and methods on a hybrid quadrupole-hexapole collision cell-Fourier transform ion cyclotron resonance (QhFTICR) mass spectrometer (Figure 1).[8] This approach decouples the ionization method from the nature of the ion to be interrogated and enables the ion type to be derivatized to any desirable form. This is achieved in the gas-phase following the ionization event, allowing subsequent MS/MS experiments to provide structural information independent of the initial ion type generated from the tissue surface. These gas-phase reactions offer a number of benefits that make them ideally suited for use in imaging mass spectrometry experiments, including their rapid reaction rates (i.e., reaction times of less than one second are common) and the ability to readily compare un-derivatized and derivatized sample types, since the initial sample is never altered.[9,10] Unlike analogous condensed-phase tissue derivatization procedures, which can lead to complex mixtures due to side reactions and incomplete reactions, a gas-phase approach eliminates physical manipulation of the tissue. This minimizes the possibility of tissue deformation and analyte delocalization that can occur during sample preparation protocols.[11]

Figure 1:

Figure 1:

(a) Instrument timing diagram showing reagent and analyte ion injection (50 and 500 ms, respectively), ion/ion reaction (1.5 s), product ion isolation and SORI CID (~10 ms), and mass analysis (~0.75 s) in the ICR cell. The entire ionization and reaction process takes ~2 to 3 s. (b) A simplified instrument diagram depicts the ion/ion reaction operation on the solariX instrument platform. This chemistry is enabled by sequentially injecting ESI-generated anions followed by MALDI-generated cations through a mass resolving quadrupole into a hexapole ion trap. Following a defined mutual storage reaction period, the product ions are transferred to the ICR for isolation, SORI CID, and mass analysis. The transfer optics from the hexapole ion trap to the ICR cell and the ICR electrodes have been omitted from the instrument diagram for simplicity. Note that the timing and instrument diagrams are not drawn to scale. Reprinted with permission Specker JT, Orden SLV, Ridgeway ME, Prentice BM (2020) Identification of phosphatidylcholine isomers in imaging mass spectrometry using gas-phase charge inversion ion/ion reactions. Anal Chem 92:13192–13201.[8] Copyright 2020 American Chemical Society.

Herein, we present (1) a sample preparation workflow to perform positive ion mode lipid imaging mass spectrometry on biological tissue sections, (2) instrumental methodology for performing charge inversion ion/ion reactions to determine the fatty acyl chain identities of phosphatidylcholine (PC) ions sampled directly from biological tissues, and (3) an experimental design to determine the relative levels of sn-positional isomers detected in tissue. While this method has been developed for the reaction of PC analyte cations with 1,4-phenylenedipropionic acid (PDPA) reagent dianions, the procedure can be adapted for alternative reaction chemistries using any desired analyte and reagent. This reaction is termed a “charge inversion” experiment because it involves the reaction of singly charged lipid cations produced via MALDI with doubly charged reagent anions produced via electrospray ionization (ESI) to produce singly charged, charge-inverted analyte anions:[12,13]

[PC+H]++[PDPA2H]2[PC+PDPAH] (1)

This product ion readily dissociates to give a de-methylated PC anion:

[PC+PDPAH][PCCH3]+PDPACH3(neutralloss) (2)

which can be subjected to sustained off resonance irradiation (SORI) CID to produce fragment ions that are diagnostic for the fatty acid tail identities and positions:

[PCCH3][R1CH2COOH]+[R2CH2COOH] (3)

The following protocol describes the experimental design and workflow for performing lipid identification directly from tissue using ion/ion reactions. A more detailed description of the instrumentation hardware can be found in a recent research article.[8]

2. Materials

2.1. Tissue Cryosectioning

  1. Cryomicrotome and accessories (cryomicrotome blade, sample specimen disk, anti-roll plate)

  2. Tissue samples

  3. Optimal cutting temperature (OCT) polymer compound

  4. Sample handling tools (forceps and small artist’s paint brushes)

  5. Teflon-coated glass slide

  6. Sample substrate (indium tin oxide-coated glass slides or common glass microscope slides)

  7. Microscope slide box

  8. Styrofoam cooler with dry ice

  9. Ethanol

  10. Kimwipes

  11. Desiccator

2.2. Matrix Application by Sublimation

  1. Sublimation assembly (consisting of a rotary vane mechanical pump, valves, tubing, a vacuum trap, a vacuum measurement gauge, glass sublimation apparatus with a flat bottom, a hot plate, a baking dish, sand, a thermometer, and support stands and clamps for stabilization during operation)

  2. 1,5-diaminonapthalene (DAN) (or other appropriate MALDI matrix)

  3. Thermally conductive adhesive tape

  4. Ice

  5. Timer

  6. Reagent grade ethanol

  7. Kimwipes

2.3. Solution Preparation

  1. 1,4-phenylenedipropionic acid (PDPA) reagent (1 mg/mL in 49.5/49.5/1 water/acetonitrile/ammonium hydroxide by volume)

  2. 1,5-diaminonapthalene (DAN) MALDI matrix (20 mg/mL in 70/30/0.1 acetonitrile/water/trifuloroacetic acid by volume)

  3. Synthetic standards of lipid isomers (10 mM in methanol)

  4. HPLC-grade water

  5. HPLC-grade acetonitrile

  6. Trifluoroacetic acid

  7. Ammonium hydroxide

  8. Hematoxylin and eosin solutions (H&E)

2.4. Instrumentation and Software

  1. 7T solariX XR FT-ICR mass spectrometer equipped with an Apollo II dual MALDI/ESI source and ETD (Bruker Daltonics, Billerica, MA, USA)

  2. flexImaging 5.0 (Bruker Daltonics, Billerica, MA, USA)

  3. DataAnalysis (Bruker Daltonics, Billerica, MA, USA)

  4. Microsoft Excel or equivalent

  5. MTP Slide Adapter

  6. MTP AnchorChip MALDI

  7. Flatbed scanner

  8. Optical microscope (Zeiss Axioscan Z1 brightfield slide scanner [Carl Zeiss Microscopy LLC, White Plains, NY, USA] or equivalent)

3. Methods

3.1. Tissue sectioning

Sample preparation is a critical aspect of any imaging mass spectrometry workflow. The quality of the resulting ion images depends on many steps, including tissue procurement and storage, tissue sectioning, and matrix application. Ensure that proper personal protective equipment is used (e.g., lab coat, lab goggles/glasses, gloves, cryostat sleeves).

  1. Transport the tissues from cold storage to the cryochamber using a Styrofoam cooler filled with dry ice and allow roughly 15 minutes for the tissue to thermally equilibrate (see Note 1).

  2. Mount the tissue to the specimen disk using a dime-sized area of OCT (use more or less OCT as required for larger or smaller tissues, respectively) (see Note 2).

  3. Install the cryomicrotome blade, rinsing with ethanol and water prior to installation to remove any residual cartridge oil.

  4. Trim the tissue to the desired organ depth, ensuring a flat and even cutting plane. Once the desired depth is reached, set the sectioning thickness (typically 8–20 μm).

  5. Section the tissue at the desired thickness. Use artist’s paintbrushes to gently position the tissue onto the Teflon-coated slide. (see Note 3). Compress the MALDI microscope slide on top of the tissue as the tissue is resting on the Teflon-coated slide (see Note 4). The tissue will adhere to the MALDI slide when the slide is removed, after which it can be thaw-mounted (see Note 5 and Note 6). Place at least two serial sections on each slide via this process.

  6. Store the samples in a −80°C freezer until use. Warm the samples in a desiccator for 30 minutes prior to matrix application to prevent condensation buildup on the tissue surface.

  7. Clean the cryomicrotome with ethanol or other appropriate disinfectant after use, taking care to properly handle and dispose of sharps and biohazardous materials.

3.2. Matrix application

MALDI matrix selection is guided by several experimental parameters, including the analytes of interest, instrument ion polarity, and application method.[1417] A standard matrix application method is described here using a custom-built sublimation apparatus for subsequent positive ion mode lipid imaging mass spectrometry.[18] A more reproducible matrix application procedure can be achieved using a robotic spraying system. Ensure that proper personal protective equipment is used (e.g., lab coat, lab goggles/glasses, gloves) and that matrix application is performed in a chemical fume hood.

  1. Prepare the sublimation assembly by turning on the vacuum pump, closing all valves, and adding crushed dry ice and ethanol to the bottom of the dewar containing the cold trap. Adjust the sand bath temperature to the desired temperature (see Note 7).

  2. Prepare the matrix by adding ~200 mg of DAN matrix to the condenser sleeve, enough to evenly coat the bottom of the device.[19]

  3. Prepare the microscope slide by mounting it onto the bottom of the condenser using conductive adhesive tape to ensure thermal equilibration during the sublimation process. The side with the tissue section should be inverted and facing downward over the matrix on the bottom of the chamber when the condenser is placed in the sleeve. Evacuate the chamber by opening the valve to the pump (see Note 8).

  4. Once the chamber has reached adequate vacuum, add an ice water slurry to the condenser sleeve. Lower the assembled apparatus onto the heated sand, ensuring that the bottom of the condenser is level and evenly submerged in the heated sand (see Note 9).

  5. After the desired amount of matrix has been added, remove the assembled apparatus from the heated sand (see Note 10). Empty the slurry and allow the apparatus to equilibrate to room temperature before releasing the vacuum and removing the sample. Clean the apparatus using ethanol.

3.3. Lipid Imaging Mass Spectrometry

  1. Prepare the matrix-coated tissue sample slide for imaging by first drawing fiducial markers using a silver metallic pen for the background and a fine pointed black Sharpie to create crosshairs at four corners bracketing the sample. Place the slide in an MTP Slide Adapter and record an image of the marked plate using a flatbed scanner.

  2. Introduce the MTP Slide Adapter containing the sample into the mass spectrometer. Optimize and save an ftmsControl acquisition method for positive ion mode PC analysis by tuning MALDI laser parameters, ion optic settings, and ICR cell analysis conditions (see Note 11). Ensure that the method is m/z calibrated. Matrix peaks, known endogenous compounds, and/or external standards are commonly used for m/z calibration.

  3. Set up an image acquisition method using flexImaging. This process includes first “teaching” the fiducial marks from the instrument’s optical camera in ftmsControl to the scanned sample image uploaded to flexImaging. Then select the appropriate ftmsControl acquisition method, select the desired step size (i.e., spatial resolution), and specify the areas to be imaged using the polygon region measurement tool.

  4. Acquire the image and view the results using flexImaging. Ions of interest can then be selected for identification using procedures outlined below.

3.4. Ion/Ion Reactions using Lipids Generated from Tissue

PC cations are tentatively identified using sum-composition nomenclature (expressed as total carbon:double bond [TC:DB]) via high resolution accurate mass (HRAM) measurements (see Note 12).[2023] However, identification of the fatty acyl tails present in the PC requires tandem mass spectrometry[24] and can be performed using the gas-phase ion/ion reactions discussed below (see Note 13).

  1. PC cations of interest from the acquired ion image are chosen for identification via gas-phase charge inversion ion/ion reactions (Figure 2a). MALDI-generated PC cations will be generated from regions of interest in the serial tissue section (Figure 2b). The “position sample carrier” function in flexImaging can be used to accurately position the MALDI laser in ftmsControl.

  2. Load the PDPA reagent sample solution into the ESI syringe and ensure reagent ion detection in negative ion mode (see Note 14).

  3. The ion/ion reaction between the MALDI-generated PC cations and ESI-generated PDPA dianions is optimized by tuning various instrument ion optics (see Note 15). Ion/ion reactions can be integrated on solariX MS systems equipped with electron transfer dissociation (ETD)[25] by modifying the pulse program and ETD-binding rules, as described in our recent manuscript (see Note 16).[8] Other gas-phase ion/ion reactions can be explored for different purposes and different reactants using this same instrumentation (see Note 17).

  4. After optimization of the ion/ion reaction, a de-methylated PC product anion should be detected (Figure 2c) (see Note 18).

  5. The desired de-methylated PC product anion is then isolated in the ICR cell (see Note 19) and subjected to SORI CID (Figure 2d) (see Note 20).

  6. Following optimization of SORI CID conditions to observe the sn-1 and sn-2 fatty acid fragment anions, replicate measurements (n=10 is common) should be made in desired regions of the tissue. These fragment ions allow for the identification of the fatty acyl groups in the original PC (see Note 21). In order to determine the sn-positions of the fatty acyl chains, comparison with synthetic lipid standards is necessary, as outlined below.

  7. After measurements are completed, tissues can be stained using hematoxylin and eosin (H&E) and scanned using an optical microscope to validate morphological features in the tissue (Figure 2a).[26]

Figure 2:

Figure 2:

(a) Ion image for m/z 760.585 in the rat brain, tentatively identified as PC34:1 by an accurate mass measurement. A PDPA charge inversion ion/ion reaction of (b) PC34:1 generated directly from the tissue surface (c) produces a PC/PDPA anionic complex and a demethylated PC anion. (d) Ion isolation of the demethylated PC anion followed by SORI CID produces fragment ions diagnostic for the 16:0 and 18:1 fatty acid tails in the lipid, allowing for the identification as PC16:0_18:1. Note that circles indicate positive ion mode analysis, squares indicate negative ion mode analysis, number signs denote fragment ions related to PDPA, asterisks denote harmonics/electronic noise, and the lightning bolt is used to denote the ion subjected to CID. All spectra are single scan measurements. Reprinted with permission Specker JT, Orden SLV, Ridgeway ME, Prentice BM (2020) Identification of phosphatidylcholine isomers in imaging mass spectrometry using gas-phase charge inversion ion/ion reactions. Anal Chem 92:13192–13201.[8] Copyright 2020 American Chemical Society.

3.5. Ion/Ion Reactions using Lipid Standards

The sn-positions of fatty acid tails in a glycerophospholipid can typically be determined when performing CID on a deprotonated ion type by examining the relative intensities of the fatty acid fragment anions.[24] However, this is only true when the precursor glycerophospholipid is isomerically pure (see Note 22). PCs measured in the complex chemical environment of biological tissue samples are likely a mixture of sn-positional isomers.[2729] Thus, a comparison with synthetic lipid standards is necessary to accurately determine the relative contribution of each isomer (see Note 23).

  1. Prepare 10 mM solutions of lipid standards for each isomer in the identified lipid. Prepare samples for a calibration curve containing varying concentrations of each isomer using defined mixtures of the lipid standards (see Note 24). For example, manually-spotted mixtures of PC16:0/18:1 and PC18:1/16:0 standards containing varying fractional amounts of each isomer are prepared for PC34:1.

  2. Mix the lipid standard solutions 1:1 (v/v) with aliquots of the DAN MALDI matrix solution. Use the dried-droplet method to deposit one microliter aliquots of this mixture onto an MTP AnchorChip MALDI target.

  3. The same ion/ion reaction and SORI CID method employed for on-tissue measurements should be used to interrogate the manually-spotted calibration curve samples. Replicate measurements (n=10) of each calibration point should be made. Data is then visualized in DataAnalysis.

  4. The intensity of the 18:1 fatty acid fragment ion relative to the summed intensities of both the 16:0 and 18:1 fatty acid fragment ions will have a linear relationship with lipid isomer content (Figure 3a). This calibration curve can be constructed in Excel and then used to determine the relative fraction of each PC16:0_18:1 isomer in different regions of the tissue (Figure 3b and 3c) (see Note 25).

Figure 3:

Figure 3:

(a) Mixtures of PC16:0/18:1 and PC18:1/16:0 lipid standards are used to calibrate the 18:1/(18:1 + 16:0) fragment ion intensity ratio obtained via CID of the [PC34:1 − CH3] anion produced via the PC/PDPA charge inversion reaction. (b) The ion/ion reaction method reveals that the relative isomeric content of PC34:1 varies throughout rat brain. Each measurement in the standard curve and each region of the brain is the average of 10 spectra. (c) H&E-stained tissue showing regions of interest. Reprinted with permission Specker JT, Orden SLV, Ridgeway ME, Prentice BM (2020) Identification of phosphatidylcholine isomers in imaging mass spectrometry using gas-phase charge inversion ion/ion reactions. Anal Chem 92:13192–13201.[8] Copyright 2020 American Chemical Society.

Footnotes

4. Notes

1.

Specimens stored in a −80°C freezer need time to warm up to roughly −25°C for optimal sectioning (this time will vary depending on the size and type of sample). While the sample tissue is warming, place other sectioning supplies (e.g., glass slides, paintbrushes, Teflon-coated slide, etc.) in the cryomicrotome chamber to cool. Tissues with higher fat content will require lower temperatures for adequate freezing and optimal sectioning.

2.

Take care not to pour OCT on the bulk of the tissue that is to be sectioned, as it can cause ionization suppression in MALDI mass spectrometry. Avoid direct manual handling of the tissue so as not to thaw the organ. Instead, use forceps to manipulate the specimen.

3.

Cryosectioning is a technique that requires patience and practice. If the tissue section adheres to the blade or anti-roll plate, use the artist’s paintbrushes to tease the tissue section free. If the tissue section strongly adheres to chamber surfaces, there may be excessive static electricity in the chamber or a mismatch between the object and chamber temperatures. An anti-static gun can be used to discharge a build-up of static electricity in the chamber. Ensure that the chamber temperature is colder than the object temperature to avoid a temperature mismatch. Small local adjustments in temperature (e.g., to the anti-roll plate) can be made using a small piece of dry ice (to slightly cool a surface) or a finger (to slightly warm a surface).

4.

Ensure that there are no folds in the tissue prior to mounting. If there is a slight curl to the tissue, face the curl downwards onto the Teflon-coated slide so that it is flattened as the tissue section is picked up with the MALDI microscope slide.

5.

If using a conductive slide, ensure that the tissue section is mounted on the conductive side (only one side of the slide is usually conductive). This can be verified by measuring the surface resistance of each side using a multimeter. The conductive side can be marked by etching a number in the corner of the slide using a diamond scribe. Serial slides can be consecutively numbered to keep track of the slide order. Numerical etches should be placed in the same corner of each slide and written so that the conductive surface can be easily identified. This is best done prior to placing the slides in the cryomicrotome.

6.

Place the backside of the MALDI microscope slide containing the tissue section onto your palm to accelerate thaw-mounting. Ensure that all water content has been evaporated during the thaw-mounting process, as remaining water can refreeze in the tissue and affect downstream analysis. Complete drying requires 15–60 seconds of thaw-mounting and will be evident when the tissue turns from a darker color to a more neutral matte color.

7.

At 50 mTorr, DAN, 2,5-dihydroxyacetophenone (DHA), and 2,5-dihydroxybenzoic acid (DHB) sublimate well at 110°C, sinapic acid sublimates well at 150°C, α-Cyano-4-hydroxycinnamic acid (CHCA) sublimates well at 170°C, and 9-aminoacridine (9AA) sublimates well at 180°C. Shake the sand bath to disperse sand evenly, allowing for uniform heating of the sand. After the temperature is set on the hot plate, it will typically take ~15–30 minutes to reach a stable temperature. The surface of the sand will typically be roughly 50°C cooler than the surface setting of the hot plate and should be measured using a digital probe thermometer placed to the same depth in the sand bath as the condenser bottom discussed in later steps.

8.

The vacuum gauge should quickly drop below 100 mTorr. If the pressure does not reach adequate pressure, ensure that the rubber O-ring is properly seated between the condenser sleeve and bottom. As the valve to the vacuum pump is opened, monitor the matrix coating on the bottom of the chamber. If the matrix particles are significantly disrupted as the valve is opened, there is likely a leak around the O-ring that is admitting air into the chamber. Leaks around the O-ring can also sometimes be audibly perceived as a high-pitched whistling.

9.

Be consistent with the submersion depth to ensure reproducible matrix applications.

10.

The application time will vary depending on the matrix (DHA will take ~3.5 minutes, DAN will take ~6 minutes, and CHCA, SA, and 9AA will take ~10–15 minutes). Weighing the MALDI microscope slide before and after matrix application allows for an accurate measure of added matrix. Typical optimal matrix coatings will weigh 1–3 mg. Sufficient matrix application can be monitored during the sublimation process by observation of a visible vapor layer roughly 0.5 cm above the bottom edge of the condenser tube.

11.

ftmsControl has a built-in Help manual that details the function of many of the instrument parameters as well as suggested optimal ranges.

12.

PC34:1 is an example of TC:DB nomenclature, where 34 is the total number of carbon atoms in the fatty acyl chains and 1 is the total number of double bonds in the fatty acyl chains. HRAM identifications with better than 5 ppm mass accuracies are considered reliable and readily achieved with an accurately calibrated dataset. Tentative lipid identifications using accurate mass measurements can be made by searching any of several lipid and metabolite databases.[30] However, care should be taken not to over-report the confidence of the identification. For example, m/z 760.585 can be tentatively identified as PC34:1, but should not be reported as any of PC16:0/18:1, PC16:1/18:0, PC(18:0/16:1), or PC18:1/16:0 based on intact mass alone.

13.

While protonated PC ions are readily abundant in positive ion mode MALDI imaging mass spectrometry, CID of these ion types typically results exclusively in fragmentation of the choline head group and gives no information about the fatty acyl chains.[24] While negative ion mode CID results in fragment ions indicative of the fatty acid identities and positions present in the lipid, negative ion mode MALDI imaging mass spectrometry rarely produces PC anions, instead giving ion signals from more acidic glycerophospholipids (e.g., phosphatidylethanolamines).[21]

14.

Stable ESI signal is key to ensuring facile ion/ion reaction tuning and is best obtained by optimizing the source gas parameters. A roughly 10-fold excess of reagent ion signal compared to analyte ion signal is desirable to operate under conditions of pseudo-first order kinetics.[31]

15.

The analyte and reagent precursor ions should each be isolated using the quadrupole mass filter as they are sequentially injected into the hexapole ion trap (Figure 2b). The hexapole ion trap RF potential and mirror RF potential are key to optimizing the reaction. These parameters define the pseudopotential well depth in the reaction cell.[32,33] If the RF potential is too high, the lower mass PDPA reactant dianions may be ejected due to a low mass cut-off (LMCO) effect. If the RF potential is too low, the higher mass product complex ions may be insufficiently confined in the ion trap.[34] The collision cell DC offset and lens potentials are also important ion/ion reaction parameters to optimize. These parameters facilitate trapping of the two ion populations. It is common to toggle back and forth between MALDI-only, ESI-only, and ion/ion reaction modes to confirm sufficient ion signal of both reactants as the reaction parameters are being optimized.

16.

The modifications to the pulse programming and ETD-binding rules have enabled user-defined parameters to be entered directly in ftmsControl.[8] However, the polarity of the ESI source had to be manually defined using the SHEDS Command Interface. This was defined by programming the polarity command (“P_HV”) of the ESI module (“ESI_”) in NICE as negative (“1”) using the “SetValue” feature. “GetSetValue” was used to confirm proper programming of the parameter.

17.

Optimal ion/ion overlap for efficient reactions is best obtained when the reagent and analyte reactant ions are similar in m/z value.[35] At least one reactant should be multiply charged to avoid neutralization, and the reaction rate scales with the square of the ion charges.[36] Typical reagent ion injection and reaction times are 50–500 ms and 500–1500 ms, respectively.

18.

The intact [PC + PDPA − H] product ion complex spontaneously decomposes to the de-methylated [PC − CH3] product ion via neutral loss of methylated PDPA. The energy to drive this spontaneous loss may originate from the coulombic recombination energy of the ion/ion reaction, the reaction conditions in the hexapole ion trap, and/or from the ion transfer conditions from the hexapole ion trap to the ICR cell.[37] It is also important to note that single proton transfer from the PC cation to the PDPA dianion is an undesired reaction pathway that competes with charge inversion and results in neutralization of the PC and a charge reduced [PDPA − H] product anion.

19.

The ion subjected to SORI CID should have a signal intensity of at least 1–5×106 in order to detect resulting fragment ion signals above the level of instrumental noise. Ion intensities of 107 will provide SORI CID fragment ion intensities of roughly 106, which are necessary to achieve satisfactory ion statistics for reliable downstream analysis.

20.

Care should be taken to allow the pressure in the ICR cell to return below roughly 1×10−9 mbarr between successive SORI CID experiments. This reduces the load on the vacuum system and avoids tripping an over-pressure interlock.

21.

For example, m/z 760.585, tentatively identified as PC34:1, was found to contain the fatty acyl chains equating to PC16:0_18:1 in rat brain tissue, where the underscore is used to denote ambiguity of the sn-position of the two fatty acyl groups.

22.

The sn-positions of the fatty acyl groups in glycerophospholipid anions subjected to CID can typically be determined by examining the relative intensities of the fragment ions. Under low energy CID conditions, cleavage at the lipid sn-2 position is favored.[24] As a result, fatty acid fragment ions arising from the sn-2 position will generally be more abundant than those arising from the sn-1 position. However, PCs measured in the complex chemical environment of biological tissue samples are likely a mixture of sn-positional isomers, so this ratio will contain fragment ion populations from mixtures of precursor ions and will no longer be an accurate reflection of sn-position.

23.

The procedure described herein allows for the differentiation of PC sn-positional isomers. However, additional structural isomers likely exist when accounting for the positions and orientations of the double bonds in the fatty acid tails (e.g., 6Z or 9Z). Alternative ion/ion reactions or other gas-phase approaches can be employed to identify these lipid structures.[28,38,39,29]

24.

Determining the relative contributions of all isomers in a mixture using this method currently requires the generation of calibration curves containing each lipid isomer. This is dependent on the availability, affordability, and purity of synthetic lipid standards and may not be feasible for all experiments.

25.

Relative standard deviations of on-tissue ratio measurements are typically <5%. The isomeric ratio can vary by at least 25% between different locations (i.e., substructures) in the tissue. Errors in this approach could be due to isomeric contamination in the synthetic lipid standards, which ranges from 95%−99% purity.

5. References

  • 1.Liebisch G, Ejsing CS, Ekroos K (2015) Identification and annotation of lipid species in metabolomics studies need improvement. Clin Chem 61 (12):1542–1544. doi: 10.1373/clinchem.2015.244830 [DOI] [PubMed] [Google Scholar]
  • 2.Fahy E, Subramaniam S, Brown HA, Glass CK, Merrill AH Jr., Murphy RC, Raetz CR, Russell DW, Seyama Y, Shaw W, Shimizu T, Spener F, van Meer G, VanNieuwenhze MS, White SH, Witztum JL, Dennis EA (2005) A comprehensive classification system for lipids. J Lipid Res 46 (5):839–861. doi: 10.1194/jlr.E400004-JLR200 [DOI] [PubMed] [Google Scholar]
  • 3.Pauling JK, Hermansson M, Hartler J, Christiansen K, Gallego SF, Peng B, Ahrends R, Ejsing CS (2017) Proposal for a common nomenclature for fragment ions in mass spectra of lipids. PLoS One 12 (11):e0188394. doi: 10.1371/journal.pone.0188394 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 4.Kertesz V, Van Berkel GJ (2010) Liquid Microjunction Surface Sampling Coupled with High-Pressure Liquid Chromatography–Electrospray Ionization-Mass Spectrometry for Analysis of Drugs and Metabolites in Whole-Body Thin Tissue Sections. Anal Chem 82 (14):5917–5921. doi: 10.1021/ac100954p [DOI] [PubMed] [Google Scholar]
  • 5.Van Berkel GJ, Kertesz V (2013) Continuous-flow liquid microjunction surface sampling probe connected on-line with high-performance liquid chromatography/mass spectrometry for spatially resolved analysis of small molecules and proteins. Rapid Commun Mass Spectrom 27 (12):1329–1334. doi: 10.1002/rcm.6580 [DOI] [PubMed] [Google Scholar]
  • 6.Prentice BM, Caprioli RM (2016) The need for speed in matrix-assisted laser desorption/ionization imaging mass spectrometry. Journal of Postdoctoral Research 4 (3):3–13 [PMC free article] [PubMed] [Google Scholar]
  • 7.McLuckey SA, Mentinova M (2011) Ion/neutral, ion/electron, ion/photon, and ion/ion interactions in tandem mass spectrometry: do we need them all? Are they enough? J Am Soc Mass Spectrom 22 (1):3–12. doi: 10.1007/s13361-010-0004-9 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 8.Specker JT, Orden SLV, Ridgeway ME, Prentice BM (2020) Identification of phosphatidylcholine isomers in imaging mass spectrometry using gas-phase charge inversion ion/ion reactions. Anal Chem 92:13192–13201 [DOI] [PubMed] [Google Scholar]
  • 9.Prentice BM, McLuckey SA (2013) Gas-phase ion/ion reactions of peptides and proteins: acid/base, redox, and covalent chemistries. Chem Commun 49 (10):947–965. doi: 10.1039/c2cc36577d [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 10.Foreman DJ, McLuckey SA (2020) Recent developments in gas-phase ion/ion reactions for analytical mass spectrometry. Anal Chem 92 (1):252–266. doi: 10.1021/acs.analchem.9b05014 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 11.Bonney JR, Prentice BM (2021) Perspective on emerging mass spectrometry technologies for comprehensive lipid structural elucidation. Anal Chem. doi: 10.1021/acs.analchem.1c00061 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 12.Stutzman JR, Blanksby SJ, McLuckey SA (2013) Gas-Phase Transformation of Phosphatidylcholine Cations to Structurally Informative Anions via Ion/Ion Chemistry. Anal Chem 85 (7):3752–3757. doi: 10.1021/ac400190k [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 13.Rojas-Betancourt S, Stutzman JR, Londry FA, Blanksby SJ, McLuckey SA (2015) Gas-Phase Chemical Separation of Phosphatidylcholine and Phosphatidylethanolamine Cations via Charge Inversion Ion/Ion Chemistry. Anal Chem 87 (22):11255–11262. doi: 10.1021/acs.analchem.5b02243 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 14.Schwartz SA, Reyzer ML, Caprioli RM (2003) Direct tissue analysis using matrix-assisted laser desorption/ionization mass spectrometry: practical aspects of sample preparation. J Mass Spectrom 38 (7):699–708. doi: 10.1002/jms.505 [DOI] [PubMed] [Google Scholar]
  • 15.Kaletaş B, van der Wiel I, Stauber J, Lennard JD, Güzel C, Kros J, Luider T, Heeren R (2009) Sample preparation issues for tissue imaging by imaging MS. Proteomics 9 (10):2622–2633. doi: 10.1002/pmic.200800364 [DOI] [PubMed] [Google Scholar]
  • 16.Norris JL, Caprioli RM (2013) Analysis of tissue specimens by matrix-assisted laser desorption/ionization imaging mass spectrometry in biological and clinical research. Chem Rev 113 (4):2309–2342. doi: 10.1021/cr3004295 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 17.Perry WJ, Patterson NH, Prentice BM, Neumann EK, Caprioli RM, Spraggins JM (2020) Uncovering matrix effects on lipid analyses in MALDI imaging mass spectrometry experiments. J Mass Spectrom 55 (4):e4491. doi: 10.1002/jms.4491 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 18.Hankin JA, Barkley RM, Murphy RC (2007) Sublimation as a method of matrix application for mass spectrometric imaging. J Am Soc Mass Spectrom 18 (9):1646–1652. doi: 10.1016/j.jasms.2007.06.010 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 19.Thomas A, Charbonneau J, Fournaise E, Chaurand P (2012) Sublimation of new matrix candidates for high spatial resolution imaging mass spectrometry of lipids: enhanced information in both positive and negative polarities after 1,5-diaminonapthalene deposition. Anal Chem 84 (4):2048–2054. doi: 10.1021/ac2033547 [DOI] [PubMed] [Google Scholar]
  • 20.Cornett DS, Frappier SL, Caprioli RM (2008) MALDI-FTICR imaging mass spectrometry of drugs and metabolites in tissue. Anal Chem 80 (14):5648–5653. doi: 10.1021/ac800617s [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 21.Zemski Berry KA, Hankin JA, Barkley RA, Spraggins JM, Caprioli RM, Murphy RC (2011) MALDI imaging of lipid biochemistry in tissues by mass spectrometry. Chem Rev 111 (10):6491–6512 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 22.Liebisch G, Vizcaíno JA, Köfeler H, Trötzmüller M, Griffiths WJ, Schmitz G, Spener F, Wakelam MJ (2013) Shorthand notation for lipid structures derived from mass spectrometry. J Lipid Res 54 (6):1523–1530. doi: 10.1194/jlr.M033506 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 23.Bowman AP, Blakney GT, Hendrickson CL, Ellis SR, Heeren RMA, Smith DF (2020) Ultra-high mass resolving power, mass accuracy, and dynamic range MALDI mass spectrometry imaging by 21-T FT-ICR MS. Anal Chem 92 (4):3133–3142. doi: 10.1021/acs.analchem.9b04768 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 24.Murphy RC, Axelsen PH (2011) Mass spectrometric analysis of long-chain lipids. Mass Spectrom Rev 30 (4):579–599. doi: 10.1002/mas.20284 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 25.Kaplan DA, Hartmer R, Speir JP, Stoermer C, Gumerov D, Easterling ML, Brekenfeld A, Kim T, Laukien F, Park MA (2008) Electron transfer dissociation in the hexapole collision cell of a hybrid quadrupole-hexapole Fourier transform ion cyclotron resonance mass spectrometer. Rapid Commun Mass Spectrom 22 (3):271–278. doi: 10.1002/rcm.3356 [DOI] [PubMed] [Google Scholar]
  • 26.Chaurand P, Schwartz SA, Billheimer D, Xu BJ, Crecelius A, Caprioli RM (2004) Integrating histology and imaging mass spectrometry. Anal Chem 76 (4):1145–1155. doi: 10.1021/ac0351264 [DOI] [PubMed] [Google Scholar]
  • 27.Ma X, Chong L, Tian R, Shi R, Hu TY, Ouyang Z, Xia Y (2016) Identification and quantitation of lipid C=C location isomers: A shotgun lipidomics approach enabled by photochemical reaction. Proc Natl Acad Sci U S A 113 (10):2573–2578. doi: 10.1073/pnas.1523356113 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 28.Paine MRL, Poad BLJ, Eijkel GB, Marshall DL, Blanksby SJ, Heeren RMA, Ellis SR (2018) Mass spectrometry imaging with isomeric resolution enabled by ozone-induced dissociation. 57 (33):10530–10534. doi: 10.1002/anie.201802937 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 29.Born M-EN, Prentice BM (2020) Structural elucidation of phosphatidylcholines from tissue using electron induced dissociation. Int J Mass spectrom 452:116338. doi: 10.1016/j.ijms.2020.116338 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 30.Sud M, Fahy E, Cotter D, Brown A, Dennis EA, Glass CK, Merrill AH, Murphy RC, Raetz CRH, Russell DW, Subramaniam S, A (2007) LMSD: LIPID MAPS structure database. Nucleic Acids Res 35 (1):D527–D532. doi: 10.1093/nar/gkl838 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 31.McLuckey SA, Stephenson JL Jr., Asano KG (1998) Ion/ion proton-transfer kinetics: implications for analysis of ions derived from electrospray of protein mixtures. Anal Chem 70:1198–1202. doi: 10.1021/ac9710137 [DOI] [PubMed] [Google Scholar]
  • 32.Dehmelt HG (1967) Radiofrequency spectroscopy of stored ions I: storage. In: Bates DR, Estermann I (eds) Advances in Atomic and Molecular Physics, vol 3. Academic Press, New York, pp 53–72 [Google Scholar]
  • 33.March RE (1997) An introduction to quadrupole ion trap mass spectrometry. J Mass Spectrom 32:351–369 [Google Scholar]
  • 34.Prentice BM, McLuckey SA (2012) Analysis of high mass-to-charge ions in a quadrupole ion trap mass spectrometer via an end-cap quadrupolar direct current downscan. Anal Chem 84 (17):7562–7569. doi: 10.1021/ac301741a [DOI] [PubMed] [Google Scholar]
  • 35.McLuckey SA (2010) The emerging role of ion/ion reactions in biological mass spectrometry: considerations for reagent ion selection. Eur J Mass Spectrom 16 (3):429–436. doi: 10.1255/ejms.1031 [DOI] [PubMed] [Google Scholar]
  • 36.Wells JM, Chrisman PA, McLuckey SA (2001) Formation of protein-protein complexes in vacuo. J Am Chem Soc 123:12428–12429. doi: 10.1021/ja0170403 [DOI] [PubMed] [Google Scholar]
  • 37.Bu JX, Fisher CM, Gilbert JD, Prentice BM, McLuckey SA (2016) Selective Covalent Chemistry via Gas-Phase Ion/ion Reactions: An Exploration of the Energy Surfaces Associated with N-Hydroxysuccinimide Ester Reagents and Primary Amines and Guanidine Groups. J Am Soc Mass Spectrom 27 (6):1089–1098. doi: 10.1007/s13361-016-1359-3 [DOI] [PubMed] [Google Scholar]
  • 38.Randolph CE, Foreman DJ, Betancourt SK, Blanksby SJ, McLuckey SA (2018) Gas-phase ion/ion reactions involving tris-phenanthroline alkaline earth metal complexes as charge inversion reagents for the identification of fatty acids. Anal Chem 90 (21):12861–12869. doi: 10.1021/acs.analchem.8b03441 [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 39.Randolph CE, Blanksby SJ, McLuckey SA (2019) Towards complete structure elucidation of glycerophospholipids in the gas phase through charge inversion ion/ion chemistry. Anal Chem. doi: 10.1021/acs.analchem.9b04376 [DOI] [PMC free article] [PubMed] [Google Scholar]

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