For research use only. Not for use in diagnostic procedures.
A major limitation of MALDI MS imaging using conventional MALDI Tof and Tof-Tof analysers is the absence of any additional dimension of separation. Owing to the complexity of the samples under investigation this poses a major risk of isobaric ions distorting the ion distribution and thus invalidating results. With the introduction of the Waters MALDI SYNAPT HDMS System, it is possible to separate ions using ion mobility separation (IMS) prior to mass analysis.
A major limitation of MALDI MS imaging using conventional MALDI Tof and Tof-Tof analysers, which separate by m/z, is the absence of any additional dimension of separation. Owing to the complexity of the samples under investigation, this poses a major risk of isobaric ions distorting the ion distribution and thus invalidating results.
With the introduction of the Waters MALDI SYNAPT HDMS System, it is possible to separate ions using ion mobility separation (IMS) prior to mass analysis. IMS allows for the separation of ions according to their size, shape, and charge state. Using this technique it is possible to separate different compound classes, giving additional confidence that the true distribution of an ion of interest is observed. On the MALDI SYNAPT HDMS System, Waters’ unique high efficiency IMS system has been combined with a state-of-theart imaging solution. Figure 1 shows two ways in which a MALDI HDMS imaging dataset can be mined, firstly imaging data analysis using BioMap and secondly HDMS data analysis of the same data using DriftScope.
The sample under investigation was a thin section of rat kidney. A 12 μm section was produced using a cryostome and deposited on thick aluminum foil. a-cyano-4-hydroxycinnamic acid matrix was applied evenly to the sample in several coats using an airbrush. The sample was mounted on a target plate.
The area to be imaged was selected using MALDI Imaging Pattern Creator (Waters Corporation, Manchester, UK) (see Figure 2). Data were acquired on a MALDI SYNAPT HDMS System operated in HDMS mode over the m/z range of 10 to 1000. Spatial resolution of 250 μm was selected and 600 laser shots were acquired per pixel at a laser repetition rate of 200 Hz. After acquisition, HDMS data evaluation was performed using Driftscope (Waters Corporation, Manchester, UK). Data were converted into Analyze file format using MALDI Imaging Converter (Waters Corporation, Manchester, UK) for image analysis using BioMap (Novartis, Basel, CH).
The combined Driftscope mobility plot showing drift time (x-axis) versus m/z (y-axis) obtained from the kidney sample is shown in Figure 3. It can clearly be seen that ions of similar m/z (on the same horizontal line in the plot) are separated in the ion mobility dimension. A full 3D data set is acquired at every spatial position consisting of m/z, IMS, and intensity, ensuring maximum flexibility for mining the data. It is also possible to perform a targeted experiment where only a small mobility and/or m/z range is acquired (not shown here).
Figure 4 shows an ion image for the ion of m/z 402.01 without ion mobility separation. When the ion mobility range from 2.7 ms–3.3 ms is combined, the ion image for m/z 402.01 has a significantly lower background noise level, as illustrated in Figure 5. Finally, Figure 6 shows the ion image of the interfering background ion with m/z 402.07 after it has been selected using ion mobility (drift time 3.4–4.1 ms).
The use of HDMS clearly helps to provide the true spatial tissue distribution of the endogenous metabolite of mass 402.01 Da by removing any contribution of the interfering matrix ion of m/z 402.07 Da.
720002443, December 2007