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of the compounds of <strong>in</strong>terest. High-resolution imag<strong>in</strong>g is typically accomplished by us<strong>in</strong>g a homogenous spray coat<strong>in</strong>g or a spotted<br />

array. The best spatial resolution is achieved by a spray coat<strong>in</strong>g that is homogeneous while improved spectral quality and precision is<br />

achieved by us<strong>in</strong>g an array that is densely spotted. On the other hand, a heterogeneous coat<strong>in</strong>g provides locations on the specimen that<br />

are either dilute or concentrated for ablation. Crystal formation, as a result, is random and images are both highly pixilated and poor <strong>in</strong><br />

quality. Robotic spott<strong>in</strong>g <strong>in</strong>struments are commercially accessible and use a variety of techniques such as capillary deposition, <strong>in</strong>k-jet<br />

pr<strong>in</strong>ter, piezoelectric and acoustic methods. Robotic spray-coat<strong>in</strong>g <strong>in</strong>struments are also available that use either a thermally assisted<br />

spray or a mist-nebulizer [16].<br />

The best type of MS detector for proteomic analysis of biological tissue is the time-of-flight or TOF MS. The TOF detector<br />

complements the pulsed laser used by MALDI. In addition, it is easy to ma<strong>in</strong>ta<strong>in</strong>, has a simple design, is capable of detect<strong>in</strong>g multiple<br />

m/z ratios, is efficient <strong>in</strong> ion-transmission, and has a theoretically unlimited dynamic range [16]. Ions generated dur<strong>in</strong>g the MALDI<br />

process are accelerated through the field-free drift tube of the TOF detector. The ions collect at the multichannel plate detector where<br />

the small m/z ions arrive first and the large m/z ions arrive last. If properly calibrated, then the arrival time is converted to m/z ratio via<br />

m 2Vt<br />

=<br />

2<br />

z L<br />

2<br />

Where V is the voltage potential applied to accelerate ions, t is the time the ion arrives at the detector, and L is the length of the fieldfree<br />

drift tube [2].<br />

MALDI/IMS quantification<br />

To quantify prote<strong>in</strong>s or peptides us<strong>in</strong>g MALDI IMS, the precision among pixels should be good. In other words, two neighbor<strong>in</strong>g<br />

pixels with the same prote<strong>in</strong> concentrations should provide the same mass spectra. These spectra typically do not differ from each<br />

other by more than 15%. Some of the items to consider if there is a significant difference <strong>in</strong>clude extraction efficiency of the MALDI,<br />

ionization efficiency of a particular compound, ion-suppression effects and the effect of post-acquisition process<strong>in</strong>g. In particular,<br />

sample preparation and matrix application are the two techniques that need to be mastered to obta<strong>in</strong> good precision among pixels.<br />

A constant laser power and voltage should also be ma<strong>in</strong>ta<strong>in</strong>ed with<strong>in</strong> the assay to achieve maximum precision. To prevent variation<br />

among operators, robotics is typically employed. It is important to note that even if these parameters are kept under control and high<br />

reproducibility is achieved, estimation of relative concentrations of two different prote<strong>in</strong>s is still difficult to obta<strong>in</strong> by compar<strong>in</strong>g peak<br />

areas or peak heights [16].<br />

MS reproducibility should be accurately estimated when attempt<strong>in</strong>g to correlate MS signal <strong>in</strong>tensities to values with biological<br />

mean<strong>in</strong>g. Statistical analysis and data preprocess<strong>in</strong>g are tools a scientist can use to probe the biological mean<strong>in</strong>g from these data. Data<br />

preprocess<strong>in</strong>g steps <strong>in</strong>clude background removal algorithms, signal <strong>in</strong>tensity normalization and peak alignment [17]. The purpose of the<br />

normalization of signal <strong>in</strong>tensity to the total ion current is to m<strong>in</strong>imize variations <strong>in</strong> the sample preparations. As a result of these data<br />

preprocess<strong>in</strong>g steps, a new ion image can be generated that better represents the biological system [16].<br />

After the data preprocess<strong>in</strong>g steps are completed, an average mass spectrum is either taken of each target area with<strong>in</strong> a specimen<br />

or of each tissue specimen itself. Statistical analyses are then performed on each of these spectra. Pr<strong>in</strong>cipal component analysis (PCA)<br />

is a methodology used to rank the variance <strong>in</strong> the system to determ<strong>in</strong>e the number of significant components that are <strong>in</strong> the system<br />

[17]. Scores can be assigned to components based on how it changes its signal <strong>in</strong>tensity relative to the standard deviation of multiple<br />

experiments. This methodology is called significance analysis of microarrays or SAM. The changes with<strong>in</strong> multiple experiments help<br />

to estimate the fraction of components that are seen by chance (potential false positives) when scores are greater than a predeterm<strong>in</strong>ed<br />

threshold. SAM specifically exposes components that demonstrate a significant change between two groups of tissues. A method that<br />

bl<strong>in</strong>dly groups samples based on their profiles is hierarchical cluster<strong>in</strong>g analysis or HCA. HCA specifically computes the dissimilarity<br />

between particular experiments [16]. Based on the dissimilarity values, a dendrogram is created, which clusters or groups similar<br />

components and depicts these similar groups <strong>in</strong> a graph that looks similar to a tournament bracket [17].<br />

Surface Characterization<br />

A specific <strong>in</strong>strument used for the characterization of prote<strong>in</strong>s is the atomic force microscope (AFM). The AFM is made out of a<br />

cantilever with a tip where van der Waals forces are measured between the tip and the sample surface. These van der Waals forces cause<br />

the tip to be redirected, and this movement is optically detected by the <strong>in</strong>strument. Constant force applied to tip enables a strict up-anddown<br />

movement of the tip provid<strong>in</strong>g data on the topography of the sample surface. The flexibility of the AFM lies <strong>in</strong> the fact that it can<br />

be used for non-conduct<strong>in</strong>g samples [2]. The three modes used for AFM are contact mode, non-contact mode, and tapp<strong>in</strong>g mode [2]. In<br />

contact mode, the tip makes contact with the sample at all times. If the sample is a liquid, then surface tension forces brought about by<br />

adsorbed gases or the surface layer of the liquid can pull the tip <strong>in</strong>to the sample. As a result, the tip can potentially damage the sample<br />

and dampen the tip. This mode is not the best sett<strong>in</strong>g for biological or prote<strong>in</strong> samples. In tapp<strong>in</strong>g mode, the tip briefly makes contact<br />

with the surface and is immediately retracted. The typical oscillation is on the order of hundreds of kHz. The least popular mode of AFM<br />

is the non-contact mode where the tip is constantly a few nanometers away from the surface of the sample. Not surpris<strong>in</strong>gly, the van der<br />

Waals forces detected on the tip and cantilever are much smaller [2].<br />

In AFM, the data provided is a force curve, which is a plot of the force applied onto the tip versus the displacement of the tip. The<br />

location of the tip and movement of the AFM cantilever can be detected down to the nanometer thanks to the reproducible piezoelectric<br />

detection units. The movement of the cantilever can be used to compute the force applied us<strong>in</strong>g Hooke’s law [18]. There are typically<br />

two plots provided by a force curve. When the tip is com<strong>in</strong>g toward the surface of the sample, this is the approach<strong>in</strong>g curve. When the<br />

tip is mov<strong>in</strong>g away from the surface of the sample, this is the retract<strong>in</strong>g curve. With respect to noise, the two curves are overlaid on top<br />

of each other if there is no sample present. There should be two regions to these curves. There should be a horizontal region called the<br />

noncontact region that represents the basel<strong>in</strong>e when a tip is not touch<strong>in</strong>g a surface. There also should be a region of the curve which rises<br />

up from the noncontact region called the vertical contact region which accounts for the van der Waals forces measured by the tip. The<br />

contact po<strong>in</strong>t is the spot on the force curve where the two regions meet and it is a critical portion of the force curve because it becomes a<br />

reference as to where the tip made contact with the surface [19].<br />

The “polyprote<strong>in</strong> strategy” has been used to <strong>in</strong>vestigate prote<strong>in</strong>s us<strong>in</strong>g AFM, especially the globular prote<strong>in</strong>s [19]. This technique<br />

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