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Transformation and normalization of oligonucleotide microarray data

Transformation and normalization of oligonucleotide microarray data

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<strong>Transformation</strong> <strong>of</strong> <strong>oligonucleotide</strong> <strong>microarray</strong> <strong>data</strong>[Fig. 3. The transformation y= ln y − 2.74+ √ ](y − 2.74) 2 +4300over the range <strong>of</strong> the untransformed <strong>data</strong>. The dotted line isln [2(y − 2.74)], the equivalent log transformation.(b)Fig. 4. (a) Median measured intensity versus IQR for the <strong>data</strong> transformedusing the procedure outlined in this paper, including theremoval <strong>of</strong> the chip effect. The line is a loess smooth with degree 1<strong>and</strong> span 2/3. (b) The rank <strong>of</strong> the median measured intensity versusIQR range for the <strong>data</strong> transformed using the procedure outlined inthis paper, including the removal <strong>of</strong> the chip effect. The line is a loesssmooth with degree 1 <strong>and</strong> span 2/3.Fig. 5. QQ plot <strong>of</strong> N(0, 0.094) <strong>and</strong> the errors <strong>of</strong> the <strong>data</strong> transformedby the procedure outlined above. The st<strong>and</strong>ard deviation (0.094) isthe robust estimate <strong>of</strong> the st<strong>and</strong>ard deviation <strong>of</strong> the errors (IQR <strong>of</strong>the errors/1.349).are scatter plots <strong>of</strong> the median <strong>and</strong> IQR <strong>of</strong> the transformed<strong>data</strong> (c = 4300) from which the flask effects had first beensubtracted. Note that the loess lines in both plots are veryclose to constant. The errors are symmetric but long-tailedcompared to a normal distribution, as is shown in the QQ plotin Figure 5.We also examined the stability <strong>of</strong> the solutions to startingpoints <strong>and</strong> parameters <strong>of</strong> the process. Whether α is estimatedor assumed to be zero, given the granularity <strong>of</strong> the <strong>data</strong> <strong>and</strong>the nature <strong>of</strong> the median <strong>and</strong> the IQR, there are <strong>of</strong>ten twosolutions that differ by a negligible amount as long as thesame value <strong>of</strong> h is used <strong>and</strong> depending on whether the startingvalue for α is lower or higher than the final estimated value.The procedure is not sensitive to the initial values <strong>of</strong> c <strong>and</strong>ks. The only factor that has a significant effect is h, probablydue to the rapid fall in measured intensity at the high levels.As noted above, when h = 125, we found c = 4300 (fromσ ɛ = 8.20 <strong>and</strong> σ η = 0.125 with α = 2.74). When h = 200,we found c = 4900 (from σ ɛ = 8.22, <strong>and</strong> σ η = 0.117 withα = 2.73). If α is assumed to be zero, then the algorithmconverges more quickly, taking only seven or eight iterations,but to essentially the same values (c = 4400 when h = 125<strong>and</strong> c = 5000 when h = 200). It is important to note herethat precise estimation <strong>of</strong> the transformation parameter is notnecessary, since transformations with similar parameters canbe indistinguishable from each other. Since the transformationconstant is not <strong>of</strong> direct interest in itself, but just a way to stabilizethe variance, there is little need for confidence intervals.[See Durbin <strong>and</strong> Rocke (2003) for confidence intervals for thetransformation constant computed using maximum likelihoodestimation.]The linearity <strong>of</strong> the chip effect, η j , on the transformed <strong>data</strong>was checked using Tukey’s ODOFFNA (one degree <strong>of</strong> freedomfor non-additivity) method [Tukey (1949)], which correspondsto adding a term to the model y ij = µ+µ i +n j +e ij1821

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