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Herein, we show that Pd nanoparticles (NPs) can be synthesized on the highly developed surface of anodically grown TiO2 nanotube (TNT) arrays by applying a simple galvanic displacement strategy.
GCOS was also used to normalize the signal levels between different arrays by applying 50th percentiles and to calculate signal intensities or reliabilities of each probe.
3. Array normalization 1. Apply within-array normalization to single arrays by applying using the MA2C software [ 37, 38] or equivalent within-array normalizations tools.
For all uniquely mapped oligonucleotides, the available raw expression data was background corrected, array-wise quantile normalized and replicates were normalized between arrays by applying Bioconductor's limma package [ 40].
For this analysis, signals were calculated using MAS5 or PLIER in ArrayAssist v4.0 (Stratagene, La Jolla, CA) for each comparison group of 6. Probe sets with tissue-selective expression were identified from body map data generated on RAE230A arrays by applying a tissue-selective index cutoff of 5, as previously described [ 15].
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Luminol ECL was generated at the distal face of the sub-micrometer sensor array by applying an adequate positive potential.
We estimated one-dimensional (1-D) isotropic electrical conductivity profiles of the mantle for Area A and Area B separately, which fit the MT response averaged in each array, by applying an iterative topographic effect correction.
Given this, a good approximate of the residual echo can be obtained from the already available estimate for each microphone on the belt microphone array by applying a maximum over the entire array to get (widehat E_{u}^{2}(mu,k)).
Fluorescence ratios were calibrated independently for each array by applying a single scaling factor to all fluorescent ratios from each; this scaling factor was computed so that the median fluorescence ratio of well-measured spots on each array was 1.0.
Fluorescence ratios were calibrated independently for each array by applying a single scaling factor to all fluorescent ratios so that the median fluorescence ratio of array elements that passed quality-control criteria was 1.0.
The reflectivity spectra of SRR arrays shift by applying gate voltage, which modulates the sheet carrier concentration, and thereby the optical conductivity of monolayer graphene.
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