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X 650 pm2 fluorescence microscopy image of the TM4 fluorescent monolayer on glass in which Cu2 and Ca2 were printed with PDMS stamps with an array of 10 pm dots. This image clearly shows that the fluorescence of the glass slide was quenched and enhanced where the Cu2 and the Ca2 ions, respectively, were printed, i.e. the dotted pattern 87. Copyright Wiley-VCH Verlag GmbH Co. KGaA. Reproduced with permission

X 7 - T curves of pure PP at different cooling rates.

X 7 liquid crystal matrix array without crosstalking using two frequency-addressing .

X 80 mr AFM height image of a polymer blend film. The phase separation of the film is ordered in a rectangular region by the underlying substrate shows unpattemed phase separation. Reprinted with permission

X 823 3D STM image. An Ag crystal growing at a step edge is shown. Arrow indicates the step at which the image showed in

X 8250 STM image pole

X 85 nm in-situ STM images obtained during the electrodissoludon of silver in 1 M

X 9835 3D STM image showing electrodeposited Ag at HOPG substrate defects

X and Y denote sulfur or oxygen. The dots in the pt orbital indicate the number of electrons.

X at High and Low Levels of Starvation

X axis time, Y axis tremor intensity, approximately 45-50 s for each stimulation condition, E effective

X band EPR compound 6 in n-butyronitrile. EPR

X band EPR spectra at 293 K of Fe22

X Br, I, n 10 and schematic representation of the disc-like arrangement.

X Breakdown of Costs tor Base Case

X Calculated intensity profiles for a simple, full aperture objective . The same NA and wavelength were used for both calculations. Note the large first-order diffraction ring for die Schwarzschild objective.

X Cff2hol in combination with ten-butyl diazoacetate is highly exo-selective exo endo 140

X Chart

X Charts for Insertion Loss Measurement Standards.

X Cl dots represent B.

X computer diagram of the generalized Van der Pol oscillator with F0 — 0 X. for 4 different values of initial conditions. Both the small and large amplitude oscillations are shown.

X Consequences of Ihe recoil effeci caused by y-ray emission and absorption in isolated nuclei. The transition lines for emission are separated by 2 Er 10 T. There is no overlap between emission and absorption line and hence no re.sonanl absorption is possible

X constitutes an extension of the preceding discussion

X Curve erf the isothermal aging

X curve of carboxyhemoglobin . Quarter millimolar extinction coeflS-oients based on graph represents the mean value



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