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The specificity of the DNA-microarray to detect of Campylobacter spp. in broiler chickens

The specificity of the query is insufficient to differentiate between the correct hit .

The specified signal-to-noise ratios for observe probes at the time of magnet launch .

The specimen

The specimen consists of an array of atomic columns .

The specimen geometry dependence of the 7-stress in DCB specimens for specimens with no residual stress. Solid line represents Fleck et al. solution for semi-infinite adherends.

The specimen is covered with the inhibitor molecules giving a protection against corrosion, where a thin layer developed on the specimen surfaces.

The specimens before plastic deformation .

The spectator hydride bridging between the two iron atoms does not participate in the H2 production cycle.

The spectra are dominated by sharp pre-edge resonances at about 285 eV, which can be associated with transitions from C Is core states into the lowest unoccupied molecular 7t -orbitals. The average molecular orientation,

The spectra are for a film of polypyrrole, but they are typical of the results seen for many conducting polymers. The spectra are interpreted as follows. The bottom spectrum is that of pristine polypyrrole, and the large absorption at 3.2 eV corresponds to the transition from the top of the valence band to the bottom of the conduction band—the HOMO-LUMO transition that defines the optical band gap. However, defects are present even in this sample, and the weak bands at 0.7,1.4, and 2.1 eV involve polarons and bipolarons. As doping progresses moving up

The spectra are of the trimethylsilyl derivatives of 2-deoxytetronic acid .

The spectra are smoothed but not baseline corrected. The spectrum of the electrolyte solution was subtracted.

The spectra are very similar to that of the linear styrene dimer 1, except for the virtual absence of vinyl protons. In contrast, the products obtained with BF30Et2 in polar solvents, such as GHjC j, are cross-linked polymers insoluble in organic solvents.

The spectra at the temperatures for were 35, 50, 55, and 65 C, respectively, and are drawn with a solid line. For reference, the spectrum at 25 C is shown in each panel with a dotted line.

The spectra can be compared to reference material or interpreted to provide additional stmctural information. The detection and identification of impurities spotted on TLC plates

The spectra collected from the polymer laminate are displayed as a function of position along the sample, in a waterfall display . The chemical differences in the layers are clearly seen. For example, the top layer has a large broad peak at about 3400 cm .

The spectra demonstrate the need for such detailed separation schemes, for the spectra of the total saturates are too detailed to allow any significant conclusions as to contributions from the various molecular types present.

The spectra for a mixture of 1890 carbon atoms per atom of boron are plotted for graphite moderation and for a free gas model.

The spectra for obtained with the bare G-matrix . All three potentials have been employed. Energies in MeV.

The spectra for Sc. Notations as in the previous figure.

The spectra for the pyrazine molecule. The damping parameter is 30 fs. All panels display the result for the exact 24-mode model . Panel A

The spectra from device I and II are characteristic of molecular phosphorescence as clearly seen from their comparison at different voltages with the PL spectrum . The DCM2-doped Alq3 layer of device III becomes dominated by their phosphorescene from the PtOEP-doped Alq3 layer in device II.

The spectra in a boric acid solution at 291 K computed from the H2O model and a free H model are compared with the experimental results obtained by Poole. The boron concentration is such as to give an absorption cross section at 2200 meters second of 4.54 bams per H atom.

The spectra in Figs, lc and Id show the B KLL transitions, respectively.



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