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Observable variables for DSC single dynamic scan kinetics experiment.

Observation area of the radar network system.

Observation at a low incidence angle of a polycrystalline thin film in which the crystals are randomly oriented

Observation by atomic force microscopy

Observation by BF and DF of a glassy pocket in a mullite ceramics and CBED pattern of this very small glass zone showing the amorphous halo

Observation by differential interference contrast suspended in a phosphoric buffer T 298 K, pH 7.0, 485 nm,

Observation by in plane-view optical microscopy of the zirconia film

Observation by Wong and Sondheimer .

Observation data from different areas of the paper miU.

Observation framework using Two-Way Link framework.

Observation from side using mirror

Observation geometry at a limiter lock of TEXTOR global

Observation Method of observation of co-crystallization of gases using a single-crystal adsorbent.

Observation of a buckybelt under mass spectrometric conditions

Observation of a CIDNP effect on fragmentation of radical 5

Observation of a cross sectional thin foil prepared from a CdS GaP sample .

Observation of a droplet spreading in total wetting, using a video camera. The spreading function 7 - is deduced

Observation of a field-induced water bridge with amplitude modulation AFM. Depicts the tip s oscillation before, during, and after the application of a voltage pulse for 20 ms that did not involve the formation of a water bridge , Depicts the tip s oscillation before, during, and after the application of a voltage pulse for 20 ms that involved the formation ofa water bridge , Step ill is indicative of the formation of a water bridge because the oscillation does not recover its initial value once the pulse is off. Each dot in the oscilloscope traces represents an instantaneous position of the atomic force microscope tip. Data adapted from Refs. 19, 53, 69, and 81.

Observation of a line at low resolutions

Observation of a narrow saturation resonance by use of a single strong coherent traveling wave and a countertraveling weak probe wave, Absorption of probe wave as a function of frequency.

Observation of a radical cation by ESR spectroscopy

Observation of a thermoelastic inversion point for natural rubber

Observation of alumina particles and slurries Upper

Observation of an inverted Lamb dip in a He-Ne laser at 3.39 xm with an intracavity CH4 absorbing cell. Output power versus laser-cavity tuning, with double scan. The saturated absorption peak has an amplitude of about 2 with a 400 kHz width, and is nicely centered on the Ne Doppler gain curve.

Observation of atmospheric CO2 concentrations and Earth s



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