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Probe opening windows

A. H. Zewail By increasing the resolution, the probe opens a spatial window at a given intemuclear separation (R). Thus, we can observe the motion to the right and the motion to the left as the wavepacket crosses the region of the probe. The observed splitting gives the trajectory in R and t and hence the spatial resolution A/ . [Pg.47]

In the two-point probe configuration, two electrodes serve as both current and voltage sensing probes, as shown in Fig. 5.11 [60] in the diagram, open window A allows the membrane to be exposed to the environment. For this method, the current and voltage are measured from two identical probes. Because the electrode/membrane interfacial impedance is always included in... [Pg.162]

Gas flow ratemeter with open window G-M probe... [Pg.205]

The Evaluation system is a Windows based open system through DLL, Dynamic Link Library, which provides great flexibility in evaluation and presentation of data. It also makes it possible to customise evaluation and images for special applications The time gates can be set after testing and there is a 256 colour range for amplitude. The software include FFT -facilities which enables measurements on used probes for parameters such as center frequenzy and bandwidth. [Pg.864]

Incorporation of fluorine into a biological substrate opens a spectral window for viewmg biomolecular structure and dynamics in solution With mmimal background mletference, fluonne NMR can provide clear spectral information for fluorme conlainmg macromolecules, in contrast to an indecipherable mass of signals from proton or carbon NMR Whether the fluonnated unit is termed a probe, tag, marker, or reporter group, its function is the same to act as a beacon of spectral information... [Pg.1070]

Recent observations of the HF (1-0) R9 line at 2.3 /tm with the Phoenix spectrograph on the Gemini-South telescope has opened a new window that sheds light on understanding the chemical evolution of fluorine and the nuclear processes that produce this element. Until recently, only a small number of observations of fluorine were available and the trend of fluorine abundances with metallicity had yet to be probed in the Galaxy. [Pg.46]

Instead of deleting a trace, we will display a current trace in a new window. Select Window and then New Window from the Probe menus. A new empty window will open ... [Pg.197]

A second method can be used to find the upper 3 dB frequency found in the previous section. We will continue from the end of the previous section. First, hide the cursors by selecting Trace, Cursor, and then Display from the Probe menus. Next, select Window and then New Window to open a new Probe window ... [Pg.294]

Run the PSpice simulation Select PSpice and then Run from the Capture menu bar. When the simulation is complete, the Probe window will open. Add the trace DB(V(VO) ) to plot the gain in decibels. Use the cursors to label the mid-band gain, and upper and lower -3 dB frequencies. Your cursor values may be slightly different than those shown here. [Pg.299]

The plot shows four Bode plots, one for each value of RF V3l. We see that for larger gains the bandwidth is reduced. This example will be continued in the next section (Section 5.G), which starts with the screen capture above. You may wish to keep the Probe window above open so that you can easily continue with the next section. [Pg.310]

When the simulation is finished, Probe will run. When the Probe window opens, notice that the x-axis is now the time axis. Add traces V(VIN)and V(VO) to observe the input and output of the regulator. To add a trace select Trace and then Add Trace from the Probe menus or press the INSERT key. You will see the following plot ... [Pg.351]

C Display Probe window when profile it opened]... [Pg.518]

Weckhuysen and coworkers (Nijhuis et al., 2003) described equipment suitable for parallel Raman and UV-vis spectroscopic measurements. Openings on the opposite sides of a furnace allowed acquisition of Raman and UV-vis spectra through optical grade windows in a tubular quartz reactor. UV-vis spectra were recorded at 823 K. Gas-phase analysis was achieved with mass spectrometry and gas chromatography. A more advanced version of the design (Nijhuis et al., 2004) accommodates four optical fiber probes, placed at 10-mm vertical spacing along the tubular reactor. The temperature that the fibers can withstand is 973 K the reported spectra characterize samples at 823 K. [Pg.165]

The shape of the minimum in the surface is experimentally probed by vibrational spectroscopy. It is here that the computations can make direct coimection with experimental information. Formation of the H-bond from a pair of isolated molecules converts three translational and three rotational degrees of freedom of the formerly free pair of molecules into six new vibrations within the complex. The frequencies of these modes are indicative of the functional dependence of the energy upon the corresponding geometrical distortions. But rather than consisting of a simple motion, for example, H-bond stretch, the normal modes are composed of a mixture of symmetry-related atomic motions, complicating their analysis in terms of the simpler motions. In addition to these new intermoleeular modes, the intramolecular vibrations within each of the subunits are perturbed by the formation of the H-bond. The nature of each perturbation opens a window into the effects of the H-bond upon the molecules involved. The intensities of the various vibrations carry valuable information about the electron density within the complex and the perturbations induced by the formation of the H-bond. [Pg.138]

The development of local probe techniques such as Scanning Tunneling Microscopy (STM) or Atomic Force Microscopy (AFM) and related methods during the past fifteen years (Nobel price for physics 1986 to H. Rohrer and G. Binning) has opened a new window to locally study of interface phenomena on solid state surfaces (metals, semiconductors, superconductors, polymers, ionic conductors, insulators etc.) at an atomic level. The in-situ application of local probe methods in different systems (UHV, gas, or electrochemical conditions) belongs to modem nanotechnology and has two different aspects. [Pg.329]


See other pages where Probe opening windows is mentioned: [Pg.150]    [Pg.107]    [Pg.146]    [Pg.1720]    [Pg.724]    [Pg.266]    [Pg.93]    [Pg.264]    [Pg.133]    [Pg.8]    [Pg.375]    [Pg.256]    [Pg.104]    [Pg.603]    [Pg.1070]    [Pg.2231]    [Pg.48]    [Pg.48]    [Pg.75]    [Pg.400]    [Pg.661]    [Pg.75]    [Pg.101]    [Pg.647]    [Pg.1]    [Pg.27]    [Pg.79]    [Pg.22]    [Pg.236]    [Pg.248]    [Pg.80]    [Pg.1720]    [Pg.281]   
See also in sourсe #XX -- [ Pg.124 ]




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