Transitions plotted

Figure 10 The calculated interaction energy for (a) the long-axis and (b) the short-axis transition plotted against a using the number of chromophores (p,q,r) as a parameter (444) (3,4,2) (344) ...

Fig. 5.5 Conductivity of doped and compensated GaS in various magnetic fields near the transition, plotted against T1/3 (Maliepaard et ai 1988).

FIGURE 14.7 (a) Experimental TREPR spectra (only the two intense central transitions are shown), obtained upon 248 nm photolysis at 122° C of PAA (leading to radical 7a) in water, at the pH values indicated, (b) Integrated intensities of these transitions plotted as a function of solution pH. 

In order to determine the efficacy of spermidine to provoke the B->Z transition, plot the net optical density values against the concentration of spermidine. The midpoint concentration isdetermined from this plot at 50% increase in net optical density. 

Mott argued that a small number of free electrons should not be possible at a very low temperature, because a small number of electrons and ions will attract each other and will form neutral pairs. This is not the case if they are strongly screened. The number of free electrons must change discon-tinuously at a Mott transition. Plotted as in fig, 13 the transition indeed looks rapid , making Hg a possible candidate for the study of a phase transition in a finite system. The insert of fig. 13 is taken from an early paper by Mott. It shows the band gap e as a function of the inverse distance in a crystal. In an independent electron calculation, one obtains the linear rise a). Including sufficient correlation leads to the discontinuous jump (b), i.e. the Mott transition. The similarity of the insert to the experimental result (which includes correlation of course) and the theoretical result (which neglects correlation), respectively, is obvious. The abscissa (z or l/d) is in both cases a measure of the bandwidth. 

Similar transition plots as well as complex phase diagrams have been generated with mixtures of lipids. The physical property of a lipid mixture is a collective property determined by each of the component lipids. A large number of studies indicate that the state... 

FIG U RE 6.7 (a) Oxygen and redox potential (Eh) profile with water table depth for transitional plot (sampling... 

Figure 5.4 Correlation of optical and tunneling spectroscopy data for InAs QDs. The inset shows a schematic of the CB and VB level structure and optical transitions I, II, and III a,b and c in Figure 5.3). (a) Comparison of the size dependence of the low-temperature optical band gap (transition I) afterCoulombcorrection (open diamonds), with the band-gap measured by the STM (filled diamonds) (b) Excited transitions plotted versus the band gap for tunneling and optical spectroscopy. The two lower data sets (II) depict the correlation...

Fig. 2. Oscillatory behavior of the normalized specific heat jump at the metal-FTSDW transition, plotted as a function of the magnetic field.

Figure 5.5. Transitions, plotted as independent variable versus dependent variable, showing a response limited to a partieular range of independent variable. (A) Representation of the thermally driven contraction for an elastic-contractile model protein, such as the cross-linked poly(GVGVP), plotted as the percent contraction (dependent variable) versus temperature (independent variable). The plot shows a poorly responsive range below the onset of the transition, the temperature interval of the inverse temperature transition for hydrophobic association, and another poorly responsive region above the tem-...

Figure 6.7 Experimental transition plot. The numbered data points represent specific conditions tested by Ford et al. (2008).

Fig. 5.12. Left panel Schematic of the rotational energy levels for both the ground and U3 = 1 vibrationally excited state of CH3. At supersonic jet temperatures of 25 K, essentially all of the population collapses into the two lowest spin allowed rotational states. The five dipole allowed transitions from these two states are indicated above. Middle panel Five transitions for both that from 7 = 1/2 (right panel) and those from 7 = 3/2 (middle panel) observed in the slit jet expansion. The shape of the absorption profile is dictated by both spin-rotation and nuclear hyperfine splitting. The magnitude of the splittings and the positions of each sub transition are shown in the tree above. A stick spectrum is plotted below, along with the Gaussian from each sub transition plotted in grey.

Fig. 14.25. Hysteresis curve for a phase transition. Plotted is the laser-induced fluorescence rate as a function of laser power at a fixed detuning (Ai/ 5= -120 MHz). At about 170 /iW laser power the phase transition occurs from the disordered ion cloud to the ordered Wigner crystal and at 400 /xW the opposite phase transition is observed [14.70]...

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