T left

Figure 8 mother wavelet y/(t) (left) and wavelet built out of the mother wavelet by time shift b, and dilatation a. Both functions are represented in the time domain and the frequency domain. 

Fig. 6.8 Mossbauer spectra of deoxy-myoglobin, obtained in applied fields of 2 T (left) and 6.2 T (right) at temperatures of 4.2, 10, 15, 20, 30 and 50 K (from bottom to top). The solid lines were calculated using a relaxation model. (Reprinted from [34] copyright 1994 by Springer-Verlag)...

So he hasn t left fine printing behind altogether. 

Fig. 2.21 Compartmental burden [t] (left panel), solid lines model experiment with aggregation of marine snow (AGG), dashed lines experiment with satellite assimilation (SAT). Migration of the centre of gravity of the total environmental burden (right panel). Dashed lines show the location of the COG at the end of the simulation. The COG of the SAT experiment is shown in blue, the COG of the AGG experiment in red. Circles represent monthly mean COGs.

Fig. 3.17 Vertical and latitudinal distribution of PFOA mass in the global oceans [t] (left), 12/2004, fraction of mass bound to organic matter [%] (right), 06/2004.Upper panels KOC115, lower panels KOC11500.

Fig. 17. Chloramine-T (left) and Iodo-gen (right) reagents, used in radio-iodination reactions.

Fig. 2. Decay traces of differential transmission AT/T (left) and differential reflection AR/R (right) in IR spectral range.

I hope they haven t left it too late, said Fitz. 

Fig. 2 Curie-Weiss jX versus T (left), /T versus T (middle), and X versus T (right) plots of magnetic susceptibility data. In the middle plot, a diamagnetic sample shows a negative response.

Fig. 16. The stacking of trigonal-prism layers above 2 T, left 2H—MoS2 (C7), right 2H—NbSa, below 3R—MoSa...

Fig. 6-3. Mdssbauer spectra of lepidocrocite. Left, spectra recorded at 294 K and 4.2 K. Right, spectra recorded at 50 K without and with an external field of 6 T. Left, Courtesy E. Murad. Right, Murad (1996) with permission.

Figure 6. Main amplitudes describing the mode contributions to time correlation functions density-density F M k,t) (right) and charge density-charge density FggCM (fc,t) (left) in LiF at small k domain.

Fig. 14. Distribution of the order parameter A in different order parameter windows for pathways of a given length t left hand side). Matching the distributions in the windows where they overlap yields the distribution over the full order parameter range from the reactant region to the product region right hand side). The data are from simulations of proton transfer in the protonated water trimer...

Fig. 6.11 -1 The dependence of the current ratio (6.11-1) (black) and of its semidifferential (blue) ontime t(left) andpotential (right).

When done sectioning, remove all tissue waste from the machine tissue. O.C.T. left in the cryostat will turn into a sticky mess if not removed after each use. Clean... 

Yet, as we explored this issue, Joe began to see that his father s abandonment had done just that. All his life, Joe had been carrying unresolved feelings of abandonment and rejection, feelings that he d buried at the time because they seemed too powerful and overwhelming to the five-year-old boy who d had to deal with them. His adult mind understood that Joe s father hadn t left because of him. But the five-year-old Joe blamed himself, as all children tend to do. Because he had never seen the issue clearly or been willing to reexperience the grief, he had never quite realized how powerful it was. 

Figure 7. Values of when particles are illuminated by S or f incident wave. t max=l t Left Volume case. Right Surface case...

Fig. 158. The onset of magnetism in CeCi%, Auj Temperature dependence of specific heat C/T (left), and of bulk susceptibility M/B (right) for various Au concentrations. After vOn Lohneysen (1996a).

Fig, 3. Hall resistance versus magnetic field along the c axis for two (TMTSF PFg samples (P 9 kbar, T = 0.5 K). The quantized values, h/2ne2=12.9/n kQ per molecular layer, are marked on the right for sample 1. The n = 0 phase is reached above 18 T (left). Magnetoresistance of the same sample up to 25 T (right linear scale in the inset). 

Figure 1. Examples of zigzag lines, numeric codes and linear symmetry groups for structures with f2 T (left) and Cl = 2 (right) a) Example of a homogeneous structure b - d) Inhomogeneous structures of different construction.

Fig. 43. Temperature dependence of the magnetization o T) in amorphous Dyo.6oGoo4o obtained in a magnetic field of 1.8 T and 0.3 T (left-hand scale). The open circles represent data of the reciprocal susceptibility (right-hand scale).

BELOW t (LEFT) ThtS pOp-Up IS Simitar to venation II txit it makes maximum use of the overhanging card. // (centre) Note how the gutter crease does not form down the bottom part of the pop-up. To achieve this, it is necessary to draw the entire construction on an uncreased sheet, then to crease and slit only where essential, m (right) In this example, part of the slit has been formed in line with the gutter. 

Fig. 2.18. Comparison of GRE sequences at 1.5 T (left) and 7 T (right) in a patient with multiple cavernomas throughout the brain 7 T showed the larger extent of all lesions and detected much more additional lesions not seen with 1.5 T...

In the end, we either have an empty composable morphism chain, which means that our process has terminated, or we have one object a, with some coefficient t, left. In the latter case, we finish our construction by putting the object with coefficient t as the first object in the composable morphism chain that we are constructing. 

The top event in Fig. 4(a) is caused when the sum of c(Tq-T) and W(Tq) is greater than Wf(T). this is true if either value is greater than Wf(T) (left branch) or if both values are smaller than (T) but their sum is greater (right branch), these events are consequences of two primary events ... 

Figure 5. Cell division as a first-passage time (FPT) problem, (a) Schematic of stochastic cell size increase from a common initial condition. Between times t and t + At, the some growth tracks cross the threshold size, 0. Using probability conservation, the cumulative probability that the size is greater than 0 (above the black dotted horizontal line) must be equal to the complement of the cumulative probability that the FPT is less than or equal to t (left of blue dotted vertical line at t). (b) Scaling of the FPT distribution. The shape of the mean-rescaled division time distribution is timescale invariant, that is, independent of K, when there is a single timescale, 1/k a t, in the FPT dynamics.

C, 550 °C, 600 °C, and 650 °C. (b) Efficiency T (left axis) as a function of the external current density. The right axis shows the corresponding power density dissipated in the external resistor. The fuel utilization is fixed at 85% at the maximum power density for each temperature. 

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