Figure 2. 4. (a): The lower two bands from Fig. 2.2 in the Nambu-Gorkov convention (with parameters qµ = 4.5, zw = 1, mΨ = 1). (b): Energy spectrum for constant gauge field qA0 = qµ = 4.5 and linear fixed scalar profile φ(z) = z at η5 = 0.25 (zw = 1, mΨ = 1). The spectrum is gapped at the Fermi surface. We determine the Green’s function by spectral decomposition. For this we solve the Dirac eigenvalue problem in presence of both the (back- reacted) scalar and gauge field H(i→k, z)χ→k,n(z) = ω→k,nχ→k,n(z). (2.21)
Figure 2. 2 illustrates the existing land uses within the Assessment Area for both PDAs and supporting infrastructures.
Figure 2. Example of Proposition AA Attribution to Construction Sign This Project was made possible in part by Proposition AA Vehicle Registration Fee funds
Figure 2. .11. Quiver for (3, 2) case represented in ’triangular’ form. spondence results in the ’enhancement’ of the symmetry group 19: a pair of commuting Weyl groups A(1) × (1) is now embedded into larger
Figure 2. Scatter plot describing the relationship between depressive symptoms (CESD score) and perceived social support (MOS-SSS) among HIV positive individuals obtaining anal cancer screening at Xxxxx De Xxxx Center Atlanta, GA 28 Figure 3. Scatterplots with regression line between depressive symptoms (CESD score) and Affectionate social support among HIV positive individuals obtaining anal cancer screening at Xxxxx De Xxxx Center Atlanta, GA 29 Figure 4. Scatterplots with regression line between depressive symptoms and tangible social support among HIV positive individuals obtaining anal cancer screening at Xxxxx De Xxxx Center Atlanta, GA. ................................................................................................................................................................... 30 Figure 5. Scatterplots with regression line between depressive symptoms and Emotional and informational social support among HIV positive individuals obtaining anal cancer screening at Xxxxx De Xxxx Center Atlanta, GA 31 Figure 5. Scatterplots with regression line between depressive symptoms and positive social interaction social support among HIV positive individuals obtaining anal cancer screening at Xxxxx De Xxxx Center Atlanta, GA 32 Figure 6. Scatterplots with regression line between depressive symptoms (CESD score) and smoking status among HIV positive individuals obtaining anal cancer screening at Xxxxx De Xxxx Center Atlanta, GA. ................................................................................................................................................................... 33
Figure 2. Evolution of cysts from epithelial cells of the renal tubules. Cystic kidneys (left), result from the growth of multiple fluid-filled cysts that originate in the renal tubules (middle) and continue developing through different pathophysiological mechanisms (right). Cysts evolve from individual cells ultimately leading to the development of blister-like structures. Once the cysts separate from the nephron that originated them, their collective effect leads to the displacement of the normal renal parenchyma and the formation of a cyst-filled kidney with reduced functional capacity. Figure modified from Xxxxxx G, et al., 2013 [38].
Figure 2. 1.6 A. The intensity of absorption for an EPR spectrum plotted versus the magnetic field. B. A typical EPR absorption spectrum. C. The first derivative of an EPR absorption spectrum; due to experimental conditions the first derivative absorption curve is typically observed. The relative intensity of absorption of observed transitions is determined by the orientation the angle, , of the molecule relative to the magnetic field, B, or approximately, by sin d dB . This angle weighting leads to the characteristic EPR line shape. The magnetic field moves from along the z-axis into the x,y-plane, as increases from 0°, when the magnetic field is aligned with the z-axis, to 90°, when the magnetic field is in the x,y-plane (Figure 2.1.7).
Figure 2. .1.7 A. EPR absorption spectrum for a powder sample (i.e. all and orientations) of a Cu(II)-bis-cis imidazole complex (see chapter 5 for further details). B-F. EPR absorption spectra for a particular orientation of , at a fixed value ( ⁰. The dotted line corresponds to the EPR absorption spectra at a particular value, and the solid line is the EPR absorption line multiplied by sin, (to observe the angle weighting effect). The spectrum was collected at 120 K,
Figure 2. Same as Figure 1 but for the IPV SST patterns. From Xxxxxx et al. 2016a A number of sensitivity studies have been performed to test the robustness of the procedure to observed SST datasets, filtering procedures, time periods (see the technical notes). The above patterns were found to be very robust among the different tests. The netcdf files containing the AMV and IPV SST anomalies are on the wiki (also available on request to xxxxxx@xxxxxxx.xx) and will be put on JASMIN. IMPORTANT Warning: please make sure you read attentively the two technical notes as they contain recommendations on some subtle points that do matter in the implementation of the protocols. Major outcomes of the work AMV and IPV WP5 sensitivity experiments defined AMV and IPV SST patterns are ready to be used for the WP5 PRIMAVERA simulations
Figure 2. (a) Coulomb staircase Ids-Vds characteristics in a Si NW SET, from 8K – 160K. Curves offset 0.1 nA per temperature step for clarity. (b) Coulomb staircase at 8 K, modulated by gate voltage Vgs. The temperature dependence of the Ids-Vds characteristics, from 8 K to 300 K, is shown in Figure 4, on log (a) and linear (b) scales. The Coulomb staircase persists up to ~220 K, beyond which it is thermally overcome. A low-current Coulomb blockade region is observed up to ~140 K. A maximum temperature for single-electron effects of ~200 K suggests an effective MTJ single-electron charging energy ~17 meV and capacitance ~5 aF. Room temperature operation requires a reduction of this to ~1 aF or less.
