FIG Sample Clauses

FIG. Calibration functions (a) u(VG) , (b) v0(VG), and (c) C(VG), filled circles L = 22 nm, symbols rxr L = 26 nm, and open rectangles L = 30 nm. In dotted lines the four-constants-fit u = 0.09, C = 0.1, β = 2/V , and v0 = −1V . The solid black line in (b) marks the position of m. The function ∆Jrms(VG) is then minimized by varying in (6) the parameters C, v0, and

FIG. A limited amount of data was collected in grower’s fields due to difficulty of access, field size and frequent pesticide applications. At the UC DREC site, a large set of observations about insect pest occurrence was collected.

FIG. 3: Difference between the electron phase calculated for a WSe2 bilayer using the DFT and IDFT methods. The area shown corresponds to the area marked by a blue rectangle in Fig. 1 in the main text. Positive values correspond to a larger electron phase in the IDFT method. The largest difference in electron phase can be found along the bonding directions of the WSe2 crystal, whereas only small differences are found in the interstitial areas. The standard deviation of the difference image is 3 mrad.

FIG. 7. dw as determined by the relation lim lnhxN i . The method converges quickly for mid to high range ✏. However, machine accuracy did not allow for probing N > 55. As a result, the transient oscillatory behavior of the walks was still present for low-✏, leading to inaccurate results for dw. Error bars were calculated using as the error in the y-intercept of our extrapolation on dw over N . determine new domains {X⇤i |X⇤i = (YR — VI. RESULTS OF dw FINDING METHODS ON NON-ULTRA WALKS‌ Fig. 9 shows the results of the proposed methodologies for finding dw in all three ad- dressed ▇▇▇▇▇▇ cases. Recall that dw should tend to one in each of these cases. The limiting moment reaches a stable value almost immedi- ately for both the ▇▇▇▇▇▇ walk and the cyclic ▇▇▇▇▇▇ walk. The hierarchical ▇▇▇▇▇▇ walk does not converge completely to one, which can be attributed to us not probing far enough in time for the lattice to appear e↵ectively con- stant. Also pictured in Fig. 9 is dw as calcu- lated using scaling over a variety of domains. Here we can see just how sensitive the scal- ing algorithm is to domain choice. The algo- rithm still finds values for dw in the neighbor- hood of one, but not in a very distinguishable way. Had we not known what dw to expect

FIG. 2 shows a scatter plot giving the relationship of the observed 1-minute average wind speed to the simultaneously reported gust wind speed. The ratio of the gust wind speed to the 1-minute average is approximately 1.52. This ratio is higher than the standard presented in the US Army Corps of Engineers Shore Protection Manual. The ratio assumed for most locations is 1.242. This indicates that Ketchikan has higher gust wind speeds in relationship to the average wind speeds than is expected at other locations.

FIG. 15 is a partial perspective view of the remote operation of the articulated boom and gripping head of the present invention.

FIG. Monkeys develop an anti-hu5A8 response that is predominantly antiidiotype.

FIG hu5A8 inhibits syncytium formation in HIV-1-infected cells as well as mu5A8. H9 cells chronically infected with HIV-1 were cocultured with uninfected C8166 cells in the presence of varying concentrations of mu5A8 (F), hu5A8 (..), or a control murine immunoglobulin ( ). Syncytia were counted in each well and expressed as percentage inhibition by comparing values with control immunoglobulin-treated wells.

FIG illustrates the overall shape of the subject design; fig.