ssrs code 39

ssrs code 39

ssrs code 39

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Focus a specimen and adjust for Koehler illumination with both polarizing filters and compensator removed from the optical path Insert the fixed polarizer (depending on the microscope, either the polarizer or analyzer might be fixed ie, glued into position in the holder so that it cannot rotate) If the polarizer is fixed, its transmission axis should be oriented horizontally eastwest as seen looking in the microscope If the polarizer is rotatable, check that the filter is positioned correctly by looking for the mark indicating the orientation of the transmission axis or checking the degrees of rotation on the holder Insert the rotatable analyzer (or polarizer), and rotate it until the two polars are crossed and maximum extinction is obtained Do this by examining a blank region on a specimen slide and making fine adjustments to the analyzer until the image is maximally dark.

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attributes, all of which are equally likely. We imagine a code book that lists all of these choices, one per page, and transmit the number of the page the actual selection of parent attributes is printed on. Note, however, that this term is often omitted based on the following argument: we have to indicate the parent attribute(s) if parents are used, but we also have to indicate if no parents are used, because otherwise the message cannot be decoded. Hence we also have to add this term to the description (rel) length Lprior (C), with k comprising the choice of an empty set of parents. Finally, the reduction of the description length that results from using the attribute A to code the values instead of coding them directly is computed as the difference of the two description lengths derived above. Note that this difference is simply Shannon information gain times N.. plus the difference in the costs of transmitting the value frequencies. If the coding is based on the absolute frequency of the values the reduction of the description length is computed as follows [Kononenko 1995]: Lprior (C)

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Delaunay triangulation (DT) is a well-known and frequently used applied structure in computational geometry [35] It can be constructed in O(n log n) time for a set of n points in the plane One de nition of Delaunay triangulation is as follows: an edge uv belongs to DT if and only if there exists a circle, whose chord is uv, which does not contain any other point from the set in its interior It immediately follows that GG is a subset of DT, since diameter uv (and the disk with diameter uv) is a special case of a chord (and the corresponding circle) Partial Delaunay triangulation (PDT) [16] is a subgraph of DT, and contains GG as its subgraph PDT can be constructed locally More precisely, it is a subset of DT containing edges of DT that can be locally con rmed.

Let Disk(u, v) be the disk with diameter uv Given an edge uv, we consider three cases: (1) if Disk(u, v) contains no other node from the network, then uv [ GG # PDT; (2) if Disk(u, v) contains nodes on both sides of uv, then uv DT and uv PDT; and (3) if Disk(u, v) only contains nodes on one side of uv, let w be one such point that maximizes the angle a /uwv ! p=2 Consider the largest angle b /upv on the other side of uv, where p is a node outside Disk(u, v) If a b .

p, then uv DT (and uv PDT); if a b , p (assume that no four nodes are cocircular), we can add uv into PDT if the following two conditions are both satis ed, which depends on whether one-hop or 2-hop neighbor topology is known to each node (this de nes two structures, PDT1 and PDT2, respectively) PDT de nition is illustrated in Figure 1012..

The transmission axis of the analyzer should now be oriented vertically or north-south The critical adjustment for extinction can only be made while looking in the microscope Extinction indicates that the polars are crossed, but does not guarantee that their azimuths are perfectly oriented east-west and north-south Insert a telescope eyepiece or Bertrand lens and focus on the back aperture of the objective lens A dark polarization cross is observed at extinction (Fig 9-3), with brighter regions of intensity between the horizontal and vertical arms of the cross Commonly, the horizontal and vertical components of the cross are broader in the center of the field and narrower at the periphery This shape is caused by the depolarizing effects of spherical lens surfaces in the condenser and the objective lenses, and is normal for most microscope systems.

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