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These simple options can be modi ed if the seller and buyer agree. Typical modi cations include: Fixed option: The price of the asset named in the option remains the same for the life of the option. Thus, if the price is $500,000, this price stays the same from day 1 to the final day of the option. Laddered option: When an option has a long term say six months or more a laddered option may be used. With this type of option the price of the asset will rise at stated intervals say every three months. Thus, with an 18-month option and a $500,000 sales price, the price might rise 10 percent every 6 months. So at the end of the first 6 months, the price of the asset would become $550,000; at the end of 12 months, $605,000. Credit-back option: With this type of option the full amount you paid for the option is credited to your purchase price when you exercise the option that is, buy the asset. Thus, if you paid $5,000 for the option to buy the asset at $500,000, your payment at closing would be $500,000 $5,000 $495,000. Reduced-credit option: With this type of option, the amount you re credited back declines as the life of the option

Figure 8.3 (Continued opposite)

class MyClass implements MyInterface1, MyInterface2 {

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The Solarize effect creates a positive and negative version of your image and then blends them together to create the solarizing effect. This can produce a lightened version of your image with darkened edges. In the Solarize Settings dialog box, shown in Figure 11-39, click and drag the Threshold slider to control the brightness level at which the Solarizing effect begins.

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an air-substrate thickness of about 5% of the wavelength of the center operating frequency When the patch s aspect ratio and desired operating frequency are xed, this lowering in resonant frequency corresponds to an antenna size reduction of about 54% Since the lengthening of the effective patch s surface current paths is due to the additional downward paths in the added rims, which is different from that of the meandered designs [1, 6], a relatively very small perturbation on the excited surface current distribution in the radiating patch is expected This implies that it is possible for the radiation characteristics of this compact design to be as good as those of a corresponding conventional patch antenna with a planar radiating patch Prototypes of this compact design have been successfully implemented [12] The planar or top portion of the inverted U-shaped radiating patch is square and has a side length L.

w = wi-1 pu; [ ycsgn(z(i)) i z(2) = uiwi-1

The two downward rims are identical and are added at the two radiating edges of the top patch The downward rims have a length of u, which is smaller than the air-substrate thickness h Centered below the inverted U-shaped patch is an H-shaped coupling slot cut in the ground plane of a microwave substrate of thickness 08 mm and relative permittivity 44 On the other side of the ground plane, a 50microstrip feed line for feeding the inverted U-shaped patch through the H-shaped coupling slot is printed The H-shaped coupling slot has a central arm of dimensions 1 mm S and two side arms of dimensions 1 mm 2Sh Compared to a conventional narrow rectangular coupling slot, the use of an H-shaped coupling slot can reduce the antenna s backward radiation.

For the proposed design with various rim lengths, good impedance matching can be obtained by selecting proper values of S, Sh , and the tuning-stub length t of the 50- microstrip feed line Figure 225 shows the measured return loss for constructed prototypes (antennas 1 3) and a reference antenna (a design without downward rims) The top square patch had a side length of 46 mm, and the air-substrate thickness was chosen to be.

The subject of this section is maximum likelihood estimation of parameters of expectation models from independent Poisson distributed observations. Suppose that w = (w1 . . W N ) is the vector of observations and 8 = (0, . . . . ~ the vector of unknown parameters. Then, the log-probability function of the observations is defined by (3.43):

(21)

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