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A fresh-out-of-the-box router typically has many of its security features disabled. If you recently installed a new router or just never got around to tweaking your older one, you can substantially raise your protection with a few simple steps.

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Optical ber consists of a core and a cladding, as illustrated in Figure 9.23. At present the most ef cient core material is silica (SiO2 ). The cladding is a dielectric material that surrounds the core of an optical ber. The practical propagation of light through an optical ber may best be explained using ray theory and Snell s law. Simply stated, we can say that when light passes from a medium of higher refractive index (n1 ) into a medium of lower refractive index (n2 ), the refractive ray is bent away from the normal. For instance, a ray traveling in water and passing into an air region is bent away from the normal to the interface between the two regions. As the angle of incidence becomes more oblique, the refracted ray is bent more until nally the refracted energy emerges at an angle of 90 with respect to the normal and just grazes the surface. Figure 9.24 shows various incident angles of light entering a ber. Figure 9.24b illustrates what is called the critical angle, where the refracted ray just grazes the surface. Figure 9.24c is an example of total internal re ection. This occurs when the angle of incidence exceeds the critical angle. A glass ber, for the effective transmission of light, requires total internal re ection.

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pro le within the SiGe alloy lm during post-epitaxial processing. The challenge comes in achieving a low sheet resistance by increasing doping concentration and at the same time limiting the boron diffusion process from thermal processes and transient enhanced diffusion (TED) processes [46 52]. In a pseudomorphic Si1 xGex lm, the lm is compressed in the growth plane and expanded in the growth direction, causing the boron atom diffusion to be nonrandom. Boron will diffuse easier in the direction parallel to the silicon surface and diffuse slower in the lm growth direction. The diffusion of boron in the Si1 xGex HBT alloy lm can be explained in a simple diffusion model that includes the modi ed strain, the effect of trapping between B and Ge, the drift eld due to the bandgap narrowing, and the spatially dependent intrinsic carrier concentration. The universal diffusion equation for a generic impurity present in a structure is qCB r JB qt where CB is the boron concentration and JB is the boron impurity ux given by JB DB j Q j qCB CB qNT 2CB nq ln ni qx Q qx Q qx

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// Read a covert char and put in overt2 file, // until covert file exhausted (normal ending) // or overt file exhausted (error) done = FALSE; while(done == FALSE) { read_cnt = fread( &ch, sizeof(char), 1, covertStream ); if(read_cnt > 0) { write_cnt = fwrite( &ch, sizeof(char), 1, overt2Stream ); if(write_cnt < 1) { printf( Error, overt2 file too small\n ); exit(0); } //if // Move the pointer into the overt file // forward one character, so that exe s // have the same size. read_cnt = fread( &ch, sizeof(char), 1, overtStream ); } else { done = TRUE; } //if } //while // Write remaining overt file to overt2... copyRemainingOvert(); return SUCCESS; } //exe_stuffer_encode();

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