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Alright, Jim says What about conflicts of interest It seems to me that the really egregious internal control problems occur when someone is afraid to rat out the boss In my experience, few people ever volunteered to tell the internal audit team that their division manager is messing around with the controls Of course, Linda says You could have a problem like that, and our system is not totally bulletproof against collusion or abuses of power However, I do believe that the more process that we can instill as well as good tone at the top control direction the more we will get out ahead of upper-level control malfeasance On a practical level, too, we are demonstrating a firm commitment to internal control, so we will avoid the appearance of being lax about controls if a matter comes under scrutiny from the auditor or the SEC.

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the amplitude distribution in each delay bin differs from the Rayleigh fading distribution. In order to evaluate the small-scale amplitude fading statistics, the relative amplitudes over small-scale areas are calculated. Empirical data from bins at speci c excess delays were matched to some typical theoretical distributions for amplitude fading statistics such as log-normal, Nakagami, Rayleigh, Rice, and Weibull distributions. The measurement results reported in [31, 50] show that the small-scale amplitude fading can be modeled by a log-normal distribution, while measurement results reported in [43, 51] show that Rayleigh distribution gives a better t. In [39], the Rice distribution is reported to give the best t for the amplitude fading statistics. Other measurement campaigns such as [44, 52] have found that the Nakagami distribution can be a good t for small-scale amplitude fading statistics. The advantage of Nakagami distribution is that, for special cases such as m 1 and for very large values of m, it can be generalized to become the Rayleigh and log-normal distributions, respectively. Furthermore, a conversion from the Nakagami distribution to the Rice distribution is also possible and can be approximately expressed as follows [40, 41]: m and p m2 m p Kr m m2 m (8:14) (Kr 1)2 (2Kr 1) (8:13)

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Their analysis shows that reducing contributes to stabilization by enlarging the basin of attraction of high-gain modes, and by increasing their stability by making them more distant from unstable modes Although is often treated as a fixed parameter, it has a strong spectral dependence Thus, by using an etalon to tune the feedback away from the gain maximum of the semiconductor medium, can be varied; decreasing corresponds to decreasing Two experiments were conducted A Hitachi HLP1400 bulk Fabry Perot diode was placed in a cavity with round-trip delay of c = 3 3 ns An intracavity etalon was used to pull the wavelength up to 10 nm from the solitary laser wavelength, which in turn shifted from 2 8 0 5 down to 1 6 0 3.

Also, Sebastian says, We re laying out a process in theoretical steps Our plan is to implement the compliance portal and project compliance teams with enough built-in flexibility to adapt to reality as we go through our shakedown period DexCo s actual business is going to throw us some curve balls, of that we are quite sure Our goal is to build our agile compliance process in a way that moves with the company..

vulnerable_function: var_50 arg_44 save st = -0x50 = 0x44 %sp, -0xb0, %sp %i0, [%fp+arg_44]

This had the effect of increasing the region over which complex dynamics coexisted with stable emission on a high-gain mode (see, for example, Figure 431 The region of parameter space in which this coexistence grew significantly indicated that the system is able to access the high-gain mode where it was unable to do so previously Furthermore, lowering also resulted in increasing the average time duration over which stable emission was observed However, complete stabilization was not attained in this system, even at its minimum attainable To investigate lower s, an Alcatel MQW-DFB laser with nominal = 1 55 m and a low value of = 0 95 0 2 was placed in an external cavity with c = 4 0 n sec With this laser, stable emission was observed for the entire parameter regime of the first experiment, with instabilities only appearing at very high pumping levels.

k,l W N sl (n)

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