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of the rst recurrence of that string This takes roughly log Rn + 2 log log Rn bits Now consider the following variant: Instead of describing Rn , the encoder describes Rn 1 plus the last symbol, Xn From these two the decoder can reconstruct the string (X1 , X2 , , Xn ) (a) What is the number of bits per symbol used in this case to encode (X1 , X2 , , Xn ) (b) Modify the proof given in the text to show that this version is also asymptotically optimal: namely, that the expected number of bits per symbol converges to the entropy rate 138 Length of pointers in LZ77 In the version of LZ77 due to Storer and Szymanski [507] described in Section 134.



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1, a short match can be represented by either (F, P , L) ( ag, pointer, length) or by (F, C) ( ag, character) Assume that the window length is W , and assume that the maximum match length is M (a) How many bits are required to represent P To represent L (b) Assume that C, the representation of a character, is 8 bits long If the representation of P plus L is longer than 8 bits, it would be better to represent a single character match as an uncompressed character rather than as a match within the dictionary As a function of W and M, what is the shortest match that one should represent as a match rather than as uncompressed characters (c) Let W = 4096 and M = 256.





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For this text field, there s no need to specify any validation beyond it being a required field. 3. From the Preview states list, choose Required. Change the error message from A value is required to Required. The background color applied to the form field is part of the style for this form field state; you ll learn how to modify it later in this chapter. Now, you can apply the same basic steps to the second text field. 4. Hover your mouse over the companyTxt form field and click the Spry tab when it appears. In the Property inspector, choose Validate on: Blur and make sure the Required option is selected. From the Preview states list, choose Required. Change the error message to Required (Figure 10-22).

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when E s2 suddenly become 10 times smaller, the ordinary learning dynamics makes the i i-th row of W become 10 times larger in order to compensate for this change and keep 2 E yi = 1. Therefore, even when W converges to the true C W , large uctuations emerge from the ine ective movements caused by changes in amplitude of si . This sometimes causes numerical instability. On the other hand, our nonholonomic dynamics is always orthogonal to C W so that such ine ective uctuations are suppressed. This is con rmed by computer simulations a few of which are presented in this chapter. There is a lot of research on nonholonomic dynamics [30]. Classical analytical dynamics uses nonholonomic bases to analyze the spinning gyro (Whittaker, 1940). It was also used in relativity. G. Kron (1952) used the nonholonomic constraints to present a general theory of electro-mechanical dynamics of generators and motors. Nonholonomic properties play a fundamental role in continuum mechanics of distributed dislocations (see, e.g., Amari, 1962). An excellent explanation is found in Brockett (1993), where the controllability of nonlinear dynamical systems is shown by using the related Lie algebra. Recently, robotics researchers have been eager to analyze dynamics with nonholonomic constraints (Suzuki and Nakamura 1995) [30]. Remark D.6 Theorem D.4 shows that the orthogonal natural gradient descent algorithm evolves along a trajectory path which doesn t include redundant (useless) components in the directions of C W . Therefore, it seems likely that the orthogonal algorithm can be more ef cient than other algorithms as has been con rmed by preliminary computer simulations. Stability Analysis In this section, we discuss the local stability of the nonholonomic orthogonal natural gradient descent algorithm de ned by W(k) = (k) F(y(k)) W(k), (D.17)

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