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been expanded and applied to a variety of both heavy and light hadronic data in recent years. The most extensive work is probably that based on the papers of Isgur and Karl (1979a,b) and references therein. In these systematic calculations one observes a fundamental continuity between the properties of the heavy quark and light quark systems. For example, in Fig. 12.21 the smooth evolution of the IS0 and 3 P levels relative to the 3 S ~ ~ level is shown for a range of qq systems. Therefore, even though a nonrelativistic calculation is formally suspect it is argued that the continuity of basic features as the quark flavors (and hence masses) are varied justifies the potential model as a useful phenomenological device, with the formal shortcomings of the model absorbed into a smooth modification of parameters. The potential could be any confining form (linear, log, power law, ...), but in many practical applications a harmonic oscillator potential yields spectra not very different from those found for potentials such as Coulomb linear that QCD prejudice would favor. For example, Fig. 12.22 shows the difference between a linear, linear Coulomb, and harmonic potential in describing cC states. Since harmonic oscillator models have nice mathematical properties, that form has often been employed for the confining potential. Isgur and Karl (1978, 1979a,b) have used such two-body confining potentials, keeping only the spin-spin and tensor components of the Fermi-Breit interaction (12.98) between quarks i and j ,

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2.1 Shannon s Classi cation of Secrecy Transformations 2.2 The Rules of Columnar Transposition Encipherment 2.3 Cribbing 2.4 Examples of Cribbing 2.5 Plaintext Language Models 2.6 Counting k-Grams 2.7 Deriving the Parameters of a Markov Model from Sliding Window Counts 2.8 Markov Scoring 2.9 The ADFGVX Transposition System 2.10 CODA 2.11 Columnar Transposition Problems

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