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Given the symmetry and the real-valuedness of states (1536), the mean value of the commutator when is one of our coherent states vanishes, even if the operator does not This result is due to the symmetry of the commutator spectrum with respect to 0 As is shown on right in Figures 151 and 152, the eigenvalues of the commutator tend to i as , or equivalently , increases Still, there are some points with modulus less than This leads to dispersions Q P in coherent states |x that are no longer bounded from below by /2 Actually, the lower bound of this product, for a region in the phase space as large as we wish, decreases as diminishes A numerical approximation is shown in Figure 153



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2,121 2,753 5,684 1,595 3,572 1,267





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From the mean values of the operators obtained here, we verify that the coherent state quantization gives well-behaved momentum and position operators The classical limit is reached once the appropriate limit for the parameter is found If we consider the behavior of the observables as a function of the dimensionless quantity = L/ , in the limit 0 and when the Gaussian functions for the momentum become very narrow, the lower symbol of the position operator is Q(q, p) ~ L/2 This corresponds to the classical average value position in the well On the other hand, at the limit , for which the Gaussians involved spread to constant functions, the function Q(q, p) converges numerically to the function q In other words, the position operator obtained through this coherent state quantization yields a fair quantitative description for the quantum localization within the well Clearly, if a classical behavior is sought, the values of have to be chosen near 0 This gives localized values for the observables Consistent with these observations, the behavior of the product Q P for low values of shows uncorrelated observables at any point in the phase space, whereas for large values of this parameter the product is constant and almost equal to the canonical quantum lowest limit /2 This is shown in Figure 153 It is interesting to note that if we replace the Gaussian distribution, used here for the p variable in the construction of the coherent states, by any positive even probability distribution R p ( p) such that n ( p n) < the results are

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Lc = 1, L*= 2 Lc = 2, L* = 4 Lc = 3, L* = 7 Lc = 4, L*= 9

m (x) n (x) dx ,

(26) (27)

From the Method-Ready state the bean can either transfer to the Does Not Exist state or to the Passivated state. The bean can enter the Does Not Exist state under the following conditions: The client application calls the remove method on the client interface (it translates to the ejbRemove() invocation on the bean instance). OR The container decides to remove the bean either to preserve resources or because the bean instance has timed out. When no client activity exists for the particular bean instance, it becomes eligible for passivation. Passivation is the process by which the application server removes the bean from memory while preserving the EJB s state on disk.

1,741,620 391,980 3,208,265 10,460,030 17,937,070 1,972,215

c n n ,

Note that the characteristic length is the standard deviation of the position in the ground state, n = 0, l c =

In momentum representation, it is the turn of operator P to be realized as a multiplication operator on H = L2 (R): P ( p, t) = p ( p, t) , Q ( p, t) = i ( p, t) p (28)

d =0

The function ( p, t) (or ( p)), its pure momentum part in the stationary case, is the Fourier transform of (x, t) at xed time t (or (x)): 1 2 1 (x, t) = 2 ( p, t) =

1,957 2,667 5,887 1,863 3,707 1,661

+

(x, t) dx ,

10 1 Average Bit Error Rate Pb(E )

(29) (210)

United States 1,631,825

Energy eigenstates n ( p) in the momentum representation are similar to their Fourier counterpart n (x): n ( p) =

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