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Hence, it will undergo motion with the classical period, modulated by the revival phase [126] Since T cl < t rev for large n, the classical period dominates for small < values of t (mod t rev ), and the motion is then periodic with period T cl As t increases from zero and becomes nonnegligible with respect to t rev , the revival term (n t n )2 t rev in the phase of (9113) causes the wave packet to spread and collapse The latter gathers into a series of subsidiary waves, the fractional revivals, which move periodically with a period equal to a rational fraction of T cl Then, a full revival obviously occurs at each multiple of t rev To put into evidence these revival structures for a given wave packet (x, t) = x| (t) , an ef cient method is to calculate its autocorrelation function [126]: A(t) = (x, 0) | (x, t) =



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share includes intermediate goods that are processed in different places and only assembled in a nal country The modern production chain of automobile manufacturing is a perfect example: The Mini Cooper, a small, fashionable, distinctly British car is actually produced and owned by the German manufacturer BMW BMW imports engines from Brazil and other parts (brakes, glass, tires) from up to a dozen countries depending on market costs In the end, only nal assembly happens in the United Kingdom Barring a prolonged worldwide depression (a possibility given the current global nancial crisis), the globalization of labor and manufacturing should continue for decades, and EMs are driving economic expansion The G7 has a combined labor force of less than 500 million people, while the 15 leading emerging markets have 25 billion people as of 20076 By 2050, the G7 labor force will be smaller than it is today In contrast to the aging, shrinking populations of Germany, Japan, and Italy, emerging markets will add an additional 375 million skilled workers in the same period7 Let us not forget what Henry Ford knew more than 100 years ago: Today s well-paid workers are tomorrow s new customers Figure 23 shows just how fast EM consumption is growing With rising disposable incomes, two or three billion emerging market workers are





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If and to the extent that a Party s performance of any of its nonmonetary obligations pursuant to this Master Agreement or the Local Service Contract is prevented, hindered, or delayed by fire, flood, earthquake, elements of nature or acts of God, acts of war, terrorism, riots, civil disorders, rebellions, revolutions, strikes, labor disputes, compliance with laws, any acts by a third party, any third-party products or services, or any other cause beyond the reasonable control of such Party, including failures or fluctuations in electrical power, heat, light, air conditioning or telecommunications equipment (each, a Force Majeure Event ), then the nonperforming, hindered, or delayed Party shall be excused for such nonperformance, hindrance, or delay, as applicable, of those obligations (except for monetary payment obligations) affected by the Force Majeure Event for as long as such Force Majeure Event continues and such Party

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Numerically, |A(t)|2 varies between 0 and 1 The maximum |A(t)|2 = 1 is reached when (x, t) exactly matches the initial wave packet (x, 0), and the minimum 0 corresponds to nonoverlapping: (x, t) is far from the initial state On the other hand, fractional revivals and fractional superrevivals appear (in the general case) as periodic peaks in |A(t)|2 with periods that are rational fractions of the classical round-trip time T cl and the revival time t rev

Since the weighting distribution |c n |2 is crucial for understanding the temporal behavior of the wave packet (9106), it is worthwhile also giving some general precisions of a statistical nature [129 133] before examining the special case of our coherent states It is clear that the revival features will be more or less apparent, de pending on the value of the deviation (n n ) (relative to n) that is effectively taken into account in the construction of the wave packet In this respect, it is interesting to compare |c n |2 with the Poissonian case n n e n /n! and with the Gaussian case, (2 ( n)2 ) 1/2 exp[ (n n )2 /2( n)2 ] A quantitative estimate is given by the so-called Mandel parameter Q [129, 131, 132] de ned as follows: QM =

5 4 3 2 1 0

(9114)

Figure 2-1

where the average is calculated with respect to the discrete probability distribution n |c n |2 In the Poissonian case, we have Q M = 0, that is, n = n 1/2 We say that the weighting distribution is sub-Poissonian (or super-Poissonian) if Q M < 0 (or Q M > 0) In the super-Poissonian case, that is, n > n 1/2 , the set of states |e n that contribute signi cantly to the wave packet can be rather widely spread around n n , and this may have important consequences for the properties of localization and temporal stability of the wave packet

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