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In order to fully perceive the physical meaning of such inequalities, it is necessary to reintegrate into them physical constants or scales appropriate for the physical system considered, that is, characteristic length l c and momentum p c : N (Q) N (Q) u 2 l 2 , c N (P ) N (P ) u 2 p 2 c N , (1238)

124. 125. 126. 127.



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where N (Q) and N (Q) are now expressed in unit l c Realistically, in any physical situation N cannot be in nite: there is an obvious limitation on the frequencies or energies accessible to observation/experimentation So it is natural to work with a nite although large value of N, which need not

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Fig 31 This is a java animation developed by L Kocbach from an original applet written by O Psencik It is found at http://webiftuibno/AMOS/MOV/HO/ This interactive toy shows the shape of Glauber (ie standard) coherent states and their time evolution It offers the possibility to select the energy ~ |z|2 : the vacuum z = 0 is shown on





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the top, and an example of CS with intermediate z = 0 is shown in the middle gure The / shape of a perfect Poisson law is easily recognized for these two cases One can see in the third gure (bottom) to what extent a small pertubation of the Poisson distribution destroys the coherent Gaussian shape of CS states

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One notices that this physical quantity can be viewed as the average value of the number operator in the coherent state |z 0 , I0 = z 0 |N |z 0 (lower symbol) At this point it is worth observing, as Schr dinger did, the close relationship between classical and quantum solutions to the oscillator problem To be more concrete, let us reintroduce physical dimensions, namely, mass m and frequency The solution to the Newton equation x + 2 x = 0 is given by x(t) = |A| cos ( t ) with amplitude = |A| = 2I 0 and phase = 0 as initial conditions Let us rewrite this solution as the real part of the complex Ae i t , with A = |A|e i = 2I 0 e i 0 : x(t) = 1 (Ae i t + Ae i t ) 2 (333)

but by 2050 they will be nearly twice as big, as Table 13 shows And the E7 are more than export-reliant economies like the smaller Asian Tigers; they are large countries with growing populations, some with sizeable armies and nuclear weapons, and they should be incorporated into the world s multilateral governing bodies Consider them country by country: China: This 5,000-plus-year-old civilization was the world s largest economy in 1820 and should be again by 20509 With enormous, skilled workforces in both low- and high-tech sectors, China has already surpassed the United States as the leading exporter to Europe, leaving its trade partners to ask, when will its arti cially cheap currency

Let us now go to the quantum side by adopting the time-dependent (Heisenberg) point of view for position and momentum operators Their respective time evolutions Q(t) = e

(334)

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+ 1 m 2 Q 2 , obey 2 (335) (336)

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i Q(t) = [Q(t), H] = P (t)/m , P (t) = m 2 Q(t)

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