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In fact the problem has two optimal solutions, which incur minimum total cost (10) The two optimal solutions are indicated by the thick paths and are shown in Table 165 Because this instance of the shunting problem is very limited, it is still manageable with DP We comment later on real instances after brie y illustrating the forward DP approach 16323 Forward Dynamic Programming Without formulating the forward recursion explicitly, we illustrate by Figure 1614 the solution procedure of the forward DP approach applied to Example 2 Again we identify two optimal solutions to the shunting problem, shown by the thick paths from starting state to nal state Note that the forward approach generates many more states at stage 1 than the backward approach does At the next stage (stage 2), most of these states.



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As stated above, the s orbital of a C H bond is unlikely to be the LUMO of H A However, if the s orbital of a C H bond is not too high in energy, the probability of reaction may still be relatively high due to the exposed nature of the hydrogen, the polarization toward H, and the lack of nodes The rst factor makes close approach possible; the other two factors allow large orbital overlap from a wide range of angles of approach The energy of the sCH may be lowered by two distinct mechanisms A change in the hybridization of the C sp n orbital toward smaller n, that is, more s character, is accompanied by a lowering of the energy (or increase of electronegativity) of the hybrid orbital The orbital interaction analysis, shown in Figure 10.





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4, predicts two consequences, a lowering of the s orbital and increased polarization of the s orbital toward H Both.

is, the beam is in an equilibrium situation where the distribution is indistinguishable from turn to turn. Since trajectories in x - ( a x + px ) phase space are circles, as can be seen by examining Equations 3.88 and 3.89, then in this equilibrium situation the distribution in the coordinate a x + px will also be Gaussian with standard deviation u.For, after all, the population on a given circle just rotates through an angle corresponding to the phase advance from turn to turn, and so the equilibrium distribution is independant of position along a circle, and depends only on the radius of the circle. The two-dimensional phase space distribution in these coordinates will be

(6.47)

of the maximum likelihood estimator of the parameters of linear models from normally distributed observations (5.93) with

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averaged value and lower than the beam quality for one shot due to the nite pointing stability of the beam To demonstrate the ability of phase conjugating mirrors to compensate phase distortions, the beam quality was measured at different locations inside the laser system and for different operating parameters (Fig 439) 2 The oscillator beam has a near-diffraction-limited beam quality (Mx 1:1 and 2 2 My 1:2) that is already reduced in front of the rst ampli er (Mx 1:6 and 2 My 1:3) This is due to phase distortions introduced by the telescope and the nonperfect polished entrance window of the polarizer After single-pass ampli cation the beam quality decreases rapidly due to phase distortions introduced by both pumped ampli er rods At low average pumping power of 3.

54 56

2 kW for each 2 2 ampli er the diffraction-limited factors are Mx 3:2 and My 2:3; these values 2 2 increase up to Mx 5:2 and My 4:5 at maximum average pumping power (65 kW for each ampli er) After double-pass ampli cation the beam quality can be nearly reproduced at the 2 2 polarizer (Mx 1:7 1:8 and My 1:4 1:9) due to the phase conjugating SBS mirror Differences between the initial and nal beam quality are caused by nonperfect compensation of phase distortions and amplitude distortions, like gain saturation and apertures After single-pass booster ampli cation by ampli er 3 and ampli er 6, the beam suffers again from phase distortions that are not yet compensated by a PCM 2 (My 1:8 5:2) The beam quality was measured only for one direction until now.

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