Exact(10)
Therefore, there is a bijection between the sets of solutions to the original and transformed systems.
Fig. 2 Phase space and propagated beam paths in the original and transformed systems.
From the transformed systems, a state observer can be constructed in a very easy way.
Figure 2 compares the phase space of the original and the transformed systems given by Fig. 1b.
Figure 2g shows the nearly identical transverse intensities, with a Pearson correlation coefficient [6] of 0.9996, between the original and the transformed systems.
The Wronskian w ˜ i ( X ( a ), X ˆ ( b ) ) for conjoined bases of the transformed systems also depends on the choice of P i , P ˆ i.
Similar(50)
From the inverse transformation of the eigenstates associated to the transformed system, one can evaluate full eigenstates in the original system.
By executing inverse transformation for the wave function obtained in the transformed system, we derived the exact wave function associated to the DSN in the original system.
where is the state vector of transformed system,, and.
Then, we design controllers to stabilize the transformed system.
Next, we analyze the characteristics of the transformed system.
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