Further we have that the uncertain descriptor fractional-order systems (6) is
normalizable if and only if the nominal descriptor fractional-order system (9) is
normalizable.
This can be argued as follows: in quantum mechanics, if we want to have a
normalizable wave function, we have to impose that R([rho]) vanishes at [rho] [right arrow] 0 and[rho] [right arrow] [infinity].
(ii) All measures affine
normalizable are homographic
normalizable, but the converse is false.
Under such concepts, the observance of WFC due to continuous spectrum operator forms such as position, momentum, and scattering Hamiltonian, is not a feasible outcome due to the fact that the corresponding eigenfunctions are not
normalizable. The expectation is these cases is that the collapse will occur amongst a small set of eigenstates which correspondingly will involve a set of eigenvalues related to the imprecision of the apparatus.
In fact, a careful inspection of this numerical solution shows that for a function f(a) which vanishes at a = 0 and a = [a.sub.0], for instance, f(a) = sin([[pi].sub.a]/[a.sub.0])/[[phi].sub.0], and then the wave function vanishes at the boundaries a = 0 and a = [a.sub.0] and at [phi] = [+ or -][[phi].sub.0] vanishes as [[phi].sub.0] [right arrow] [infinity], pointing to a
normalizable wave function.
This is because it is given the role of a probability for a measurement so must be positive definite and
normalizable. This fails in the classical theory of Dirac particles but is "fixed up" in the quantum field theory by choices for the commutation relations of the operators and their action on the vacuum ground state (as with the Gupta-Bluer formalism [13]).
It is perhaps a response to the "theory of the double solution" that Louis de Broglie was seeking since 1927: "I introduced as the "double solution theory" the idea that it was necessary to distinguish two different solutions that are both linked to the wave equation, one that I called wave u, which was a real physical wave represented by a singularity as it was not
normalizable due to a local anomaly defining the particle, the other one as Schrodingers [PSI] wave, which is a probability representation as it is
normalizable without singularities" 77].
Compared with OMP, ROMP, and BAOMP algorithms, the atom selection process will be more traceable,
normalizable, and structural.
No es tampoco una sociedad en la que se exija el mecanismo de la normalizacion general y la exclusion de lo no
normalizable.